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Physics PYQs · MHT CET · JEE Main · NEET

Work, Energy and Power

Questions
263
MHT CET
35
JEE Main
156
NEET
72
Years
1989–2026
0 of 263 attemptedPick an answer to see the solution

Q1MHT CET 2026 · 13 MAY · SHIFT 1Easy

Work by a Constant Force · Work as a dot product: W = F·s

A particle moves from position 3i^+2j^−6k^3\hat{i} + 2\hat{j} - 6\hat{k} to 14i^+13j^+9k^14\hat{i} + 13\hat{j} + 9\hat{k} due to uniform force of (4i^+j^+3k^)(4\hat{i} + \hat{j} + 3\hat{k}) N. If displacement is in metre then work done will be

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Answer: (a)

  1. Work by a constant force: W=F⃗⋅s⃗W = \vec{F}\cdot\vec{s}.
  2. s⃗=(14−3)i^+(13−2)j^+(9+6)k^=11i^+11j^+15k^\vec{s} = (14-3)\hat{i} + (13-2)\hat{j} + (9+6)\hat{k} = 11\hat{i} + 11\hat{j} + 15\hat{k} m
  3. W=4(11)+1(11)+3(15)=44+11+45=100W = 4(11) + 1(11) + 3(15) = 44 + 11 + 45 = 100 J
  4. So the answer is (a) 100100 J.
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Q2JEE Main 2026 · 4 APR · SHIFT 1Easy

Work by a Constant Force · Work as a dot product: W = F·s

A 1 kg block subjected to two simultaneous forces (2i^+3j^+4k^) N(2\hat{i} + 3\hat{j} + 4\hat{k})\text{ N} and (3i^−j^−2k^) N(3\hat{i} - \hat{j} - 2\hat{k})\text{ N} is moved a distance of 25 m along (3i^−4j^)(3\hat{i} - 4\hat{j}) direction. The work done in this process is ______ J.

Numerical answer type. Work it out, then open the answer.

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Answer: 35

  1. Net force F⃗=(2+3)i^+(3−1)j^+(4−2)k^=5i^+2j^+2k^\vec{F} = (2+3)\hat{i} + (3-1)\hat{j} + (4-2)\hat{k} = 5\hat{i} + 2\hat{j} + 2\hat{k} N
  2. Unit vector along 3i^−4j^3\hat{i} - 4\hat{j} is 3i^−4j^5\frac{3\hat{i} - 4\hat{j}}{5}, so s⃗=25⋅3i^−4j^5=15i^−20j^\vec{s} = 25 \cdot \frac{3\hat{i} - 4\hat{j}}{5} = 15\hat{i} - 20\hat{j} m
  3. W=5(15)+2(−20)+2(0)=75−40=35W = 5(15) + 2(-20) + 2(0) = 75 - 40 = 35 J
  4. Work done =35= 35 J.
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Q3JEE Main 2026 · 5 APR · SHIFT 2Medium

Work by a Constant Force · Work against friction

A mass of 1 kg is kept on an inclined plane with 30∘30^\circ inclination with respect to horizontal plane and it is at rest initially. Then the whole assembly is moved up with constant velocity of 4 m/s4\text{ m/s}. The work done by the frictional force in time 2 s is ______ J. (Take g=10 m/s2g = 10\text{ m/s}^2)

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Answer: (a)

f = 5 Nv = 4 m/ss = 8 m30°f vertical = f sin30° = 2.5 N
  1. Block stays at rest on the incline, so static friction balances mgsin⁡30∘mg\sin 30^\circ: f=1×10×12=5f = 1 \times 10 \times \frac{1}{2} = 5 N, directed up the incline.
  2. The assembly moves vertically up by s=vt=4×2=8s = vt = 4 \times 2 = 8 m.
  3. Friction makes angle 60∘60^\circ with the vertical, so its vertical component is fsin⁡30∘=2.5f\sin 30^\circ = 2.5 N.
  4. Wf=2.5×8=20W_f = 2.5 \times 8 = 20 J
  5. So the answer is (a) 20.
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Q4MHT CET 2025 · 23 APR · SHIFT 2Easy

Work by a Constant Force · Work as a dot product: W = F·s

A particle is displaced from point P(3 m,4 m,5 m)P(3\text{ m}, 4\text{ m}, 5\text{ m}) to a point Q(2 m,3 m,4 m)Q(2\text{ m}, 3\text{ m}, 4\text{ m}) under a constant force F⃗=(3i^+4j^+5k^) N\vec{F} = (3\hat{i} + 4\hat{j} + 5\hat{k})\text{ N}. The work done by the force in this process is

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Answer: (d)

  1. W=F⃗⋅s⃗W = \vec{F}\cdot\vec{s} with s⃗=r⃗Q−r⃗P\vec{s} = \vec{r}_Q - \vec{r}_P.
  2. s⃗=(2−3)i^+(3−4)j^+(4−5)k^=−i^−j^−k^\vec{s} = (2-3)\hat{i} + (3-4)\hat{j} + (4-5)\hat{k} = -\hat{i} - \hat{j} - \hat{k} m
  3. W=3(−1)+4(−1)+5(−1)=−12W = 3(-1) + 4(-1) + 5(-1) = -12 J
  4. So the answer is (d) −12-12 J.
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Q5JEE Main 2025 · 22 JAN · SHIFT 2Easy

Work by a Constant Force · Work as a dot product: W = F·s

A force F⃗=2i^+bj^+k^\vec{F} = 2\hat{i} + b\hat{j} + \hat{k} is applied on a particle and it undergoes a displacement i^−2j^−k^\hat{i} - 2\hat{j} - \hat{k}. What will be the value of bb, if work done on the particle is zero.

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Answer: (b)

  1. Zero work means F⃗⋅s⃗=0\vec{F}\cdot\vec{s} = 0.
  2. 2(1)+b(−2)+1(−1)=0⇒1−2b=02(1) + b(-2) + 1(-1) = 0 \Rightarrow 1 - 2b = 0
  3. So the answer is (b) b=12b = \frac{1}{2}.
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Q6JEE Main 2025 · 4 APR · SHIFT 2Medium

Work by a Constant Force · Work against friction

A block of mass 25 kg is pulled along a horizontal surface by a force at an angle 45∘45^\circ with the horizontal. The friction coefficient between the block and the surface is 0.25. The block travels at a uniform velocity. The work done by the applied force during a displacement of 5 m of the block is:

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Answer: (d)

  1. Uniform velocity: Fcos⁡45∘=μNF\cos 45^\circ = \mu N with N=mg−Fsin⁡45∘N = mg - F\sin 45^\circ.
  2. F2(1+μ)=μmg⇒F2=0.25×25×9.81.25=49\frac{F}{\sqrt{2}}(1 + \mu) = \mu mg \Rightarrow \frac{F}{\sqrt{2}} = \frac{0.25 \times 25 \times 9.8}{1.25} = 49 N
  3. W=Fcos⁡45∘×s=49×5=245W = F\cos 45^\circ \times s = 49 \times 5 = 245 J
  4. So the answer is (d) 245 J (with g=9.8 m/s2g = 9.8\text{ m/s}^2).
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Q7JEE Main 2024 · 9 APR · SHIFT 2Easy

Work by a Constant Force · Work as a dot product: W = F·s

A force (3x2+2x−5) N(3x^2 + 2x - 5)\text{ N} displaces a body from x=2 mx = 2\text{ m} to x=4 mx = 4\text{ m}. Work done by this force is ________ J.

Numerical answer type. Work it out, then open the answer.

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Answer: 58

  1. Variable force: W=∫24(3x2+2x−5) dx=[x3+x2−5x]24W = \int_{2}^{4} (3x^2 + 2x - 5)\,dx = \left[x^3 + x^2 - 5x\right]_2^4
  2. =(64+16−20)−(8+4−10)=60−2= (64 + 16 - 20) - (8 + 4 - 10) = 60 - 2
  3. Work done =58= 58 J.
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Q8JEE Main 2024 · 5 APR · SHIFT 1Easy

Work by a Constant Force · Work against gravity

A body of mass 50 kg50\text{ kg} is lifted to a height of 20 m20\text{ m} from the ground in the two different ways as shown in the figures. The ratio of work done against the gravity in both the respective cases, will be:

Figure

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Answer: (c)

  1. Work against gravity depends only on the vertical rise: W=mghW = mgh (gravity is conservative).
  2. Both cases: W=50×g×20W = 50 \times g \times 20, same value.
  3. So the answer is (c) 1:11 : 1.
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Q9JEE Main 2024 · 29 JAN · SHIFT 1Easy

Work by a Constant Force · Work against friction

A block of mass 100 kg100\text{ kg} slides over a distance of 10 m10\text{ m} on a horizontal surface. If the co-efficient of friction between the surfaces is 0.4, then the work done against friction (in J(\text{in } J) is:

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Answer: (d)

  1. Friction f=μmg=0.4×100×10=400f = \mu mg = 0.4 \times 100 \times 10 = 400 N
  2. Work against friction W=fd=400×10=4000W = f d = 400 \times 10 = 4000 J
  3. So the answer is (d) 4000 (taking g=10 m/s2g = 10\text{ m/s}^2).
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Q10JEE Main 2024 · 30 JAN · SHIFT 2Medium

Work by a Constant Force · Work against friction

A block of mass 1 kg1\text{ kg} is pushed up a surface inclined to horizontal at an angle of 60∘60^\circ by a force of 10 N10\text{ N} parallel to the inclined surface as shown in figure. When the block is pushed up by 10 m10\text{ m} along inclined surface, the work done against frictional force is:

[g=10 m/s2]\left[g = 10\text{ m/s}^2\right]

Figure

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Answer: (b)

  1. Normal reaction N=mgcos⁡60∘=1×10×12=5N = mg\cos 60^\circ = 1 \times 10 \times \frac{1}{2} = 5 N
  2. Friction f=μN=0.1×5=0.5f = \mu N = 0.1 \times 5 = 0.5 N
  3. Work against friction =fs=0.5×10=5= f s = 0.5 \times 10 = 5 J
  4. So the answer is (b) 5 J.
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Q11JEE Main 2023 · 1 FEB · SHIFT 1Easy

Work by a Constant Force · Work as a dot product: W = F·s

A small particle moves to position 5i^−2j^+k^5\hat{i} - 2\hat{j} + \hat{k} from its initial position 2i^+3j^−4k^2\hat{i} + 3\hat{j} - 4\hat{k} under the action of force 5i^+2j^+7k^ N5\hat{i} + 2\hat{j} + 7\hat{k}\text{ N}. The value of work done will be __________ J.

Numerical answer type. Work it out, then open the answer.

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Answer: 40

  1. s⃗=(5−2)i^+(−2−3)j^+(1+4)k^=3i^−5j^+5k^\vec{s} = (5-2)\hat{i} + (-2-3)\hat{j} + (1+4)\hat{k} = 3\hat{i} - 5\hat{j} + 5\hat{k} m
  2. W=F⃗⋅s⃗=5(3)+2(−5)+7(5)=15−10+35W = \vec{F}\cdot\vec{s} = 5(3) + 2(-5) + 7(5) = 15 - 10 + 35
  3. Work done =40= 40 J.
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Q12JEE Main 2023 · 29 JAN · SHIFT 2Easy

Work by a Constant Force · Positive, negative & zero work

Identify the correct statements from the following:

A. Work done by a man in lifting a bucket out of a well by means of a rope tied to the bucket is negative.

B. Work done by gravitational force in lifting a bucket out of a well by a rope tied to the bucket is negative.

C. Work done by friction on a body sliding down an inclined plane is positive.

D. Work done by an applied force on a body moving on a rough horizontal plane with uniform velocity is zero.

E. Work done by the air resistance on an oscillating pendulum is negative.

Choose the correct answer from the options given below:

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Answer: (d)

  1. A: the man pulls up and the bucket moves up, so his work is positive. False.
  2. B: gravity acts down, bucket moves up, so its work is negative. True.
  3. C: friction opposes the sliding, so its work is negative. False.
  4. D: applied force is along the motion (balancing friction), so its work is positive. False.
  5. E: air resistance always opposes the motion, so its work is negative. True.
  6. So the answer is (d) B and E only.
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Q13JEE Main 2023 · 12 APR · SHIFT 1Medium

Work by a Constant Force · Work against friction

To maintain a speed of 80 km/h by a bus of mass 500 kg on a plane rough road for 4 km distance, the work done by the engine of the bus will be ____________ kJ. [The coefficient of friction between tyre of bus and road is 0.04.]

Numerical answer type. Work it out, then open the answer.

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Answer: 784

  1. Constant speed, so engine force = friction =μmg=0.04×500×9.8=196= \mu mg = 0.04 \times 500 \times 9.8 = 196 N
  2. W=Fd=196×4000=784000W = F d = 196 \times 4000 = 784000 J
  3. Work done by the engine =784= 784 kJ.
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Q14JEE Main 2021 · 27 AUG · SHIFT 1Easy

Work by a Constant Force · Work at an angle: W = Fs cosθ

Two persons A and B perform same amount of work in moving a body through a certain distance d with application of forces acting at angle 45∘{}^\circ and 60∘{}^\circ with the direction of displacement respectively. The ratio of force applied by person A to the force applied by person B is 1x\frac{1}{\sqrt{x}}. The value of x is .....................

Numerical answer type. Work it out, then open the answer.

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Answer: 2

  1. Same work over the same dd: FAdcos⁡45∘=FBdcos⁡60∘F_A d\cos 45^\circ = F_B d\cos 60^\circ
  2. FAFB=cos⁡60∘cos⁡45∘=1/21/2=12\frac{F_A}{F_B} = \frac{\cos 60^\circ}{\cos 45^\circ} = \frac{1/2}{1/\sqrt{2}} = \frac{1}{\sqrt{2}}
  3. Comparing with 1x\frac{1}{\sqrt{x}}, x=2x = 2.
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Q15JEE Main 2021 · 22 JUL · SHIFT 2Easy

Work by a Constant Force · Work against gravity

A porter lifts a heavy suitcase of mass 80 kg and at the destination lowers it down by a distance of 80 cm with a constant velocity. Calculate the work done by the porter in lowering the suitcase. (take g = 9.8 ms−2{}^{-2})

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Answer: (c)

  1. Constant velocity, so the porter's upward force F=mgF = mg.
  2. Displacement is downward, so the angle is 180∘180^\circ: W=−mghW = -mgh.
  3. W=−80×9.8×0.8=−627.2W = -80 \times 9.8 \times 0.8 = -627.2 J
  4. So the answer is (c) −627.2-627.2 J.
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Q16MHT CET 2019 · 2 MAY · SHIFT 2Easy

Work by a Constant Force · Work as a dot product: W = F·s

A force (F)=−5i^−7j^+3k^(F) = -5\hat{\mathbf{i}} - 7\hat{\mathbf{j}} + 3\hat{\mathbf{k}} acting on a particle causes a displacement (s)=3i^−2j^+ak^(s) = 3\hat{\mathbf{i}} - 2\hat{\mathbf{j}} + a\hat{\mathbf{k}} in its own direction. If the work done is 14 J, then the value of ' aa ' is

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Answer: (b)

  1. W=F⃗⋅s⃗=(−5)(3)+(−7)(−2)+3aW = \vec{F}\cdot\vec{s} = (-5)(3) + (-7)(-2) + 3a
  2. 14=−15+14+3a⇒3a=1514 = -15 + 14 + 3a \Rightarrow 3a = 15
  3. So the answer is (b) a=5a = 5.
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Q17JEE Main 2019 · 10 JAN · SHIFT 1Medium

Work by a Constant Force · Positive, negative & zero work

A block of mass m is kept on a platform which starts from rest with constant acceleration g/2 upward, as shown in figure. Work done by normal reaction on block in time t is -

Figure

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Answer: (b)

  1. On the block: N−mg=mg2⇒N=3mg2N - mg = m\frac{g}{2} \Rightarrow N = \frac{3mg}{2}
  2. Displacement from rest: s=12⋅g2t2=gt24s = \frac{1}{2}\cdot\frac{g}{2}t^2 = \frac{gt^2}{4} (upward, along NN)
  3. WN=Ns=3mg2⋅gt24=3mg2t28W_N = Ns = \frac{3mg}{2}\cdot\frac{gt^2}{4} = \frac{3mg^2t^2}{8}
  4. So the answer is (b) 3mg2t28\frac{3mg^2t^2}{8}.
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Q18NEET 2016 · PHASE 2Easy

Work by a Constant Force · Work as a dot product: W = F·s

A particle moves from a point (−2i^+5j^)\left(-2\hat{i} + 5\hat{j}\right) to (4j^+3k^)\left(4\hat{j} + 3\hat{k}\right) when a force of (4i^+3j^)\left(4\hat{i} + 3\hat{j}\right) N is applied. How much work has been done by the force?

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Answer: (c)

  1. s⃗=(0+2)i^+(4−5)j^+3k^=2i^−j^+3k^\vec{s} = (0+2)\hat{i} + (4-5)\hat{j} + 3\hat{k} = 2\hat{i} - \hat{j} + 3\hat{k} m
  2. W=F⃗⋅s⃗=4(2)+3(−1)+0(3)=5W = \vec{F}\cdot\vec{s} = 4(2) + 3(-1) + 0(3) = 5 J
  3. So the answer is (c) 5 J.
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Q19NEET 2013Easy

Work by a Constant Force · Work as a dot product: W = F·s

A uniform force of (3i^+j^)\left(3\hat{i} + \hat{j}\right) newton acts on a particle of mass 2 kg. Hence the particle is displaced from position (2i^+k^)\left(2\hat{i} + \hat{k}\right) metre to position (4i^+3j^−k^)\left(4\hat{i} + 3\hat{j} - \hat{k}\right) metre. The work done by the force on the particle is

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Answer: (c)

  1. s⃗=(4−2)i^+3j^+(−1−1)k^=2i^+3j^−2k^\vec{s} = (4-2)\hat{i} + 3\hat{j} + (-1-1)\hat{k} = 2\hat{i} + 3\hat{j} - 2\hat{k} m
  2. W=F⃗⋅s⃗=3(2)+1(3)+0(−2)=9W = \vec{F}\cdot\vec{s} = 3(2) + 1(3) + 0(-2) = 9 J (mass is not needed)
  3. So the answer is (c) 9 J.
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Q20JEE Main 2006 · AIEEEEasy

Work by a Constant Force · Work against gravity

A particle of mass 100 g100\text{ g} is thrown vertically upwards with a speed of 5 m/s5\text{ m/s}. The work done by the force of gravity during the time the particle goes up is

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Answer: (b)

  1. Work-energy theorem: Wg=ΔK=0−12mu2W_g = \Delta K = 0 - \frac{1}{2}mu^2 (speed becomes zero at the top).
  2. Wg=−12(0.1)(5)2=−1.25W_g = -\frac{1}{2}(0.1)(5)^2 = -1.25 J
  3. So the answer is (b) −1.25-1.25 J.
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Q21NEET 2006 · AIPMTMedium

Work by a Constant Force · Work against friction

300 J of work is done in sliding a 2 kg block up an inclined plane of height 10 m. Work done against friction is (Take g = 10 m/s2)

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Answer: (c)

  1. Work done = increase in PE + work against friction.
  2. mgh=2×10×10=200mgh = 2 \times 10 \times 10 = 200 J
  3. Wf=300−200=100W_f = 300 - 200 = 100 J
  4. So the answer is (c) 100 J.
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Q22JEE Main 2004 · AIEEEEasy

Work by a Constant Force · Work as a dot product: W = F·s

A force F⃗=(5i⃗+3j⃗+2k⃗) N\vec{F} = \left(5\vec{i} + 3\vec{j} + 2\vec{k}\right)\text{ N} is applied over a particle which displaces it from its origin to the point r⃗=(2i⃗−j⃗) m\vec{r} = \left(2\vec{i} - \vec{j}\right)\text{ m} The work done on the particle in joules is

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Answer: (b)

  1. s⃗=2i^−j^\vec{s} = 2\hat{i} - \hat{j} m (from the origin).
  2. W=F⃗⋅s⃗=5(2)+3(−1)+2(0)=7W = \vec{F}\cdot\vec{s} = 5(2) + 3(-1) + 2(0) = 7 J
  3. So the answer is (b) +7+7.
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Q23JEE Main 2004 · AIEEEEasy

Work by a Constant Force · Positive, negative & zero work

A particle is acted upon by a force of constant magnitude which is always perpendicular to the velocity of the particle, the motion of the particles takes place in a plane. It follows that

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Answer: (a)

  1. A force always perpendicular to velocity does zero work: P=F⃗⋅v⃗=0P = \vec{F}\cdot\vec{v} = 0.
  2. By the work-energy theorem, KE (and speed) stays constant.
  3. The force changes direction, so acceleration and velocity are not constant and the path is a circle, not a straight line.
  4. So the answer is (a) its kinetic energy is constant.
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Q24NEET 1997 · AIPMTEasy

Work by a Constant Force · Work at an angle: W = Fs cosθ

A body moves a distance of 10 m10\text{ m} along a straight line under the action of a 5 N5\text{ N} force. If the work done is 25 J25\text{ J}, then angle between the force and direction of motion of the body is

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Answer: (a)

  1. W=Fscos⁡θ⇒25=5×10cos⁡θW = Fs\cos\theta \Rightarrow 25 = 5 \times 10 \cos\theta
  2. cos⁡θ=12⇒θ=60∘\cos\theta = \frac{1}{2} \Rightarrow \theta = 60^\circ
  3. So the answer is (a) 60∘60^\circ.
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Q25NEET 1994 · AIPMTEasy

Work by a Constant Force · Positive, negative & zero work

When a body moves with a constant speed along a circle

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Answer: (a)

  1. In uniform circular motion the net (centripetal) force is always perpendicular to the velocity.
  2. W=Fscos⁡90∘=0W = Fs\cos 90^\circ = 0, which agrees with constant speed (no change in KE).
  3. There is centripetal acceleration and the velocity direction changes, so (b), (c), (d) are false.
  4. So the answer is (a) no work is done on it.
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Q26NEET 2026 · RE-NEETMedium

Work by a Variable Force · Force as a function of x: W = ∫F dx

A particle of mass MM moves along a horizontal xx axis from x=0x = 0 to x=Lx = L. The coefficient of kinetic friction varies as a function of xx as μk(x)=μ0−αx\mu_k(x) = \mu_0 - \alpha x, where μ0,α\mu_0, \alpha are constants of appropriate dimensions, so that μk(L)=0\mu_k(L) = 0. The total work done by the frictional force during the motion is nμ0MgLn\mu_0 MgL, where gg is the acceleration due to gravity. The value of nn is:

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Answer: (a)

  1. μk(L)=0⇒α=μ0L\mu_k(L) = 0 \Rightarrow \alpha = \frac{\mu_0}{L}
  2. Wf=−∫0LμkMg dx=−Mg[μ0L−αL22]=−Mg[μ0L−μ0L2]W_f = -\int_0^L \mu_k Mg\,dx = -Mg\left[\mu_0 L - \frac{\alpha L^2}{2}\right] = -Mg\left[\mu_0 L - \frac{\mu_0 L}{2}\right]
  3. Wf=−12μ0MgLW_f = -\frac{1}{2}\mu_0 MgL, magnitude 12μ0MgL\frac{1}{2}\mu_0 MgL
  4. So the answer is (a) n=12n = \frac{1}{2}.
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Q27JEE Main 2025 · 24 JAN · SHIFT 1Medium

Work by a Variable Force · Force as a function of x: W = ∫F dx

A force F=α+βx2F = \alpha + \beta x^2 acts on an object in the x -direction. The work done by the force is 5 J when the object is displaced by 1 m. If the constant α=1 N\alpha = 1\text{ N} then β\beta will be

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Answer: (c)

  1. Taking the displacement from x=0x = 0 to x=1x = 1 m: W=∫01(α+βx2) dx=α+β3W = \int_0^1 (\alpha + \beta x^2)\,dx = \alpha + \frac{\beta}{3}
  2. 5=1+β3⇒β=125 = 1 + \frac{\beta}{3} \Rightarrow \beta = 12
  3. So the answer is (c) 12 N/m212\text{ N/m}^2.
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Q28JEE Main 2025 · 23 JAN · SHIFT 1Medium

Work by a Variable Force · Force in two dimensions: line integral

A force f=x2yi^+y2j^f = x^2y\hat{i} + y^2\hat{j} acts on a particle in a plane x+y=10x + y = 10. The work done by this force during a displacement from (0,0)(0, 0) to (4 m,2 m)(4\text{ m}, 2\text{ m}) is _________ Joule (round off to the nearest integer)

Numerical answer type. Work it out, then open the answer.

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Answer: 152

  1. W=∫fx dx+∫fy dy=∫x2y dx+∫y2 dyW = \int f_x\,dx + \int f_y\,dy = \int x^2 y\,dx + \int y^2\,dy
  2. Using the given constraint y=10−xy = 10 - x in the first term: ∫04x2(10−x) dx=10x33−x44∣04=6403−64≈149.3 J\int_0^4 x^2(10 - x)\,dx = \frac{10x^3}{3} - \frac{x^4}{4}\Big|_0^4 = \frac{640}{3} - 64 \approx 149.3\text{ J}
  3. ∫02y2 dy=83≈2.7 J\int_0^2 y^2\,dy = \frac{8}{3} \approx 2.7\text{ J}
  4. W≈149.3+2.7=152 JW \approx 149.3 + 2.7 = 152\text{ J}
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Q29NEET 2024Medium

Work by a Variable Force · Force as a function of x: W = ∫F dx

An object moving along horizontal xx-direction with kinetic energy 10 J10\text{ J} is displaced through x=(3i^) mx = (3\hat{i})\text{ m} by the force F⃗=(−2i^+3j^) N\vec{F} = (-2\hat{i} + 3\hat{j})\text{ N}. The kinetic energy of the object at the end of the displacement xx is

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Answer: (c)

  1. W=F⃗⋅s⃗=(−2)(3)+3(0)=−6W = \vec{F}\cdot\vec{s} = (-2)(3) + 3(0) = -6 J
  2. Work-energy theorem: Kf=Ki+W=10−6=4K_f = K_i + W = 10 - 6 = 4 J
  3. So the answer is (c) 4 J4\text{ J}.
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Q30JEE Main 2023 · 11 APR · SHIFT 1Easy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A force F⃗=(2+3x)i^\vec{F} = (2 + 3x)\hat{i} acts on a particle in the xx direction where F is in newton and xx is in meter. The work done by this force during a displacement from x=0x = 0 to x=4 mx = 4\text{ m}, is __________ J.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 32

  1. W=∫04(2+3x) dx=[2x+3x22]04W = \int_0^4 (2 + 3x)\,dx = \left[2x + \frac{3x^2}{2}\right]_0^4
  2. W=8+24=32W = 8 + 24 = 32 J
  3. Work done =32= 32 J.
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Q31JEE Main 2023 · 1 FEB · SHIFT 2Easy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A force F=(5+3y2)F = \left(5 + 3y^2\right) acts on a particle in the yy-direction, where FF is in newton and yy is in meter. The work done by the force during a displacement from y=2 my = 2\text{ m} to y=5 my = 5\text{ m} is ___________ J.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 132

  1. W=∫25(5+3y2) dy=[5y+y3]25W = \int_2^5 (5 + 3y^2)\,dy = \left[5y + y^3\right]_2^5
  2. W=5(3)+(125−8)=15+117W = 5(3) + (125 - 8) = 15 + 117
  3. Work done =132= 132 J.
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Q32JEE Main 2023 · 15 APR · SHIFT 1Medium

Work by a Variable Force · Force as a function of x: W = ∫F dx

A block of mass 10 kg10\text{ kg} is moving along xx-axis under the action of force F=5x NF = 5x\text{ N}. The work done by the force in moving the block from x=2 mx = 2\text{ m} to 4 m4\text{ m} will be __________ J.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 30

  1. W=∫24F dx=∫245x dxW = \int_{2}^{4} F\,dx = \int_{2}^{4} 5x\,dx
  2. W=52(42−22)=52(12)W = \frac{5}{2}\left(4^2 - 2^2\right) = \frac{5}{2}(12)
  3. W=30 JW = 30\text{ J}
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Q33JEE Main 2023 · 6 APR · SHIFT 1Medium

Work by a Variable Force · Retardation proportional to displacement

A particle of mass 10 g10\text{ g} moves in a straight line with retardation 2x2x, where xx is the displacement in SI units. Its loss of kinetic energy for above displacement is (10x)−n\left(\frac{10}{x}\right)^{-n} J. The value of nn will be __________

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 2

  1. Retarding force F=m(2x)=0.01×2x=0.02xF = m(2x) = 0.01 \times 2x = 0.02x N.
  2. Loss of KE =∫0x0.02x dx=0.01x2=(x10)2= \int_0^x 0.02x\,dx = 0.01x^2 = \left(\frac{x}{10}\right)^2
  3. (x10)2=(10x)−2\left(\frac{x}{10}\right)^2 = \left(\frac{10}{x}\right)^{-2}, so n=2n = 2.
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Q34JEE Main 2023 · 25 JAN · SHIFT 1Difficult

Work by a Variable Force · Force as a function of x: W = ∫F dx

An object of mass 'm' initially at rest on a smooth horizontal plane starts moving under the action of force F = 2N. In the process of its linear motion, the angle θ\theta (as shown in figure) between the direction of force and horizontal varies as θ=kx\theta = kx, where k is a constant and xx is the distance covered by the object from its initial position. The expression of kinetic energy of the object will be E=nksin⁡θE = \frac{n}{k}\sin\theta. The value of n is ___________.

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 2

  1. Only the horizontal component does work on the smooth floor: dW=Fcos⁡θ dxdW = F\cos\theta\,dx with θ=kx\theta = kx.
  2. E=∫0x2cos⁡(kx) dx=2ksin⁡(kx)=2ksin⁡θE = \int_0^x 2\cos(kx)\,dx = \frac{2}{k}\sin(kx) = \frac{2}{k}\sin\theta
  3. Comparing with E=nksin⁡θE = \frac{n}{k}\sin\theta: n=2n = 2.
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Q35JEE Main 2022 · 26 JUN · SHIFT 2Easy

Work by a Variable Force · F-x graph: area = work

Arrange the four graphs in descending order of total work done; where W1, W2, W3 and W4 are the work done corresponding to figure a, b, c and d respectively.

FigureFigure
FigureFigure
Show answer and solution

Answer: (a)

  1. Work = signed area under each FF-xx graph (below the axis counts negative).
  2. (a): small negative triangle (0→x0)(0 \to x_0) + positive triangle (x0→x1)(x_0 \to x_1).
  3. (b): same as (a) plus a positive rectangle (x1→x2)(x_1 \to x_2), so W2>W1W_2 > W_1.
  4. (c): same as (b) plus a positive triangle beyond x2x_2, so W3>W2W_3 > W_2.
  5. (d): a small positive part, then a large negative area up to x2x_2; net is the least, so W4W_4 is smallest.
  6. So the answer is (a) W3>W2>W1>W4W_3 > W_2 > W_1 > W_4.
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Q36JEE Main 2022 · 28 JUN · SHIFT 2Medium

Work by a Variable Force · Force as a function of x: W = ∫F dx

A block of mass 2 kg moving on a horizontal surface with speed of 4 ms−1{}^{-1} enters a rough surface ranging from x = 0.5 m to x = 1.5 m. The retarding force in this range of rough surface is related to distance by F = −- kx where k = 12 Nm−1{}^{-1}. The speed of the block as it just crosses the rough surface will be:

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Answer: (c)

  1. Work by the retarding force: W=−∫0.51.512x dx=−6(1.52−0.52)=−12W = -\int_{0.5}^{1.5} 12x\,dx = -6(1.5^2 - 0.5^2) = -12 J
  2. Initial KE =12(2)(4)2=16= \frac{1}{2}(2)(4)^2 = 16 J, so final KE =16−12=4= 16 - 12 = 4 J
  3. 12(2)v2=4⇒v=2\frac{1}{2}(2)v^2 = 4 \Rightarrow v = 2 m/s
  4. So the answer is (c) 2.0 ms−1^{-1}.
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Q37JEE Main 2022 · 24 JUN · SHIFT 1Medium

Work by a Variable Force · Force in two dimensions: line integral

A particle experiences a variable force F⃗=(4xi^+3y2j^)\vec{F} = \left(4x\hat{i} + 3y^2\hat{j}\right) in a horizontal x-y plane. Assume distance in meters and force is newton. If the particle moves from point (1, 2) to point (2, 3) in the x-y plane, then Kinetic Energy changes by:

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Answer: (c)

  1. ΔK=W=∫Fx dx+∫Fy dy\Delta K = W = \int F_x\,dx + \int F_y\,dy
  2. ∫124x dx=2(4−1)=6 J\int_1^2 4x\,dx = 2(4 - 1) = 6\text{ J}
  3. ∫233y2 dy=27−8=19 J\int_2^3 3y^2\,dy = 27 - 8 = 19\text{ J}
  4. ΔK=6+19=25 J\Delta K = 6 + 19 = 25\text{ J}, so the answer is (c).
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Q38JEE Main 2021 · 25 JUL · SHIFT 2Easy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A force of F = (5y + 20)j^\hat{j} N acts on a particle. The work done by this force when the particle is moved from y = 0 m to y = 10 m is ___________ J.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 450

  1. W=∫010(5y+20) dy=[5y22+20y]010W = \int_0^{10} (5y + 20)\,dy = \left[\frac{5y^2}{2} + 20y\right]_0^{10}
  2. W=250+200W = 250 + 200
  3. Work done =450= 450 J.
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Q39JEE Main 2020 · 4 SEP · SHIFT 2Medium

Work by a Variable Force · F-x graph: area = work

A person pushes a box on a rough horizontal platform surface. He applies a force of 200 N over a distance of 15 m. Thereafter, he gets progressively tired and his applied force reduces linearly with distance to 100 N. The total distance through which the box has been moved is 30 m. What is the work done by the person during the total movement of the box?

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Answer: (b)

  1. Work = area under the FF-xx graph.
  2. First 15 m (constant 200 N): W1=200×15=3000 JW_1 = 200 \times 15 = 3000\text{ J}
  3. Next 15 m (200 N falling linearly to 100 N, trapezium): W2=12(200+100)(15)=2250 JW_2 = \frac{1}{2}(200 + 100)(15) = 2250\text{ J}
  4. W=3000+2250=5250 JW = 3000 + 2250 = 5250\text{ J}, so the answer is (b).
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Q40JEE Main 2020 · 9 JAN · SHIFT 1Difficult

Work by a Variable Force · Force in two dimensions: line integral

Consider a force F⃗=−xi^+yj^\vec{F} = -x\hat{i} + y\hat{j}. The work done by this force in moving a particle from point A(1, 0) to B(0, 1) along the line segment is: (all quantities are in SI units)

Figure

Show answer and solution

Answer: (c)

  1. W=∫Fx dx+∫Fy dyW = \int F_x\,dx + \int F_y\,dy from A(1, 0) to B(0, 1).
  2. ∫10(−x) dx=12\int_1^0 (-x)\,dx = \frac{1}{2}
  3. ∫01y dy=12\int_0^1 y\,dy = \frac{1}{2}
  4. W=12+12=1 JW = \frac{1}{2} + \frac{1}{2} = 1\text{ J}, so the answer is (c).
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Q41NEET 2019Easy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A force F = 20 + 10y acts on a particle in y-direction where F is in newton and y in meter. Work done by this force to move the particle from y = 0 to y = 1 m is:

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Answer: (b)

  1. W=∫01(20+10y) dy=[20y+5y2]01W = \int_0^1 (20 + 10y)\,dy = \left[20y + 5y^2\right]_0^1
  2. W=20+5=25W = 20 + 5 = 25 J
  3. So the answer is (b) 25 J.
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Q42NEET 2019Medium

Work by a Variable Force · F-x graph: area = work

An object of mass 500 g, initially at rest, is acted upon by a variable force whose X-component varies with X in the manner shown. The velocities of the object at the points X = 8 m and X = 12 m, would have the respective values of (nearly)

Figure

Show answer and solution

Answer: (d)

  1. Work = area under the FF-xx graph, and W=ΔKW = \Delta K (starts from rest, m=0.5 kgm = 0.5\text{ kg}).
  2. 0→80 \to 8 m: W=20×5+10×3=130 JW = 20 \times 5 + 10 \times 3 = 130\text{ J}, so v8=2×1300.5=520≈23 m/sv_8 = \sqrt{\frac{2 \times 130}{0.5}} = \sqrt{520} \approx 23\text{ m/s}.
  3. 8→128 \to 12 m: the large negative dip (down to −25-25 N) outweighs the +10+10 N strip, so net work is negative (about −24-24 J) and the speed must drop below 23 m/s.
  4. K12≈130−24=106 J⇒v12=2×1060.5≈20.6 m/sK_{12} \approx 130 - 24 = 106\text{ J} \Rightarrow v_{12} = \sqrt{\frac{2 \times 106}{0.5}} \approx 20.6\text{ m/s}
  5. So the answer is (d) 23 m/s and 20.6 m/s.
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Q43JEE Main 2019 · 8 APR · SHIFT 1Medium

Work by a Variable Force · F-x graph: area = work

A particle moves in one dimension from rest under the influence of a force that varies with the distance travelled by the particle as shown in the figure. The kinetic energy of the particle after it has travelled 3m is:

Figure

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Answer: (a)

  1. Starting from rest, K=W=K = W = area under the FF-xx graph.
  2. 0→20 \to 2 m: rectangle =2×2=4 J= 2 \times 2 = 4\text{ J}
  3. 2→32 \to 3 m: trapezium =12(2+3)(1)=2.5 J= \frac{1}{2}(2 + 3)(1) = 2.5\text{ J}
  4. K=4+2.5=6.5 JK = 4 + 2.5 = 6.5\text{ J}, so the answer is (a).
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Q44NEET 2015 · AIPMT · CANCELLED PAPEREasy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A block of mass 10 kg, moving in x direction with a constant speed of 10 m s−1{}^{-1}, is subjected to a retarding force F = 0.1x J/m during its travel from x = 20 m to 30 m. Its final KE will be

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Answer: (c)

  1. Initial KE =12(10)(10)2=500= \frac{1}{2}(10)(10)^2 = 500 J
  2. Work by retarding force W=−∫20300.1x dx=−0.05(900−400)=−25W = -\int_{20}^{30} 0.1x\,dx = -0.05(900 - 400) = -25 J
  3. Final KE =500−25=475= 500 - 25 = 475 J
  4. So the answer is (c) 475 J.
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Q45JEE Main 2014Medium

Work by a Variable Force · Force as a function of x: W = ∫F dx

When a rubber-band is stretched by a distance xx, it exerts restoring force of magnitude F=ax+bx2F = ax + bx^2 where aa and bb are constants. The work done in stretching the unstretched rubber-band by LL is:

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Answer: (c)

  1. Work done against a variable force: W=∫0LF dxW = \int_0^L F\,dx.
  2. W=∫0L(ax+bx2) dx=aL22+bL33W = \int_0^L (ax + bx^2)\,dx = \frac{aL^2}{2} + \frac{bL^3}{3}
  3. So the answer is (c) aL22+bL33\frac{aL^2}{2} + \frac{bL^3}{3}.
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Q46NEET 2011 · AIPMT · PRELIMSEasy

Work by a Variable Force · F-x graph: area = work

Force F on a particle moving in a straight line varies with distance d as shown in figure.

Figure

The work done on the particle during its displacement of 12 m is

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Answer: (d)

8 J5 J23712d (m)F (N)
  1. Work = area under the FF-dd graph.
  2. From 3 m to 7 m (rectangle): 2×4=82 \times 4 = 8 J
  3. From 7 m to 12 m (triangle): 12×5×2=5\frac{1}{2} \times 5 \times 2 = 5 J
  4. Total W=8+5=13W = 8 + 5 = 13 J, so the answer is (d) 13 J.
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Q47NEET 2005 · AIPMTEasy

Work by a Variable Force · F-x graph: area = work

A force F acting

Figure

on an object varies with distance x as shown here. The force is in N and x in m. The work done by the force in moving the object from x = 0 to x = 6 m is

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Answer: (b)

  1. Work = area under the FF-xx graph.
  2. From 0 to 3 m (rectangle): 3×3=93 \times 3 = 9 J
  3. From 3 m to 6 m (triangle): 12×3×3=4.5\frac{1}{2} \times 3 \times 3 = 4.5 J
  4. Total W=13.5W = 13.5 J, so the answer is (b) 13.5 J.
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Q48JEE Main 2004 · AIEEEMedium

Work by a Variable Force · Retardation proportional to displacement

A particle moves in a straight line with retardation proportional to its displacement. Its loss of kinetic energy for any displacement xx is proportional to

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Answer: (c)

  1. Retardation a=−kxa = -kx, so vdvdx=−kxv\frac{dv}{dx} = -kx.
  2. Loss of KE =∫0xmkx dx=12mkx2= \int_0^x m k x\,dx = \frac{1}{2}mkx^2
  3. So loss of KE ∝x2\propto x^2; the answer is (c).
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Q49NEET 1994 · AIPMTEasy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A body, constrained to move in yy-direction, is subjected to a force given by F⃗=(−2i^+15j^+6k^) N\vec{F} = (-2\hat{i} + 15\hat{j} + 6\hat{k})\text{ N}. The work done by this force in moving the body through a distance of 10j^ m10\hat{j}\text{ m} along yy-axis, is

Show answer and solution

Answer: (a)

  1. W=F⃗⋅s⃗W = \vec{F}\cdot\vec{s} with s⃗=10j^\vec{s} = 10\hat{j} m.
  2. Only the j^\hat{j} component contributes: W=15×10=150W = 15 \times 10 = 150 J
  3. So the answer is (a) 150 J150\text{ J}.
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Q50NEET 1994 · AIPMTEasy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A position dependent force, F=(7−2x+3x2) NF = (7 - 2x + 3x^2)\text{ N} acts on a small body of mass 2 kg2\text{ kg} and displaces it from x=0x = 0 to x=5 mx = 5\text{ m}. The work done in joule is

Show answer and solution

Answer: (a)

  1. W=∫05(7−2x+3x2) dx=[7x−x2+x3]05W = \int_0^5 (7 - 2x + 3x^2)\,dx = \left[7x - x^2 + x^3\right]_0^5
  2. W=35−25+125=135W = 35 - 25 + 125 = 135 J (mass is not needed)
  3. So the answer is (a) 135.
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Q51NEET 1992 · AIPMTEasy

Work by a Variable Force · Force as a function of x: W = ∫F dx

A position dependent force, F=(7−2x+3x2) NF = (7 - 2x + 3x^2)\text{ N} acts on a small body of mass 2 kg2\text{ kg} and displaces it from x=0x = 0 to x=5 mx = 5\text{ m}. The work done in joule is

Show answer and solution

Answer: (a)

  1. W=∫05(7−2x+3x2) dx=[7x−x2+x3]05W = \int_0^5 (7 - 2x + 3x^2)\,dx = \left[7x - x^2 + x^3\right]_0^5
  2. W=35−25+125=135W = 35 - 25 + 125 = 135 J (mass is not needed)
  3. So the answer is (a) 135.
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Q52MHT CET 2026 · 20 MAY · SHIFT 1Easy

Kinetic Energy & Momentum · K = p²/2m and percentage change

If 'm' is the mass of the body moving with velocity 'v' having kinetic energy 'E', then the linear momentum of the body is

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Answer: (d)

  1. E=p22mE = \frac{p^2}{2m}
  2. p=2mEp = \sqrt{2mE}, so the answer is (d).
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Q53MHT CET 2026 · 20 MAY · SHIFT 1Easy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

The kinetic energy of light body and a heavy body is same. Which one of the following statement is true?

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Answer: (b)

  1. p=2mKp = \sqrt{2mK}; for equal KK, p∝mp \propto \sqrt{m}.
  2. The heavier body has greater momentum, so the answer is (b).
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Q54MHT CET 2026 · 19 MAY · SHIFT 1Easy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

A 66 kg mass and 1.51.5 kg mass are moving with equal kinetic energies. The ratio of the magnitudes of their linear momenta is

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Answer: (b)

  1. Equal KE: p=2mK∝mp = \sqrt{2mK} \propto \sqrt{m}.
  2. p1p2=61.5=4=2\frac{p_1}{p_2} = \sqrt{\frac{6}{1.5}} = \sqrt{4} = 2
  3. So the answer is (b) 2:12 : 1.
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Q55MHT CET 2024 · 10 MAY · SHIFT 1Easy

Kinetic Energy & Momentum · K = p²/2m and percentage change

If the momentum of a body of mass ' mm ' is increased by 20%20\% then its kinetic energy increases by

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Answer: (a)

  1. K=p22mK = \frac{p^2}{2m}, so K∝p2K \propto p^2 for the same mass.
  2. p′=1.2p⇒K′=(1.2)2K=1.44Kp' = 1.2p \Rightarrow K' = (1.2)^2 K = 1.44K
  3. Increase =44%= 44\%, so the answer is (a).
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Q56JEE Main 2024 · 6 APR · SHIFT 2Easy

Kinetic Energy & Momentum · K = p²/2m and percentage change

When kinetic energy of a body becomes 36 times of its original value, the percentage increase in the momentum of the body will be:

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Answer: (b)

  1. p=2mKp = \sqrt{2mK}, so p∝Kp \propto \sqrt{K}.
  2. K′=36K⇒p′=6pK' = 36K \Rightarrow p' = 6p
  3. Increase =6p−pp×100=500%= \frac{6p - p}{p} \times 100 = 500\%, so the answer is (b).
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Q57JEE Main 2024 · 8 APR · SHIFT 1Easy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

Three bodies A, B and C have equal kinetic energies and their masses are 400 g,1.2 kg400\text{ g}, 1.2\text{ kg} and 1.6 kg1.6\text{ kg} respectively. The ratio of their linear momenta is:

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Answer: (a)

  1. Equal KE: p∝mp \propto \sqrt{m}.
  2. pA:pB:pC=0.4:1.2:1.6=1:3:4p_A : p_B : p_C = \sqrt{0.4} : \sqrt{1.2} : \sqrt{1.6} = \sqrt{1} : \sqrt{3} : \sqrt{4}
  3. =1:3:2= 1 : \sqrt{3} : 2, so the answer is (a).
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Q58JEE Main 2024 · 6 APR · SHIFT 1Easy

Kinetic Energy & Momentum · Equal momentum: lighter body has more KE

Four particles A,B,C,DA, B, C, D of mass m2,m,2m,4m\frac{m}{2}, m, 2m, 4m, have same momentum, respectively. The particle with maximum kinetic energy is:

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Answer: (d)

  1. Equal momentum: K=p22m∝1mK = \frac{p^2}{2m} \propto \frac{1}{m}.
  2. A has the smallest mass m2\frac{m}{2}, so it has the maximum KE. The answer is (d) A.
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Q59JEE Main 2023 · 13 APR · SHIFT 2Easy

Kinetic Energy & Momentum · K = p²/2m and percentage change

A car accelerates from rest to u m/su\text{ m/s}. The energy spent in this process is E J. The energy required to accelerate the car from u m/su\text{ m/s} to 2u m/s2u\text{ m/s} is nE JnE\text{ J}. The value of nn is ____________.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 3

  1. Energy spent = gain in KE.
  2. 0→u0 \to u: E=12mu2E = \frac{1}{2}mu^2
  3. u→2uu \to 2u: 12m(4u2−u2)=3×12mu2=3E\frac{1}{2}m(4u^2 - u^2) = 3 \times \frac{1}{2}mu^2 = 3E
  4. n=3n = 3
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Q60MHT CET 2023 · 10 MAY · SHIFT 1Easy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

If a lighter body of mass 'M1M_1' and velocity 'V1V_1' and a heavy body (mass M2M_2 and velocity V2V_2) have the same kinetic energy then

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Answer: (d)

  1. Momentum MV=2MKMV = \sqrt{2MK}; for equal KK, p∝Mp \propto \sqrt{M}.
  2. M2>M1⇒M2V2>M1V1M_2 > M_1 \Rightarrow M_2V_2 > M_1V_1, so the answer is (d).
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Q61JEE Main 2023 · 13 APR · SHIFT 1Easy

Kinetic Energy & Momentum · Equal momentum: lighter body has more KE

Two bodies are having kinetic energies in the ratio 16: 9. If they have same linear momentum, the ratio of their masses respectively is:

Show answer and solution

Answer: (c)

  1. Equal momentum: m∝1Km \propto \frac{1}{K}.
  2. m1m2=K2K1=916\frac{m_1}{m_2} = \frac{K_2}{K_1} = \frac{9}{16}
  3. So the answer is (c) 9:169 : 16.
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Q62MHT CET 2023 · 13 MAY · SHIFT 1Medium

Kinetic Energy & Momentum · Force, momentum & KE change

Using variation of force and time given below, final velocity of a particle of mass 2 kg2\text{ kg} moving with initial velocity 6 m/s6\text{ m/s} will be

Figure

Show answer and solution

Answer: (c)

  1. Impulse = area under the FF-tt graph =mΔv= m\Delta v.
  2. Taking the peak force as 6 N (the value the options are built on): impulse =12×6×4=12 N s= \frac{1}{2} \times 6 \times 4 = 12\text{ N s}.
  3. Δv=122=6 m/s\Delta v = \frac{12}{2} = 6\text{ m/s}
  4. v=6+6=12 m/sv = 6 + 6 = 12\text{ m/s}, so the answer is (c).
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Q63JEE Main 2023 · 8 APR · SHIFT 2Medium

Kinetic Energy & Momentum · Force, momentum & KE change

A body of mass 5 kg5\text{ kg} is moving with a momentum of 10 kg ms−110\text{ kg ms}^{-1}. Now a force of 2 N2\text{ N} acts on the body in the direction of its motion for 5 s5\text{ s}. The increase in the Kinetic energy of the body is ___________ J\text{J}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 30

  1. Initial p1=10 kg m/sp_1 = 10\text{ kg m/s}; impulse =Ft=2×5=10 N s= F t = 2 \times 5 = 10\text{ N s}, so p2=20 kg m/sp_2 = 20\text{ kg m/s}.
  2. K=p22mK = \frac{p^2}{2m}: K1=10010=10 JK_1 = \frac{100}{10} = 10\text{ J}, K2=40010=40 JK_2 = \frac{400}{10} = 40\text{ J}
  3. Increase in KE =40−10=30 J= 40 - 10 = 30\text{ J}
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Q64JEE Main 2021 · 17 MAR · SHIFT 1Easy

Kinetic Energy & Momentum · K = p²/2m and percentage change

A boy is rolling a 0.5 kg ball on the frictionless floor with the speed of 20 ms-1. The ball gets deflected by an obstacle on the way. After deflection it moves with 5% of its initial kinetic energy. What is the speed of the ball now?

Show answer and solution

Answer: (c)

  1. K∝v2K \propto v^2, so v′=vK′/Kv' = v\sqrt{K'/K}.
  2. v′=200.05=20×0.2236v' = 20\sqrt{0.05} = 20 \times 0.2236
  3. v′≈4.47 m/sv' \approx 4.47\text{ m/s}, so the answer is (c).
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Q65MHT CET 2021 · 24 SEP · SHIFT 2Easy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

The kinetic energy of a light body and a heavy body is same. Which one of them has greater momentum?

Show answer and solution

Answer: (b)

  1. p=2mKp = \sqrt{2mK}; for equal KK, p∝mp \propto \sqrt{m}.
  2. The heavy body has greater momentum, so the answer is (b).
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Q66MHT CET 2021 · 21 SEP · SHIFT 2Easy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

Three bodies P, Q and R have masses 'm' kg, '2m' kg and '3m' kg respectively. If all the bodies have equal kinetic energy, then greater momentum will be for body/bodies.

Show answer and solution

Answer: (b)

  1. Equal KE: p=2mK∝mp = \sqrt{2mK} \propto \sqrt{m}.
  2. R has the largest mass 3m3m, so it has the greatest momentum. The answer is (b) R.
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Q67JEE Main 2008 · AIEEEEasy

Kinetic Energy & Momentum · K = p²/2m and percentage change

An athlete in the Olympic games covers a distance of 100 m100\text{ m} in 10 s10\text{ s} His kinetic energy can be estimated to be in the range

Show answer and solution

Answer: (d)

  1. Average speed v=10010=10 m/sv = \frac{100}{10} = 10\text{ m/s}.
  2. An athlete's mass is about 40 to 100 kg.
  3. K=12mv2≈12(40 to 100)(100)=2000 to 5000 JK = \frac{1}{2}mv^2 \approx \frac{1}{2}(40\text{ to }100)(100) = 2000\text{ to }5000\text{ J}
  4. So the answer is (d).
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Q68NEET 2004 · AIPMTEasy

Kinetic Energy & Momentum · Equal momentum: lighter body has more KE

A particle of mass m1 is moving with a velocity v1 and another particle of mass m2 is moving with a velocity v2. Both of them have the same momentum but their different kinetic energies are E1 and E2 respectively. If m1 > m2 then:

Show answer and solution

Answer: (a)

  1. E=p22mE = \frac{p^2}{2m}; for equal pp, E∝1mE \propto \frac{1}{m}.
  2. m1>m2⇒E1<E2m_1 > m_2 \Rightarrow E_1 < E_2, so the answer is (a).
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Q69NEET 1999 · AIPMTEasy

Kinetic Energy & Momentum · Equal momentum: lighter body has more KE

Two bodies with kinetic energies in the ratio 4:14 : 1 are moving with equal linear momentum. The ratio of their masses is

Show answer and solution

Answer: (d)

  1. Equal momentum: K=p22m⇒m∝1KK = \frac{p^2}{2m} \Rightarrow m \propto \frac{1}{K}.
  2. m1m2=K2K1=14\frac{m_1}{m_2} = \frac{K_2}{K_1} = \frac{1}{4}
  3. So the answer is (d) 1:41 : 4.
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Q70NEET 1997 · AIPMTEasy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

Two bodies of masses mm and 4m4m are moving with equal kinetic energies. The ratio of their linear momenta is

Show answer and solution

Answer: (a)

  1. Equal KE: p∝mp \propto \sqrt{m}.
  2. p1p2=m4m=12\frac{p_1}{p_2} = \sqrt{\frac{m}{4m}} = \frac{1}{2}
  3. So the answer is (a) 1:21 : 2.
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Q71NEET 1993 · AIPMTEasy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

Two masses of 1 g1\text{ g} and 9 g9\text{ g} are moving with equal kinetic energies. The ratio of the magnitudes of their respective linear momenta is

Show answer and solution

Answer: (c)

  1. Equal KE: p∝mp \propto \sqrt{m}.
  2. p1p2=19=13\frac{p_1}{p_2} = \sqrt{\frac{1}{9}} = \frac{1}{3}
  3. So the answer is (c) 1:31 : 3.
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Q72NEET 1989 · AIPMTEasy

Kinetic Energy & Momentum · Equal KE: heavier body has more momentum

Two bodies of masses mm and 4m4m are moving with equal kinetic energies. The ratio of their linear momenta is

Show answer and solution

Answer: (a)

  1. Equal KE: p∝mp \propto \sqrt{m}.
  2. p1p2=m4m=12\frac{p_1}{p_2} = \sqrt{\frac{m}{4m}} = \frac{1}{2}
  3. So the answer is (a) 1:21 : 2.
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Q73JEE Main 2026 · 6 APR · SHIFT 1Easy

Work-Energy Theorem · Work by air resistance

The rain drop of mass 1 g, starts with zero velocity from a height of 1 km. It hits the ground with a speed of 5 m/s5\text{ m/s}. The work done by the unknown resistive force is ______ J.

(take g=10 m/s2g = 10\text{ m/s}^2)

Show answer and solution

Answer: (d)

  1. Wg=mgh=10−3×10×1000=10 JW_g = mgh = 10^{-3} \times 10 \times 1000 = 10\text{ J}
  2. Final KE =12(10−3)(5)2=0.0125 J= \frac{1}{2}(10^{-3})(5)^2 = 0.0125\text{ J}
  3. Wr=ΔK−Wg=0.0125−10=−9.9875≈−9.98 JW_r = \Delta K - W_g = 0.0125 - 10 = -9.9875 \approx -9.98\text{ J}
  4. So the answer is (d).
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Q74JEE Main 2026 · 6 APR · SHIFT 2Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A body of mass 1 kg moves along a straight line with a velocity v=2x2v = 2x^2. The work done by the body during displacement from x=0x = 0 to 5 m is ______ J.

Show answer and solution

Answer: (c)

  1. Net work == change in KE.
  2. v(0)=0v(0) = 0, v(5)=2(25)=50 m/sv(5) = 2(25) = 50\text{ m/s}
  3. W=12(1)(502)−0=1250 JW = \frac{1}{2}(1)(50^2) - 0 = 1250\text{ J}
  4. So the answer is (c) 1250.
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Q75JEE Main 2026 · 21 JAN · SHIFT 2Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A body of mass 2 kg is moving along x-direction such that its displacement as function of time is given by x(t)=αt2+βt+γx(t) = \alpha t^2 + \beta t + \gamma m, where α=1 m/s2,β=1 m/s\alpha = 1\text{ m/s}^2, \beta = 1\text{ m/s} and γ=1 m\gamma = 1\text{ m}. The work done on the body during the time interval t=2 st = 2\text{ s} to t=3 st = 3\text{ s}, is ________ J.

Show answer and solution

Answer: (b)

  1. v=dxdt=2αt+β=2t+1v = \frac{dx}{dt} = 2\alpha t + \beta = 2t + 1
  2. v(2)=5 m/sv(2) = 5\text{ m/s}, v(3)=7 m/sv(3) = 7\text{ m/s}
  3. W=12(2)(72−52)=49−25=24 JW = \frac{1}{2}(2)(7^2 - 5^2) = 49 - 25 = 24\text{ J}
  4. So the answer is (b) 24.
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Q76JEE Main 2026 · 2 APR · SHIFT 2Medium

Work-Energy Theorem · Bullet penetration

A spherical ball of mass 2 kg falls from a height of 10 m and is brought to rest after penetrating 10 cm into sand.

The average force exerted by sand on the ball is _________ N.

(Take g=10 m/s2g = 10\text{ m/s}^2)

Show answer and solution

Answer: (b)

  1. From release to rest: Wgravity+Wsand=0W_{gravity} + W_{sand} = 0.
  2. mg(h+d)=Fd⇒F=2×10×(10+0.1)0.1mg(h + d) = F d \Rightarrow F = \frac{2 \times 10 \times (10 + 0.1)}{0.1}
  3. F=2020 NF = 2020\text{ N}
  4. So the answer is (b) 2020.
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Q77NEET 2025Easy

Work-Energy Theorem · Stopping distance & braking

The kinetic energies of two similar cars AA and BB are 100 J and 225 J respectively. On applying brakes, car AA stops after 1000 m and car BB stops after 1500 m. If FAF_A and FBF_B are the forces applied by the brakes on cars AA and BB respectively, then the ratio of FAFB\frac{F_A}{F_B} is

Show answer and solution

Answer: (d)

  1. Work-energy theorem: braking force ×\times stopping distance == initial KE, so F=KdF = \frac{K}{d}.
  2. FA=1001000=0.1 NF_A = \frac{100}{1000} = 0.1\text{ N}, FB=2251500=0.15 NF_B = \frac{225}{1500} = 0.15\text{ N}
  3. FAFB=0.10.15=23\frac{F_A}{F_B} = \frac{0.1}{0.15} = \frac{2}{3}
  4. So the answer is (d) 23\frac{2}{3}.
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Q78JEE Main 2024 · 6 APR · SHIFT 1Easy

Work-Energy Theorem · Bullet penetration

A bullet of mass 50 g50\text{ g} is fired with a speed 100 m/s100\text{ m/s} on a plywood and emerges with 40 m/s40\text{ m/s}. The percentage loss of kinetic energy is:

Show answer and solution

Answer: (c)

  1. K∝v2K \propto v^2, so fractional loss =1−vf2vi2= 1 - \frac{v_f^2}{v_i^2}.
  2. =1−(40100)2=1−0.16=0.84= 1 - \left(\frac{40}{100}\right)^2 = 1 - 0.16 = 0.84
  3. So the answer is (c) 84%84\%.
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Q79JEE Main 2024 · 9 APR · SHIFT 1Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A particle of mass mm moves on a straight line with its velocity increasing with distance according to the equation v=αxv = \alpha\sqrt{x}, where α\alpha is a constant. The total work done by all the forces applied on the particle during its displacement from x=0x = 0 to x=dx = d, will be:

Show answer and solution

Answer: (c)

  1. Total work == change in KE.
  2. v(0)=0v(0) = 0, v(d)=αd⇒v2=α2dv(d) = \alpha\sqrt{d} \Rightarrow v^2 = \alpha^2 d
  3. W=12mα2dW = \frac{1}{2}m\alpha^2 d
  4. So the answer is (c) mα2d2\frac{m\alpha^2 d}{2}.
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Q80JEE Main 2024 · 27 JAN · SHIFT 2Medium

Work-Energy Theorem · Bullet penetration

A bullet is fired into a fixed target loses one third of its velocity after travelling 4 cm4\text{ cm}. It penetrates further D×10−3 mD \times 10^{-3}\text{ m} before coming to rest. The value of DD is:

Show answer and solution

Answer: (b)

  1. Constant resistance: distance ∝\propto KE lost.
  2. v→2v3v \to \frac{2v}{3}: KE goes K→4K9K \to \frac{4K}{9}, so 5K9\frac{5K}{9} is lost in 4 cm4\text{ cm}.
  3. Remaining 4K9\frac{4K}{9} needs 4×45=3.2 cm=32×10−3 m4 \times \frac{4}{5} = 3.2\text{ cm} = 32 \times 10^{-3}\text{ m}.
  4. So the answer is (b) D=32D = 32.
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Q81JEE Main 2023 · 31 JAN · SHIFT 1Medium

Work-Energy Theorem · Net work = change in KE

A lift of mass M=500 kgM = 500\text{ kg} is descending with speed of 2 ms−12\text{ ms}^{-1}. Its supporting cable begins to slip thus allowing it to fall with a constant acceleration of 2 ms−22\text{ ms}^{-2}. The kinetic energy of the lift at the end of fall through to a distance of 6 m6\text{ m} will be _____________ kJ\text{kJ}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 7

  1. v2=u2+2as=22+2(2)(6)=28 m2/s2v^2 = u^2 + 2as = 2^2 + 2(2)(6) = 28\text{ m}^2/\text{s}^2
  2. K=12Mv2=12(500)(28)=7000 JK = \frac{1}{2}Mv^2 = \frac{1}{2}(500)(28) = 7000\text{ J}
  3. So K=7 kJK = 7\text{ kJ}.
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Q82JEE Main 2023 · 24 JAN · SHIFT 1Medium

Work-Energy Theorem · Net work = change in KE

A spherical body of mass 2 kg starting from rest acquires a kinetic energy of 10000 J at the end of 5th5^{\text{th}} second. The force acted on the body is ________ N.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 40

  1. 12mv2=10000⇒v2=2×100002=104\frac{1}{2}mv^2 = 10000 \Rightarrow v^2 = \frac{2 \times 10000}{2} = 10^4, so v=100 m/sv = 100\text{ m/s} at t=5 st = 5\text{ s}.
  2. From rest, a=vt=1005=20 m/s2a = \frac{v}{t} = \frac{100}{5} = 20\text{ m/s}^2
  3. F=ma=2×20=40 NF = ma = 2 \times 20 = 40\text{ N}
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Q83JEE Main 2023 · 12 APR · SHIFT 1Medium

Work-Energy Theorem · Stopping distance & braking

Given below are two statements:

Statement I: A truck and a car moving with same kinetic energy are brought to rest by applying brakes which provide equal retarding forces. Both come to rest in equal distance. Statement II: A car moving towards east takes a turn and moves towards north, the speed remains unchanged. The acceleration of the car is zero.

In the light of given statements, choose the most appropriate answer from the options given below

Show answer and solution

Answer: (b)

  1. Statement I: Fs=KF s = K; same KK and same FF give the same ss. Correct.
  2. Statement II: the direction of velocity changes, so velocity changes and acceleration is not zero. Incorrect.
  3. So the answer is (b).
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Q84JEE Main 2022 · 25 JUL · SHIFT 1Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A body of mass 0.5 kg0.5\text{ kg} travels on straight line path with velocity v=(3x2+4) m/sv = \left(3x^2 + 4\right)\text{ m/s}. The net workdone by the force during its displacement from x=0x = 0 to x=2 mx = 2\text{ m} is:

Show answer and solution

Answer: (b)

  1. Net work == change in KE.
  2. v(0)=4 m/sv(0) = 4\text{ m/s}, v(2)=3(4)+4=16 m/sv(2) = 3(4) + 4 = 16\text{ m/s}
  3. W=12(0.5)(162−42)=0.25×240=60 JW = \frac{1}{2}(0.5)(16^2 - 4^2) = 0.25 \times 240 = 60\text{ J}
  4. So the answer is (b) 60 J.
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Q85JEE Main 2022 · 29 JUN · SHIFT 1Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A particle of mass 500 gm is moving in a straight line with velocity v = b x5/2. The work done by the net force during its displacement from x = 0 to x = 4 m is: (Take b = 0.25 m−3{}^{-3}/2 s−1{}^{-1}).

Show answer and solution

Answer: (d)

  1. Net work == change in KE.
  2. v(0)=0v(0) = 0, v(4)=0.25×45/2=0.25×32=8 m/sv(4) = 0.25 \times 4^{5/2} = 0.25 \times 32 = 8\text{ m/s}
  3. W=12(0.5)(82)=16 JW = \frac{1}{2}(0.5)(8^2) = 16\text{ J}
  4. So the answer is (d) 16 J.
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Q86JEE Main 2022 · 28 JUL · SHIFT 2Medium

Work-Energy Theorem · Bullet penetration

A bullet of mass 200 g200\text{ g} having initial kinetic energy 90 J90\text{ J} is shot inside a long swimming pool as shown in the figure. If its kinetic energy reduces to 40 J40\text{ J} within 1 s1\text{ s}, the minimum length of the pool, the bullet has to travel so that it completely comes to rest is

Figure

Show answer and solution

Answer: (a)

  1. 12(0.2)v2=K\frac{1}{2}(0.2)v^2 = K: K=90 J⇒v1=30 m/sK = 90\text{ J} \Rightarrow v_1 = 30\text{ m/s}; K=40 J⇒v2=20 m/sK = 40\text{ J} \Rightarrow v_2 = 20\text{ m/s}.
  2. Taking constant retardation: a=30−201=10 m/s2a = \frac{30 - 20}{1} = 10\text{ m/s}^2
  3. Distance to stop: s=v122a=90020=45 ms = \frac{v_1^2}{2a} = \frac{900}{20} = 45\text{ m}
  4. So the answer is (a) 45 m.
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Q87JEE Main 2021 · 1 SEP · SHIFT 2Easy

Work-Energy Theorem · Work by air resistance

A body of mass 'm' dropped from a height 'h' reaches the ground with a speed of 0.8 gh\sqrt{gh}. The value of work done by the air-friction is:

Show answer and solution

Answer: (a)

  1. Work-energy theorem: Wg+Wf=12mv2W_g + W_f = \frac{1}{2}mv^2.
  2. 12m(0.8gh)2=0.32 mgh\frac{1}{2}m(0.8\sqrt{gh})^2 = 0.32\,mgh
  3. Wf=0.32 mgh−mgh=−0.68 mghW_f = 0.32\,mgh - mgh = -0.68\,mgh, so the answer is (a).
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Q88JEE Main 2020 · 3 SEP · SHIFT 1Medium

Work-Energy Theorem · Net work = change in KE

A cricket ball of mass 0.15 kg is thrown vertically up by a bowling machine so that it rises to a maximum height of 20 m after leaving the machine. If the part pushing the ball applies a constant force F on the ball and moves horizontally a distance of 0.2 m while launching the ball, the value of F (in N) is (g = 10 ms–2) ____.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 150

  1. KE given by the machine becomes PE at the top: F×0.2=mghF \times 0.2 = mgh.
  2. mgh=0.15×10×20=30 Jmgh = 0.15 \times 10 \times 20 = 30\text{ J}
  3. F=300.2=150 NF = \frac{30}{0.2} = 150\text{ N}
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Q89MHT CET 2020 · 16 OCT · SHIFT 1Medium

Work-Energy Theorem · Stopping distance & braking

A vehicle of mass mm is moving with momentum pp on a rough horizontal road. The coefficient of friction between the tyres and the horizontal road is μ\mu. The stopping distance is (g=g = acceleration due to gravity)

Show answer and solution

Answer: (b)

  1. Friction work removes all KE: μmg s=p22m\mu mg\,s = \frac{p^2}{2m}.
  2. s=p22μgm2s = \frac{p^2}{2\mu g m^2}
  3. So the answer is (b) p22μgm2\frac{p^2}{2\mu g m^2}.
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Q90JEE Main 2019 · 10 JAN · SHIFT 2Easy

Work-Energy Theorem · Net work = change in KE

A particle which is experiencing a force, given by F⃗=3i^−12j^,\vec{F} = 3\hat{i} - 12\hat{j}, undergoes a displacement of d⃗=4i⃗\vec{d} = 4\vec{i} particle had a kinetic energy of 3 J at the beginning of the displacement, what is its kinetic energy at the end of the displacement?

Show answer and solution

Answer: (d)

  1. W=F⃗⋅d⃗=(3i^−12j^)⋅4i^=12 JW = \vec{F} \cdot \vec{d} = (3\hat{i} - 12\hat{j}) \cdot 4\hat{i} = 12\text{ J}
  2. Kf=Ki+W=3+12=15 JK_f = K_i + W = 3 + 12 = 15\text{ J}
  3. So the answer is (d).
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Q91JEE Main 2019 · 9 JAN · SHIFT 2Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A force acts on a 2 kg object so that its position is given as a function of time as x = 3t2 + 5. What is the work done by this force in first 5 seconds?

Show answer and solution

Answer: (d)

  1. v=dxdt=6tv = \frac{dx}{dt} = 6t: v(0)=0v(0) = 0, v(5)=30 m/sv(5) = 30\text{ m/s}
  2. W=ΔK=12(2)(302)=900 JW = \Delta K = \frac{1}{2}(2)(30^2) = 900\text{ J}
  3. So the answer is (d) 900 J.
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Q92JEE Main 2018 · 16 APR · SHIFT 1Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A body of mass m starts moving from rest along x-axis so that its velocity varies as v=asv = a\sqrt{s} where a is a constant and s is the distance covered by the body. The total work done by all the forces acting on the body in the first t seconds after the start of the motion is:

Show answer and solution

Answer: (a)

  1. v2=a2sv^2 = a^2 s; compare with v2=2acsv^2 = 2a_c s: constant acceleration ac=a22a_c = \frac{a^2}{2}.
  2. From rest, v=act=a2t2v = a_c t = \frac{a^2 t}{2}
  3. W=ΔK=12m(a2t2)2=18ma4t2W = \Delta K = \frac{1}{2}m\left(\frac{a^2 t}{2}\right)^2 = \frac{1}{8}ma^4t^2
  4. So the answer is (a) 18ma4t2\frac{1}{8}ma^4t^2.
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Q93NEET 2017Easy

Work-Energy Theorem · Work by air resistance

Consider a drop of rain water having mass 1 g falling from a height of 1 km. It hits the ground with a speed of 50 m s−1{}^{-1}. Take 'g' constant with a value 10 m s−2{}^{-2}. The work done by the (i) gravitational force and the (ii) resistive force of air is

Show answer and solution

Answer: (c)

  1. (i) Wg=mgh=10−3×10×1000=10 JW_g = mgh = 10^{-3} \times 10 \times 1000 = 10\text{ J}
  2. Final KE =12(10−3)(50)2=1.25 J= \frac{1}{2}(10^{-3})(50)^2 = 1.25\text{ J}
  3. (ii) Wg+Wair=ΔK⇒Wair=1.25−10=−8.75 JW_g + W_{air} = \Delta K \Rightarrow W_{air} = 1.25 - 10 = -8.75\text{ J}
  4. So the answer is (c).
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Q94JEE Main 2017Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A time dependent force F = 6t acts on a particle of mass 1 kg. If the particle starts from rest, the work done by the force during the first 1 sec. will be:

Show answer and solution

Answer: (b)

  1. a=Fm=6ta = \frac{F}{m} = 6t, so v=∫0t6t dt=3t2v = \int_0^t 6t\,dt = 3t^2.
  2. v(1)=3 m/sv(1) = 3\text{ m/s}
  3. W=ΔK=12(1)(32)=4.5 JW = \Delta K = \frac{1}{2}(1)(3^2) = 4.5\text{ J}
  4. So the answer is (b) 4.5 J.
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Q95JEE Main 2016 · 10 APR · SHIFT 1Medium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

Velocity-time graph for a body of mass 10 kg is shown in figure. Work-done on the body in first two seconds of the motion is:

Figure

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Answer: (c)

  1. From the graph: v=50−5tv = 50 - 5t (falls from 5050 to 00 in 10 s10\text{ s}).
  2. v(0)=50 m/sv(0) = 50\text{ m/s}, v(2)=40 m/sv(2) = 40\text{ m/s}
  3. W=ΔK=12(10)(402−502)=5×(−900)=−4500 JW = \Delta K = \frac{1}{2}(10)(40^2 - 50^2) = 5 \times (-900) = -4500\text{ J}
  4. So the answer is (c) −4500 J-4500\text{ J}.
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Q96JEE Main 2014 · 19 APR · SHIFT 1Medium

Work-Energy Theorem · Bullet penetration

A bullet loses (1n)th\left(\frac{1}{n}\right)^{th} of its velocity passing through one plank. The number of such planks that are required to stop the bullet can be:

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Answer: (a)

  1. Each plank removes the same energy FdFd. After one plank v′=v(1−1n)v' = v\left(1 - \frac{1}{n}\right).
  2. KE lost per plank =12mv2[1−(1−1n)2]=12mv2⋅2n−1n2= \frac{1}{2}mv^2\left[1 - \left(1 - \frac{1}{n}\right)^2\right] = \frac{1}{2}mv^2 \cdot \frac{2n - 1}{n^2}
  3. Number of planks =12mv2KE lost per plank=n22n−1= \frac{\frac{1}{2}mv^2}{\text{KE lost per plank}} = \frac{n^2}{2n - 1}
  4. So the answer is (a) n22n−1\frac{n^2}{2n-1}.
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Q97NEET 2009 · AIPMTEasy

Work-Energy Theorem · Work by air resistance

A body of mass 1 kg is thrown upwards with a velocity 20 m/s. It momentarily comes to rest after attaining a height of 18 m. How much energy is lost due to air friction? (g = 10 m/s2)

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Answer: (d)

  1. Initial KE =12(1)(20)2=200 J= \frac{1}{2}(1)(20)^2 = 200\text{ J}
  2. PE gained at 18 m =mgh=1×10×18=180 J= mgh = 1 \times 10 \times 18 = 180\text{ J}
  3. Energy lost to air friction =200−180=20 J= 200 - 180 = 20\text{ J}, so the answer is (d).
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Q98NEET 2006 · AIPMTEasy

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A body of mass 3 kg is under a constant force which causes a displacement s in metres in it, given by the relation s = 13\frac{1}{3} t2, where t is in seconds. Work done by the force in 2 seconds is

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Answer: (d)

  1. s=t23⇒v=dsdt=2t3s = \frac{t^2}{3} \Rightarrow v = \frac{ds}{dt} = \frac{2t}{3}; at t=0t = 0, v=0v = 0.
  2. At t=2t = 2 s: v=43 m/sv = \frac{4}{3}\text{ m/s}
  3. W=ΔK=12(3)(43)2=83 JW = \Delta K = \frac{1}{2}(3)\left(\frac{4}{3}\right)^2 = \frac{8}{3}\text{ J}
  4. So the answer is (d).
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Q99JEE Main 2006 · AIEEEMedium

Work-Energy Theorem · Net work = change in KE

A ball of mass 0.2 kg0.2\text{ kg} is thrown vertically upwards by applying a force by hand. If the hand moves 0.2 m0.2\text{ m} while applying the force and the ball goes upto 2 m2\text{ m} height further, find the magnitude of the force. (consider g=10 m/s2g = 10\text{ m/s}^2 ).

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Answer: (d)

  1. From start (rest) to top (rest): Whand+Wgravity=ΔK=0W_{hand} + W_{gravity} = \Delta K = 0.
  2. Ball rises 0.2+2=2.2 m0.2 + 2 = 2.2\text{ m} in total: F(0.2)=mg(2.2)F(0.2) = mg(2.2)
  3. F=0.2×10×2.20.2=22 NF = \frac{0.2 \times 10 \times 2.2}{0.2} = 22\text{ N}
  4. So the answer is (d) 22 N22\text{ N}.
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Q100JEE Main 2005 · AIEEEEasy

Work-Energy Theorem · Bullet penetration

A bullet fired into a fixed target loses half of its velocity after penetrating 3 cm3\text{ cm} How much further it will penetrate before coming to rest assuming that it faces constant resistance to motion?

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Answer: (c)

  1. Constant resistance FF: work done FxFx equals KE lost.
  2. Speed v→v2v \to \frac{v}{2}: KE falls from KK to K4\frac{K}{4}, so 3K4\frac{3K}{4} is lost in 3 cm3\text{ cm}.
  3. Remaining K4\frac{K}{4} is one-third of 3K4\frac{3K}{4}, so it needs 33=1 cm\frac{3}{3} = 1\text{ cm} more.
  4. So the answer is (c) 1.0 cm1.0\text{ cm}.
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Q101JEE Main 2002 · AIEEEEasy

Work-Energy Theorem · Bullet penetration

If a body loses half of its velocity on penetrating 3 cm3\text{ cm} in a wooden block, then how much will it penetrate more before coming to rest?

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Answer: (a)

  1. Constant resistance: distance ∝\propto KE lost.
  2. Half velocity means KE drops to 14\frac{1}{4}: 34K\frac{3}{4}K lost in 3 cm3\text{ cm}, so 14K\frac{1}{4}K per 1 cm1\text{ cm}.
  3. Remaining KE K4\frac{K}{4} is lost in 1 cm1\text{ cm}.
  4. So the answer is (a) 1 cm1\text{ cm}.
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Q102NEET 1998 · AIPMTMedium

Work-Energy Theorem · Work from v(x), x(t) or a v-t graph

A force acts on a 3.0 g3.0\text{ g} particle in such a way that the position of the particle as a function of time is given by x=3t−4t2+t3x = 3t - 4t^2 + t^3, where xx is in metre and tt in second. The work done during the first 4 s4\text{ s} is

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Answer: (d)

  1. v=dxdt=3−8t+3t2v = \frac{dx}{dt} = 3 - 8t + 3t^2
  2. v(0)=3 m/sv(0) = 3\text{ m/s}, v(4)=3−32+48=19 m/sv(4) = 3 - 32 + 48 = 19\text{ m/s}
  3. W=ΔK=12(3×10−3)(192−32)=1.5×10−3×352=0.528 JW = \Delta K = \frac{1}{2}(3 \times 10^{-3})(19^2 - 3^2) = 1.5 \times 10^{-3} \times 352 = 0.528\text{ J}
  4. So the answer is (d) 528 mJ528\text{ mJ}.
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Q103NEET 1994 · AIPMTEasy

Work-Energy Theorem · Net work = change in KE

The kinetic energy acquired by a mass mm in travelling distance dd, starting from rest, under the action of a constant force is directly proportional to

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Answer: (b)

  1. Work-energy theorem: K=W=FdK = W = Fd (starting from rest).
  2. FF and dd are fixed, so KK does not depend on mm: K∝m0K \propto m^0.
  3. So the answer is (b).
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Q104NEET 1989 · AIPMTEasy

Work-Energy Theorem · Work by air resistance

A bullet of mass 10 g10\text{ g} leaves a rifle at an initial velocity of 1000 m/s1000\text{ m/s} and strikes the earth at the same level with a velocity of 500 m/s500\text{ m/s}. The work done in joule overcoming the resistance of air will be

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Answer: (b)

  1. Same level, so gravity does no net work; the KE loss is the work against air resistance.
  2. W=12m(u2−v2)=12(0.01)(106−2.5×105)W = \frac{1}{2}m(u^2 - v^2) = \frac{1}{2}(0.01)(10^6 - 2.5 \times 10^5)
  3. W=0.005×7.5×105=3750 JW = 0.005 \times 7.5 \times 10^5 = 3750\text{ J}, so the answer is (b).
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Q105JEE Main 2026 · 22 JAN · SHIFT 2Easy

Potential Energy & Equilibrium · Conservative & non-conservative forces

Given below are two statements:

Statement I: An object moves from position r1r_1 to position r2r_2 under a conservative force field F⃗\vec{F}. The work done by the force is W=−∫r1r2F⃗⋅dr→W = -\int_{r_1}^{r_2} \vec{F} \cdot \overrightarrow{dr}.

Statement II: Any object moving from one location to another location can follow infinite number of paths. Therefore, the amount of work done by the object changes with the path it follows for a conservative force.

In the light of the above statements, choose the correct answer from the options given below:

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Answer: (c)

  1. Statement I: work done by the force is W=+∫r1r2F⃗⋅dr⃗W = +\int_{r_1}^{r_2} \vec F \cdot d\vec r; the minus sign gives ΔU\Delta U, not WW. False.
  2. Statement II: work by a conservative force is independent of path. False.
  3. So the answer is (c).
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Q106JEE Main 2026 · 21 JAN · SHIFT 1Medium

Potential Energy & Equilibrium · U-x graphs & allowed region

Potential energy ( VV) versus distance ( xx) is given by the graph. Rank various regions as per the magnitudes of the force ( FF) acting on a particle from high to low.

Figure

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Answer: (a)

  1. ∣F∣=∣dVdx∣|F| = \left|\frac{dV}{dx}\right| = slope of the graph.
  2. AB:11=1AB: \frac{1}{1} = 1, BC:31=3BC: \frac{3}{1} = 3, CD:0CD: 0, DE:12=0.5DE: \frac{1}{2} = 0.5
  3. FBC>FAB>FDE>FCDF_{BC} > F_{AB} > F_{DE} > F_{CD}
  4. So the answer is (a).
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Q107JEE Main 2025 · 7 APR · SHIFT 2Easy

Potential Energy & Equilibrium · Conservative & non-conservative forces

Which one of the following forces cannot be expressed in terms of potential energy?

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Answer: (a)

  1. A potential energy exists only for conservative forces.
  2. Friction is non-conservative (its work depends on path), so it has no potential energy.
  3. So the answer is (a) Frictional force.
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Q108JEE Main 2025 · 28 JAN · SHIFT 1Medium

Potential Energy & Equilibrium · Conservative & non-conservative forces

Given below are two statements: one is labelled as Assertion A and the other is labelled as Reason R\mathbf{R}

Assertion A: In a central force field, the work done is independent of the path chosen. Reason R: Every force encountered in mechanics does not have an associated potential energy. In the light of the above statements, choose the most appropriate answer from the options given below

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Answer: (b)

  1. A: a central force F(r)r^F(r)\hat r is conservative, so its work is path-independent. True.
  2. R: forces like friction have no potential energy. True.
  3. R talks about non-conservative forces, so it does not explain A.
  4. So the answer is (b).
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Q109JEE Main 2024 · 29 JAN · SHIFT 1Medium

Potential Energy & Equilibrium · Force from potential: F = −dU/dx

The potential energy function (in JJ) of a particle in a region of space is given as U=(2x2+3y3+2z)U = \left(2x^2 + 3y^3 + 2z\right). Here x,yx, y and zz are in meter. The magnitude of xx-component of force (in NN) acting on the particle at point P(1,2,3) mP(1, 2, 3)\text{ m} is:

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Answer: (a)

  1. Fx=−∂U∂x=−4xF_x = -\frac{\partial U}{\partial x} = -4x
  2. At x=1x = 1: Fx=−4 NF_x = -4\text{ N}, magnitude 4 N4\text{ N}.
  3. So the answer is (a) 4.
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Q110JEE Main 2022 · 24 JUN · SHIFT 2Medium

Potential Energy & Equilibrium · Equilibrium from U(r)

Potential energy as a function of r is given by U=Ar10−Br5U = \frac{A}{r^{10}} - \frac{B}{r^5}, where r is the interatomic distance, A and B are positive constants. The equilibrium distance between the two atoms will be:

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Answer: (c)

  1. dUdr=−10Ar11+5Br6=0\frac{dU}{dr} = -\frac{10A}{r^{11}} + \frac{5B}{r^6} = 0
  2. r5=2ABr^5 = \frac{2A}{B}
  3. So the answer is (c) (2AB)1/5\left(\frac{2A}{B}\right)^{1/5}.
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Q111JEE Main 2021 · 27 JUL · SHIFT 2Medium

Potential Energy & Equilibrium · U-x graphs & allowed region

Given below is the plot of a potential energy function U(x) for a system, in which a particle is in one dimensional motion, while a conservative force F(x) acts on it. Suppose that Emech = 8 J, the incorrect statement for this system is:

Figure

[ where K.E. = kinetic energy ]

Show answer and solution

Answer: (b)

  1. K=E−U=8−UK = E - U = 8 - U.
  2. (a) x>x4x > x_4: U=6U = 6, K=2 JK = 2\text{ J} constant. True.
  3. (b) x<x1x < x_1: U=8U = 8, K=0K = 0, so the particle is at rest, not moving. Incorrect.
  4. (c) x2x_2: U=0U = 0, K=8 JK = 8\text{ J} maximum. True. (d) x3x_3: U=4U = 4, K=4 JK = 4\text{ J}. True.
  5. So the answer is (b).
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Q112JEE Main 2021 · 25 FEB · SHIFT 1Medium

Potential Energy & Equilibrium · Equilibrium from U(r)

The potential energy (U) of a diatomic molecule is a function dependent on r (interatomic distance) as

U=αr10−βr5−3U = \frac{\alpha}{r^{10}} - \frac{\beta}{r^5} - 3

where, α\alpha and β\beta are positive constants. The equilibrium distance between two atoms will be (2αβ)ab\left(\frac{2\alpha}{\beta}\right)^{\frac{a}{b}}, where a = ___________.

Numerical answer type. Work it out, then open the answer.

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Answer: 1

  1. The constant −3-3 does not affect dUdr\frac{dU}{dr}.
  2. dUdr=−10αr11+5βr6=0⇒r5=2αβ\frac{dU}{dr} = -\frac{10\alpha}{r^{11}} + \frac{5\beta}{r^6} = 0 \Rightarrow r^5 = \frac{2\alpha}{\beta}
  3. r=(2αβ)1/5r = \left(\frac{2\alpha}{\beta}\right)^{1/5}, so ab=15\frac{a}{b} = \frac{1}{5} and a=1a = 1.
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Q113JEE Main 2020 · 6 SEP · SHIFT 1Medium

Potential Energy & Equilibrium · Equilibrium from U(r)

If the potential energy between two molecules is given by

U = −Ar6+Br12-\frac{A}{r^6} + \frac{B}{r^{12}},

then at equilibrium, separation between molecules, and the potential energy are:

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Answer: (a)

  1. dUdr=6Ar7−12Br13=0⇒r6=2BA\frac{dU}{dr} = \frac{6A}{r^7} - \frac{12B}{r^{13}} = 0 \Rightarrow r^6 = \frac{2B}{A}
  2. U=−Ar6+Br12=−A22B+BA24B2=−A24BU = -\frac{A}{r^6} + \frac{B}{r^{12}} = -\frac{A^2}{2B} + \frac{BA^2}{4B^2} = -\frac{A^2}{4B}
  3. So the answer is (a) (2BA)1/6,−A24B\left(\frac{2B}{A}\right)^{1/6}, -\frac{A^2}{4B}.
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Q114NEET 2013Easy

Potential Energy & Equilibrium · U-x graphs & allowed region

A particle with total energy E is moving in a potential energy region U(x). Motion of the particle is restricted to the region when

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Answer: (c)

  1. K=E−U(x)K = E - U(x) and K≥0K \ge 0.
  2. So the particle can only be where U(x)≤EU(x) \le E.
  3. So the answer is (c).
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Q115NEET 2012 · AIPMT · PRELIMSMedium

Potential Energy & Equilibrium · Equilibrium from U(r)

The potential energy of a particle in a force field is U=Ar2−BrU = \frac{A}{r^2} - \frac{B}{r} where A and B are positive constants and r is the distance of particle from the centre of the field. For stable equilibrium, the distance of the particle is

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Answer: (b)

  1. Equilibrium: dUdr=−2Ar3+Br2=0⇒r=2AB\frac{dU}{dr} = -\frac{2A}{r^3} + \frac{B}{r^2} = 0 \Rightarrow r = \frac{2A}{B}
  2. d2Udr2=6Ar4−2Br3=1r3(3B−2B)>0\frac{d^2U}{dr^2} = \frac{6A}{r^4} - \frac{2B}{r^3} = \frac{1}{r^3}(3B - 2B) > 0 there, so it is stable.
  3. So the answer is (b) 2AB\frac{2A}{B}.
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Q116NEET 2011 · AIPMT · PRELIMSEasy

Potential Energy & Equilibrium · Conservative & non-conservative forces

The potential energy of a system increases if work is done

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Answer: (b)

  1. ΔU=−Wconservative\Delta U = -W_{conservative}.
  2. When the system does work against a conservative force, that force does negative work, so ΔU>0\Delta U > 0.
  3. So the answer is (b).
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Q117NEET 2011 · AIPMT · PRELIMSMedium

Potential Energy & Equilibrium · U-x graphs & allowed region

A particle of mass m is released from rest and follows a parabolic path as shown. Assuming that the displacement of the mass from the origin is small, which graph correctly depicts the position of the particle as a function of time?

Figure

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Answer: (b)

  1. V∝x2V \propto x^2 gives F=−kxF = -kx, so the motion is SHM about x=0x = 0.
  2. Released from rest at a positive xx, so x=Acos⁡ωtx = A\cos\omega t: starts at maximum, smooth curve.
  3. So the answer is (b).
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Q118JEE Main 2010 · AIEEEDifficult

Potential Energy & Equilibrium · Equilibrium from U(r)

The potential energy function for the force between two atoms in a diatomic molecule is approximately given by U(x)=ax12−bx6,U(x) = \frac{a}{x^{12}} - \frac{b}{x^6}, where aa and bb are constants and xx is the distance between the atoms. If the dissociation energy of the molecule is

D=[U(x=∞)−Uat equilibrium],DD = \left[U(x = \infty) - U_{at\ equilibrium}\right], \quad D is

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Answer: (c)

  1. Equilibrium: dUdx=0⇒x6=2ab\frac{dU}{dx} = 0 \Rightarrow x^6 = \frac{2a}{b}.
  2. Ueq=ax12−bx6=ab24a2−b22a=−b24aU_{eq} = \frac{a}{x^{12}} - \frac{b}{x^6} = \frac{ab^2}{4a^2} - \frac{b^2}{2a} = -\frac{b^2}{4a}
  3. U(∞)=0U(\infty) = 0, so D=0−(−b24a)=b24aD = 0 - \left(-\frac{b^2}{4a}\right) = \frac{b^2}{4a}
  4. So the answer is (c) b24a\frac{b^2}{4a}.
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Q119JEE Main 2006 · AIEEEMedium

Potential Energy & Equilibrium · U-x graphs & allowed region

The potential energy of a 1 kg1\text{ kg} particle free to move along the xx-axis is given by V(x)=(x44−x22) JV(x) = \left(\frac{x^4}{4} - \frac{x^2}{2}\right)\text{ J}. The total mechanical energy of the particle is 2 J.2\text{ J}. Then, the maximum speed (in m/s\text{m/s}) is

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Answer: (a)

  1. Speed is maximum where VV is minimum: dVdx=x3−x=0⇒x=±1\frac{dV}{dx} = x^3 - x = 0 \Rightarrow x = \pm 1.
  2. Vmin=14−12=−14 JV_{min} = \frac{1}{4} - \frac{1}{2} = -\frac{1}{4}\text{ J}
  3. Kmax=2+14=94 J=12(1)v2⇒v=32 m/sK_{max} = 2 + \frac{1}{4} = \frac{9}{4}\text{ J} = \frac{1}{2}(1)v^2 \Rightarrow v = \frac{3}{\sqrt{2}}\text{ m/s}
  4. So the answer is (a) 32\frac{3}{\sqrt 2}.
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Q120NEET 1995 · AIPMTMedium

Potential Energy & Equilibrium · Equilibrium from U(r)

The potential energy between two atoms, in a molecule, is given by U(x)=ax12−bx6U(x) = \frac{a}{x^{12}} - \frac{b}{x^6} where aa and bb are positive constants and xx is the distance between the atoms. The atom is in stable equilibrium, when

Show answer and solution

Answer: (a)

  1. dUdx=−12ax13+6bx7=0\frac{dU}{dx} = -\frac{12a}{x^{13}} + \frac{6b}{x^7} = 0
  2. x6=2abx^6 = \frac{2a}{b} (this is a minimum of UU, so stable)
  3. So the answer is (a) x=(2ab)1/6x = \left(\frac{2a}{b}\right)^{1/6}.
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Q121MHT CET 2026 · 16 APR · SHIFT 1Easy

Spring & Elastic Energy · Block hits a spring

A block of mass 'm' moving on a frictionless horizontal surface collides with a spring of spring constant 'K' and compresses it through a distance 'x'. The maximum momentum of the block after collision is

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Answer: (b)

  1. Momentum is maximum just before compression starts (all energy is kinetic).
  2. 12mv2=12Kx2⇒v=xK/m\frac{1}{2}mv^2 = \frac{1}{2}Kx^2 \Rightarrow v = x\sqrt{K/m}
  3. p=mv=xKmp = mv = x\sqrt{Km}
  4. So the answer is (b) km x\sqrt{km}\,x.
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Q122MHT CET 2026 · 19 APR · SHIFT 1Medium

Spring & Elastic Energy · Stretching from x1 to x2

The spring is initially in unstretched condition. It is first stretched by a length 'xx' and the work done is W1W_1. Then again it is stretched by further length 'xx' when the work done is W2W_2. The value of W2W_2 is given by

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Answer: (c)

  1. W1=12kx2W_1 = \frac{1}{2}kx^2.
  2. Total work to stretch by 2x2x: 12k(2x)2=4W1\frac{1}{2}k(2x)^2 = 4W_1.
  3. W2=4W1−W1=3W1W_2 = 4W_1 - W_1 = 3W_1
  4. So the answer is (c) 3W13W_1.
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Q123JEE Main 2026 · 23 JAN · SHIFT 1Medium

Spring & Elastic Energy · Same force or same stretch

Two blocks with masses 100 g and 200 g are attached to the ends of springs AA and BB as shown in figure. The energy stored in AA is EE. The energy stored in BB, when spring constants kA,kBk_A, k_B of AA and BB, respectively satisfy the relation 4kA=3kB4k_A = 3k_B, is:

Figure

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Answer: (d)

  1. Each spring holds its block in equilibrium: F=mgF = mg, so E=F22kE = \frac{F^2}{2k}.
  2. EA=(0.1g)22kA=EE_A = \frac{(0.1g)^2}{2k_A} = E, EB=(0.2g)22kBE_B = \frac{(0.2g)^2}{2k_B}
  3. EBEA=4⋅kAkB=4⋅34=3\frac{E_B}{E_A} = 4 \cdot \frac{k_A}{k_B} = 4 \cdot \frac{3}{4} = 3
  4. So the answer is (d) 3E3E.
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Q124MHT CET 2026 · 15 MAY · SHIFT 2Medium

Spring & Elastic Energy · Spring launch

A sphere of mass 5050 gram is placed on a vertical spring. It is compressed by 0.40.4 m using a force 1010 N. When the spring is released the sphere will reach to a height of (g=10 m/s2g = 10\text{ m/s}^2)

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Answer: (b)

  1. k=Fx=100.4=25k = \frac{F}{x} = \frac{10}{0.4} = 25 N/m
  2. Stored energy =12(25)(0.4)2=2= \frac{1}{2}(25)(0.4)^2 = 2 J
  3. mgh=2⇒h=20.05×10=4mgh = 2 \Rightarrow h = \frac{2}{0.05 \times 10} = 4 m
  4. So the answer is (b) 44 m.
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Q125MHT CET 2024 · 9 MAY · SHIFT 1Easy

Spring & Elastic Energy · Hooke's law & U = ½kx²

The potential energy of a long spring when it is stretched by 3 cm is ' UU '. If the spring is stretched by 9 cm, potential energy stored in it will be

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Answer: (d)

  1. Spring energy U=12kx2U = \frac{1}{2}kx^2, so U∝x2U \propto x^2.
  2. U′U=(93)2=9\frac{U'}{U} = \left(\frac{9}{3}\right)^2 = 9
  3. So the answer is (d) 9U9U.
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Q126JEE Main 2024 · 8 APR · SHIFT 2Medium

Spring & Elastic Energy · Falling or hanging on a spring

Figure

A block is simply released from the top of an inclined plane as shown in the figure above. The maximum compression in the spring when the block hits the spring is:

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Answer: (d)

  1. Height of incline top: h=10sin⁡30∘=5h = 10\sin 30^\circ = 5 m, so energy =mgh=5×10×5=250= mgh = 5 \times 10 \times 5 = 250 J.
  2. Friction on the 2 m rough patch: μmgd=0.5×50×2=50\mu mg d = 0.5 \times 50 \times 2 = 50 J.
  3. Energy given to spring: 250−50=200=12(100)x2⇒x2=4250 - 50 = 200 = \frac{1}{2}(100)x^2 \Rightarrow x^2 = 4
  4. So the answer is (d) 22 m.
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Q127NEET 2023Easy

Spring & Elastic Energy · Hooke's law & U = ½kx²

The potential energy of a long spring when stretched by 2 cm2\text{ cm} is U. If the spring is stretched by 8 cm8\text{ cm}, potential energy stored in it will be:

Show answer and solution

Answer: (c)

  1. U=12kx2U = \frac{1}{2}kx^2, so U∝x2U \propto x^2.
  2. U′U=(82)2=16\frac{U'}{U} = \left(\frac{8}{2}\right)^2 = 16
  3. So the answer is (c) 16U16U.
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Q128JEE Main 2023 · 1 FEB · SHIFT 2Easy

Spring & Elastic Energy · Hooke's law & U = ½kx²

A block is fastened to a horizontal spring. The block is pulled to a distance x=10 cmx = 10\text{ cm} from its equilibrium position (at x=0x = 0) on a frictionless surface from rest. The energy of the block at x=5 cmx = 5\text{ cm} is 0.25 J0.25\text{ J}. The spring constant of the spring is ___________ Nm−1\text{Nm}^{-1}

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 67

  1. Released from rest at x=10x = 10 cm; at x=5x = 5 cm the kinetic energy equals the loss in spring PE.
  2. 12k(0.102−0.052)=0.25\frac{1}{2}k(0.10^2 - 0.05^2) = 0.25
  3. 12k(0.0075)=0.25⇒k=66.7≈67 N m−1\frac{1}{2}k(0.0075) = 0.25 \Rightarrow k = 66.7 \approx 67\ \text{N m}^{-1}
  4. So k≈67 N m−1k \approx 67\ \text{N m}^{-1}.
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Q129MHT CET 2023 · 10 MAY · SHIFT 2Medium

Spring & Elastic Energy · Falling or hanging on a spring

A ball of mass 'm\text{m}' is dropped from a height 's\text{s}' on a horizontal platform fixed at the top of a vertical spring. The platform is depressed by a distance 'hh'. The spring constant is ( g=\text{g} = acceleration due to gravity)

Show answer and solution

Answer: (b)

  1. The ball falls a total height s+hs + h; all this PE is stored in the spring at maximum depression.
  2. mg(s+h)=12kh2mg(s + h) = \frac{1}{2}kh^2
  3. So the answer is (b) k=2mg(s+h)h2k = \frac{2mg(s+h)}{h^2}.
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Q130NEET 2022 · PHASE 2Easy

Spring & Elastic Energy · Hooke's law & U = ½kx²

The restoring force of a spring with a block attached to the free end of the spring is represented by

Show answer and solution

Answer: (a)

xFF = −kx
  1. Restoring force obeys Hooke's law: Fx=−kxF_x = -kx.
  2. This is a straight line through the origin with negative slope (Fx<0F_x < 0 for x>0x > 0, Fx>0F_x > 0 for x<0x < 0).
  3. So the answer is (a).
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Q131JEE Main 2022 · 26 JUL · SHIFT 1Medium

Spring & Elastic Energy · Block hits a spring

As per the given figure, two blocks each of mass 250 g250\text{ g} are connected to a spring of spring constant 2 Nm−12\text{ Nm}^{-1}. If both are given velocity vv in opposite directions, then maximum elongation of the spring is:

Figure

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Answer: (b)

  1. Momenta are equal and opposite, so at maximum elongation both blocks are momentarily at rest.
  2. 2×12mv2=12kx2⇒x2=2mv2k2 \times \frac{1}{2}mv^2 = \frac{1}{2}kx^2 \Rightarrow x^2 = \frac{2mv^2}{k}
  3. x2=2(0.25)v22=v24x^2 = \frac{2(0.25)v^2}{2} = \frac{v^2}{4}
  4. So the answer is (b) v2\frac{v}{2}.
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Q132JEE Main 2022 · 28 JUL · SHIFT 1Medium

Spring & Elastic Energy · Block hits a spring

A block of mass 'm\text{m}' (as shown in figure) moving with kinetic energy E compresses a spring through a distance 25 cm25\text{ cm} when its speed is halved. The value of spring constant of used spring will be nE Nm−1\text{nE Nm}^{-1} for n=\text{n} = _________.

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 24

  1. Speed halves, so KE becomes E/4E/4; spring stores E−E4=3E4E - \frac{E}{4} = \frac{3E}{4}.
  2. 12k(0.25)2=3E4⇒k32=3E4\frac{1}{2}k(0.25)^2 = \frac{3E}{4} \Rightarrow \frac{k}{32} = \frac{3E}{4}
  3. k=24Ek = 24E
  4. So n=24n = 24.
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Q133JEE Main 2022 · 25 JUN · SHIFT 1Medium

Spring & Elastic Energy · Block hits a spring

A 0.5 kg block moving at a speed of 12 ms−1{}^{-1} compresses a spring through a distance 30 cm when its speed is halved. The spring constant of the spring will be _______________ Nm−1{}^{-1}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 600

  1. Initial KE =12(0.5)(122)=36= \frac{1}{2}(0.5)(12^2) = 36 J; at half speed KE =9= 9 J.
  2. Spring PE =36−9=27= 36 - 9 = 27 J =12k(0.3)2= \frac{1}{2}k(0.3)^2
  3. k=540.09=600k = \frac{54}{0.09} = 600
  4. So k=600 N m−1k = 600\ \text{N m}^{-1}.
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Q134JEE Main 2022 · 24 JUN · SHIFT 1Medium

Spring & Elastic Energy · Falling or hanging on a spring

A ball of mass 100 g is dropped from a height h = 10 cm on a platform fixed at the top of a vertical spring (as shown in figure). The ball stays on the platform and the platform is depressed by a distance h2\frac{h}{2}. The spring constant is _____________ Nm−1{}^{-1}.

(Use g = 10 ms−2{}^{-2})

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 120

  1. The ball falls h+h2=0.15h + \frac{h}{2} = 0.15 m in all; this PE goes into the spring.
  2. mg(0.15)=12k(0.05)2mg(0.15) = \frac{1}{2}k\left(0.05\right)^2
  3. 0.1×10×0.15=0.15=0.00125k0.1 \times 10 \times 0.15 = 0.15 = 0.00125k
  4. So k=120 N m−1k = 120\ \text{N m}^{-1}.
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Q135JEE Main 2021 · 18 MAR · SHIFT 2Easy

Spring & Elastic Energy · Block hits a spring

A ball of mass 4 kg, moving with a velocity of 10 ms−1{}^{-1}, collides with a spring of length 8 m and force constant 100 Nm−1{}^{-1}. The length of the compressed spring is x m. The value of x, to the nearest integer, is ____________.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 6

  1. 12mv2=12kc2\frac{1}{2}mv^2 = \frac{1}{2}kc^2, where cc is the compression.
  2. c=vmk=104100=2c = v\sqrt{\frac{m}{k}} = 10\sqrt{\frac{4}{100}} = 2 m
  3. Compressed length x=8−2=6x = 8 - 2 = 6 m
  4. So x=6x = 6.
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Q136MHT CET 2021 · 21 SEP · SHIFT 1Medium

Spring & Elastic Energy · Spring launch

A sphere of mass 25 gram is placed on a vertical spring. It is compressed by 0.2 m0.2\text{ m} using a force 5 N5\text{ N}. When the spring is released, the sphere will reach a height of (g=10 m/s2)\left(\text{g} = 10\text{ m/s}^2\right)

Show answer and solution

Answer: (d)

  1. k=Fx=50.2=25k = \frac{F}{x} = \frac{5}{0.2} = 25 N/m
  2. Stored energy =12(25)(0.2)2=0.5= \frac{1}{2}(25)(0.2)^2 = 0.5 J
  3. mgh=0.5⇒h=0.50.025×10=2mgh = 0.5 \Rightarrow h = \frac{0.5}{0.025 \times 10} = 2 m
  4. So the answer is (d) 22 m.
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Q137JEE Main 2021 · 20 JUL · SHIFT 1Medium

Spring & Elastic Energy · Spring launch

In a spring gun having spring constant 100 N/m a small ball 'B' of mass 100 g is put in its barrel (as shown in figure) by compressing the spring through 0.05 m. There should be a box placed at a distance 'd' on the ground so that the ball falls in it. If the ball leaves the gun horizontally at a height of 2 m above the ground. The value of d is _________ m. (g = 10 m/s2).

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 1

  1. Launch speed: 12kx2=12mv2⇒v=xk/m=0.051000≈1.58\frac{1}{2}kx^2 = \frac{1}{2}mv^2 \Rightarrow v = x\sqrt{k/m} = 0.05\sqrt{1000} \approx 1.58 m/s
  2. Time to fall 2 m: t=2Hg=0.4≈0.632t = \sqrt{\frac{2H}{g}} = \sqrt{0.4} \approx 0.632 s
  3. d=vt=1.58×0.632≈1d = vt = 1.58 \times 0.632 \approx 1 m
  4. So d=1d = 1 m.
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Q138JEE Main 2021 · 1 SEP · SHIFT 2Difficult

Spring & Elastic Energy · Block hits a spring

An engine is attached to a wagon through a shock absorber of length 1.5 m. The system with a total mass of 40,000 kg is moving with a speed of 72 kmh−1{}^{-1} when the brakes are applied to bring it to rest. In the process of the system being brought to rest, the spring of the shock absorber gets compressed by 1.0 m. If 90% of energy of the wagon is lost due to friction, the spring constant is ____________ ×\times 105 N/m.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 16

  1. v=72v = 72 km/h =20= 20 m/s; KE=12(40000)(202)=8×106KE = \frac{1}{2}(40000)(20^2) = 8 \times 10^6 J
  2. Spring gets 10%: 8×105=12k(1.0)28 \times 10^5 = \frac{1}{2}k(1.0)^2
  3. k=1.6×106=16×105k = 1.6 \times 10^6 = 16 \times 10^5 N/m
  4. So the answer is 1616.
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Q139JEE Main 2019 · 9 JAN · SHIFT 1Difficult

Spring & Elastic Energy · Falling or hanging on a spring

A block of mass m, lying on a smooth horizontal surface, is attached to a spring (of negligible mass) of spring constant k. The other end of the spring is fixed, as shown in the figure. The block is initially at rest in its equilibrium position. If now the block is pulled with a constant force F, the maximum speed of the block is:

Figure

Show answer and solution

Answer: (d)

  1. Speed is maximum where net force is zero: kx=F⇒x=F/kkx = F \Rightarrow x = F/k.
  2. Work-energy: Fx−12kx2=12mv2Fx - \frac{1}{2}kx^2 = \frac{1}{2}mv^2
  3. F2k−F22k=F22k=12mv2⇒v=Fmk\frac{F^2}{k} - \frac{F^2}{2k} = \frac{F^2}{2k} = \frac{1}{2}mv^2 \Rightarrow v = \frac{F}{\sqrt{mk}}
  4. So the answer is (d) Fmk\frac{F}{\sqrt{mk}}.
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Q140NEET 2015 · AIPMT · CANCELLED PAPERMedium

Spring & Elastic Energy · Same force or same stretch

Two similar springs P and Q have spring constants KP and KQ, such that KP > KQ. They are stretched first by the same amount (case a), then by the same force (case b). The work done by the springs WP and WQ are related as, in case (a) and case (b) respectively

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Answer: (a)

  1. Same stretch: W=12kx2∝kW = \frac{1}{2}kx^2 \propto k, and KP>KQK_P > K_Q, so WP>WQW_P > W_Q.
  2. Same force: W=F22k∝1kW = \frac{F^2}{2k} \propto \frac{1}{k}, so WQ>WPW_Q > W_P.
  3. So the answer is (a) WP>WQW_P > W_Q; WQ>WPW_Q > W_P.
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Q141JEE Main 2015 · 10 APR · SHIFT 1Medium

Spring & Elastic Energy · Block hits a spring

A block of mass m = 0.1 kg is connected to a spring of unknown spring constant k. It is compressed to a distance x from its equilibrium position and released from rest.

After approaching half the distance (x2)\left(\frac{x}{2}\right) from equilibrium position, it hits another block and comes to rest momentarily, while the other block moves with a velocity 3 ms−1{}^{-1}. The total initial energy of the spring is:

Show answer and solution

Answer: (b)

  1. The block stops and the other block moves at 33 m/s, so (equal-mass elastic collision) the block's speed at x/2x/2 was 33 m/s.
  2. KE at x/2x/2: 12(0.1)(32)=0.45\frac{1}{2}(0.1)(3^2) = 0.45 J
  3. This equals spring PE released: 12k(x2−x24)=34E0\frac{1}{2}k\left(x^2 - \frac{x^2}{4}\right) = \frac{3}{4}E_0
  4. E0=43(0.45)=0.6E_0 = \frac{4}{3}(0.45) = 0.6 J
  5. So the answer is (b) 0.60.6 J.
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Q142JEE Main 2014 · 12 APR · SHIFT 1Difficult

Spring & Elastic Energy · Hooke's law & U = ½kx²

A spring of unstretched length ll has a mass m with one end fixed to a rigid support. Assuming spring to be made of a uniform wire, the kinetic energy possessed by it if its free end is pulled with uniform velocity vv is:

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Answer: (d)

  1. An element at distance yy from the fixed end moves with speed vyl\frac{vy}{l}; its mass is mldy\frac{m}{l}dy.
  2. K=∫0l12ml(vyl)2dy=mv22l3⋅l33K = \int_0^l \frac{1}{2}\frac{m}{l}\left(\frac{vy}{l}\right)^2 dy = \frac{mv^2}{2l^3}\cdot\frac{l^3}{3}
  3. So the answer is (d) 16mv2\frac{1}{6}mv^2.
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Q143JEE Main 2013 · 9 APR · SHIFT 1Medium

Spring & Elastic Energy · Same force or same stretch

Two springs of force constants 300 N/m (Spring A) and 400 N/m (Spring B) are joined together in series. The combination is compressed by 8.75 cm. The ratio of energy stored in A and B is EAEB\frac{E_A}{E_B}. Then EAEB\frac{E_A}{E_B} is equal to:

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Answer: (a)

  1. In series both springs carry the same force FF, so E=F22kE = \frac{F^2}{2k}.
  2. EAEB=kBkA=400300\frac{E_A}{E_B} = \frac{k_B}{k_A} = \frac{400}{300}
  3. So the answer is (a) 43\frac{4}{3}.
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Q144JEE Main 2012 · AIEEEMedium

Spring & Elastic Energy · Same force or same stretch

This question has Statement 11 and Statement 2.2. Of the four choices given after the Statements, choose the one that best describes the two Statements.

If two springs S1S_1 and S2S_2 of force constants k1k_1 and k2k_2, respectively, are stretched by the same force, it is found that more work is done on spring S1S_1 than on spring S2S_2.

STATEMENT 1: If stretched by the same amount, work done on S1S_1 is more than that on S2S_2 STATEMENT 2: k1<k2k_1 < k_2

Show answer and solution

Answer: (a)

  1. Same force: W=F22kW = \frac{F^2}{2k}; more work on S1S_1 means k1<k2k_1 < k_2, so Statement 2 is true.
  2. Same stretch: W=12kx2W = \frac{1}{2}kx^2; since k1<k2k_1 < k_2, work on S1S_1 is less, so Statement 1 is false.
  3. So the answer is (a).
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Q145NEET 2012 · AIPMT · PRELIMSMedium

Spring & Elastic Energy · Block hits a spring

A solid cylinder of mass 3 kg is rolling on a horizontal surface with velocity 4 m s−1{}^{-1}. It collides with a horizontal spring of force constant 200 N m−1{}^{-1}. The maximum compression produced in the spring will be

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Answer: (b)

  1. Rolling solid cylinder: KE=12mv2+12⋅12mr2ω2=34mv2KE = \frac{1}{2}mv^2 + \frac{1}{2}\cdot\frac{1}{2}mr^2\omega^2 = \frac{3}{4}mv^2.
  2. KE=34(3)(42)=36KE = \frac{3}{4}(3)(4^2) = 36 J
  3. 12(200)x2=36⇒x2=0.36\frac{1}{2}(200)x^2 = 36 \Rightarrow x^2 = 0.36
  4. So the answer is (b) 0.60.6 m.
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Q146NEET 2009 · AIPMTMedium

Spring & Elastic Energy · Falling or hanging on a spring

A block of mass M is attached to the lower end of a vertical spring. The spring is hung from a ceiling and has force constant value k. The mass is released from rest with the spring initially unstretched. The maximum extension produced in the length of the spring will be

Show answer and solution

Answer: (a)

  1. At maximum extension the block is momentarily at rest.
  2. Loss in gravitational PE = gain in spring PE: Mgx=12kx2Mgx = \frac{1}{2}kx^2
  3. So the answer is (a) x=2Mgkx = \frac{2Mg}{k}.
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Q147JEE Main 2007 · AIEEEMedium

Spring & Elastic Energy · Block hits a spring

A 2 kg2\text{ kg} block slides on a horizontal floor with a speed of 4 m/s.4\text{ m/s}. It strikes an uncompressed spring and compresses it till the block is motionless. The kinetic friction force is 15 N15\text{ N} and spring constant is 10,000 N/m.10{,}000\text{ N/m}. The spring compresses by

Show answer and solution

Answer: (b)

  1. Work-energy: 12mv2=fx+12kx2\frac{1}{2}mv^2 = fx + \frac{1}{2}kx^2.
  2. 16=15x+5000x2⇒5000x2+15x−16=016 = 15x + 5000x^2 \Rightarrow 5000x^2 + 15x - 16 = 0
  3. x=−15+225+32000010000≈0.055x = \frac{-15 + \sqrt{225 + 320000}}{10000} \approx 0.055 m
  4. So the answer is (b) 5.55.5 cm.
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Q148NEET 2007 · AIPMTMedium

Spring & Elastic Energy · Falling or hanging on a spring

A vertical spring with force constant k is fixed on a table. A ball of mass m at a height h above the free upper end of the spring falls vertically on the spring so that the spring is compressed by a distance d. The net work done in the process is

Show answer and solution

Answer: (a)

  1. Gravity acts over the full fall h+dh + d: Wg=mg(h+d)W_g = mg(h+d).
  2. Spring force does Ws=−12kd2W_s = -\frac{1}{2}kd^2.
  3. So the answer is (a) mg(h+d)−12kd2mg(h+d) - \frac{1}{2}kd^2.
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Q149NEET 2006 · AIPMTEasy

Spring & Elastic Energy · Hooke's law & U = ½kx²

The potential energy of a long spring when stretched by 2 cm is U. If the spring is stretched by 8 cm the potential energy stored in it is

Show answer and solution

Answer: (d)

  1. U=12kx2⇒U∝x2U = \frac{1}{2}kx^2 \Rightarrow U \propto x^2.
  2. U′U=(82)2=16\frac{U'}{U} = \left(\frac{8}{2}\right)^2 = 16
  3. So the answer is (d) 16U16U.
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Q150NEET 2004 · AIPMTEasy

Spring & Elastic Energy · Block hits a spring

A mass of 0.5 kg moving with a speed of 1.5 m/s on horizontal smooth surface, collides with a nearly weightless spring of force constant k = 50 N/m. The maximum compression of the spring would be

Figure

Show answer and solution

Answer: (a)

  1. All kinetic energy goes into the spring: 12mv2=12kx2\frac{1}{2}mv^2 = \frac{1}{2}kx^2.
  2. x=vmk=1.50.550=1.5×0.1x = v\sqrt{\frac{m}{k}} = 1.5\sqrt{\frac{0.5}{50}} = 1.5 \times 0.1
  3. So the answer is (a) 0.150.15 m.
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Q151NEET 2003 · AIPMTEasy

Spring & Elastic Energy · Hooke's law & U = ½kx²

When a long spring is stretched by 2 cm, its potential energy is U. If the spring is stretched by 10 cm, the potential energy stored in it will be

Show answer and solution

Answer: (d)

  1. U=12kx2⇒U∝x2U = \frac{1}{2}kx^2 \Rightarrow U \propto x^2.
  2. U′U=(102)2=25\frac{U'}{U} = \left(\frac{10}{2}\right)^2 = 25
  3. So the answer is (d) 25U25U.
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Q152JEE Main 2003 · AIEEEEasy

Spring & Elastic Energy · Stretching from x1 to x2

A spring of spring constant 5×103 N/m5 \times 10^{3}\text{ N/m} is stretched initially by 5 cm5\text{ cm} from the unstretched position. Then the work required to stretch it further by another 5 cm5\text{ cm} is

Show answer and solution

Answer: (b)

  1. W=12k(x22−x12)W = \frac{1}{2}k(x_2^2 - x_1^2) with x1=0.05x_1 = 0.05 m, x2=0.10x_2 = 0.10 m.
  2. W=12(5000)(0.01−0.0025)=2500×0.0075W = \frac{1}{2}(5000)(0.01 - 0.0025) = 2500 \times 0.0075
  3. W=18.75W = 18.75 N m
  4. So the answer is (b) 18.7518.75 N-m.
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Q153JEE Main 2002 · AIEEEEasy

Spring & Elastic Energy · Stretching from x1 to x2

A spring of force constant 800 N/m800\text{ N/m} has an extension of 5 cm.5\text{ cm}. The work done in extending it from 5 cm5\text{ cm} to 15 cm15\text{ cm} is

Show answer and solution

Answer: (b)

  1. W=12k(x22−x12)W = \frac{1}{2}k(x_2^2 - x_1^2) with x1=0.05x_1 = 0.05 m, x2=0.15x_2 = 0.15 m.
  2. W=12(800)(0.0225−0.0025)=400×0.02W = \frac{1}{2}(800)(0.0225 - 0.0025) = 400 \times 0.02
  3. So the answer is (b) 88 J.
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Q154NEET 2001 · AIPMTEasy

Spring & Elastic Energy · Same force or same stretch

Two springs A and B having spring constant KA and KB (KA = 2KB) are stretched by applying force of equal magnitude. If energy stored in spring A is EA then energy stored in B will be

Show answer and solution

Answer: (a)

  1. For the same force F=kx⇒x=F/kF = kx \Rightarrow x = F/k, so E=12kx2=F22kE = \frac{1}{2}kx^2 = \frac{F^2}{2k}.
  2. E∝1kE \propto \frac{1}{k}: EBEA=kAkB=2\frac{E_B}{E_A} = \frac{k_A}{k_B} = 2
  3. So the answer is (a) 2EA2E_A.
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Q155JEE Main 2026 · 23 JAN · SHIFT 1Medium

Conservation of Energy · Projectile: KE & PE at the top

An object is projected with kinetic energy KK from a point AA at an angle 60∘60^\circ with the horizontal. The ratio of the difference in kinetic energies at points BB and CC to that at point AA (see figure), in the absence of air friction is:

Figure

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Answer: (a)

  1. A and C are at the same level, so KC=KA=KK_C = K_A = K.
  2. At the top B only ucos⁡60∘u\cos 60^\circ remains: KB=Kcos⁡260∘=K4K_B = K\cos^2 60^\circ = \frac{K}{4}.
  3. KC−KB=K−K4=3K4K_C - K_B = K - \frac{K}{4} = \frac{3K}{4}
  4. Ratio to KAK_A: 34\frac{3}{4}. So the answer is (a) 3:43 : 4.
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Q156JEE Main 2026 · 6 APR · SHIFT 2Medium

Conservation of Energy · Tracks, hills & pulleys

The velocity at which 6 kg mass (shown in figure) strikes the ground when it is released from a height of 6 m above the ground is ‾ m/s\underline{\qquad}\ \text{m/s}. Assume pulley is massless and string is light and inextensible. (Take g=10 m/s2\text{g} = 10\text{ m/s}^2)

Figure

Show answer and solution

Answer: (a)

  1. Energy conservation for the system: the 6 kg falls 6 m while the 2 kg rises 6 m; both have the same speed vv.
  2. (6−2)×10×6=12(6+2)v2(6 - 2) \times 10 \times 6 = \frac{1}{2}(6 + 2)v^2
  3. 240=4v2⇒v2=60240 = 4v^2 \Rightarrow v^2 = 60
  4. v=60≈7.74 m/sv = \sqrt{60} \approx 7.74\text{ m/s}, option (a).
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Q157MHT CET 2026 · 19 MAY · SHIFT 1Medium

Conservation of Energy · Pendulum & swing

The bob of a simple pendulum of length 2m is kept at P. It is released and when it reaches Q, it losses 20% of its total energy due to air resistance. Its velocity at Q is [Take g=9.8g = 9.8 m/s2{}^{2} ]

Figure

Show answer and solution

Answer: (c)

  1. Bob falls through h=2 mh = 2\text{ m} from P to Q; total energy (relative to Q) is mghmgh.
  2. 20% is lost, so 12mv2=0.8 mgh\frac{1}{2}mv^2 = 0.8\,mgh.
  3. v=2×0.8×9.8×2=31.36v = \sqrt{2 \times 0.8 \times 9.8 \times 2} = \sqrt{31.36}
  4. v=5.6 m/sv = 5.6\text{ m/s}. So the answer is (c).
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Q158JEE Main 2026 · 23 JAN · SHIFT 2Difficult

Conservation of Energy · Tracks, hills & pulleys

A bead PP sliding on a frictionless semi-circular string (ACB)(ACB) and it is at point SS at t=0t = 0 and at this instant the horizontal component of its velocity is vv. Another bead QQ of the same mass as PP is ejected from point AA at t=0t = 0 along the horizontal string ABAB, with the speed vv, friction between the beads and the respective strings may be neglected in both cases. Let tPt_P and tQt_Q be the respective times taken by beads PP and QQ to reach the point BB, then the relation between tPt_P and tQt_Q is

Figure

Show answer and solution

Answer: (a)

  1. Bead Q has constant speed vv along AB: tQ=2Rvt_Q = \frac{2R}{v}.
  2. At S the radius is at 45∘45^\circ, so the velocity is at 45∘45^\circ too: speed of P =vcos⁡45∘=2v= \frac{v}{\cos 45^\circ} = \sqrt{2}v.
  3. Path of P is arc SCB =3πR4≈2.36R= \frac{3\pi R}{4} \approx 2.36R; at speed 2v\sqrt{2}v this takes about 2.36R1.41v≈1.67Rv\frac{2.36R}{1.41v} \approx 1.67\frac{R}{v}.
  4. P speeds up while dipping to C, so its time stays below 2R/v2R/v (a full calculation gives tP≈0.83t_P \approx 0.83 to 0.95 tQ0.95\,t_Q).
  5. So the answer is (a) tP<tQt_P < t_Q.
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Q159MHT CET 2025 · 19 APR · SHIFT 2Easy

Conservation of Energy · Projectile: KE & PE at the top

A stone is projected with kinetic energy E, making an angle θ\theta with the horizontal. When it reaches a highest point, its kinetic energy is

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Answer: (c)

  1. At the highest point only the horizontal velocity vcos⁡θv\cos\theta remains.
  2. KEtop=12mv2cos⁡2θ=Ecos⁡2θKE_{top} = \frac{1}{2}m v^2\cos^2\theta = E\cos^2\theta
  3. So the answer is (c) Ecos⁡2θE\cos^2\theta.
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Q160JEE Main 2025 · 23 JAN · SHIFT 2Easy

Conservation of Energy · Projectile: KE & PE at the top

A ball having kinetic energy KE, is projected at an angle of 60∘60^\circ from the horizontal. What will be the kinetic energy of ball at the highest point of its flight?

Show answer and solution

Answer: (c)

  1. At the top, KE=KE0cos⁡2θKE = KE_0\cos^2\theta.
  2. cos⁡260∘=14\cos^2 60^\circ = \frac{1}{4}
  3. So the answer is (c) KE4\frac{KE}{4}.
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Q161JEE Main 2025 · 3 APR · SHIFT 1Medium

Conservation of Energy · Free fall: K and U at a height

A particle is released from height SS above the surface of the earth. At certain height its kinetic energy is three times its potential energy. The height from the surface of the earth and the speed of the particle at that instant are respectively.

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Answer: (c)

  1. Total energy mgS=K+UmgS = K + U and K=3UK = 3U, so 4U=mgS4U = mgS.
  2. mgh=mgS4⇒h=S4mgh = \frac{mgS}{4} \Rightarrow h = \frac{S}{4}
  3. Fall distance =3S4= \frac{3S}{4}: v=2g⋅3S4=3gS2v = \sqrt{2g \cdot \frac{3S}{4}} = \sqrt{\frac{3gS}{2}}
  4. So the answer is (c) S4,3gS2\frac{S}{4}, \sqrt{\frac{3gS}{2}}.
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Q162JEE Main 2025 · 28 JAN · SHIFT 1Difficult

Conservation of Energy · Tracks, hills & pulleys

A bead of mass ' mm ' slides without friction on the wall of a vertical circular hoop of radius ' RR ' as shown in figure. The bead moves under the combined action of gravity and a massless spring (k) attached to the bottom of the hoop. The equilibrium length of the spring is ' RR '. If the bead is released from top of the hoop with (negligible) zero initial speed, velocity of bead, when the length of spring becomes ' RR ', would be (spring constant is ' kk ', gg is acceleration due to gravity)

Figure

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Answer: (b)

  1. Spring length becomes RR at the point where chord from the bottom =R= R: 2Rsin⁡θ2=R⇒θ=60∘2R\sin\frac{\theta}{2} = R \Rightarrow \theta = 60^\circ from the bottom.
  2. Height of that point above the bottom =R(1−cos⁡60∘)=R2= R(1 - \cos 60^\circ) = \frac{R}{2}, so the bead falls 2R−R2=3R22R - \frac{R}{2} = \frac{3R}{2}.
  3. At the top the spring (length 2R2R) is stretched by RR; at the new point it is relaxed.
  4. 12kR2+mg3R2=12mv2⇒v=3Rg+kR2m\frac{1}{2}kR^2 + mg\frac{3R}{2} = \frac{1}{2}mv^2 \Rightarrow v = \sqrt{3Rg + \frac{kR^2}{m}}
  5. So the answer is (b).
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Q163JEE Main 2024 · 30 JAN · SHIFT 1Easy

Conservation of Energy · Tracks, hills & pulleys

A particle is placed at the point AA of a frictionless track ABCABC as shown in figure. It is gently pushed towards right. The speed of the particle when it reaches the point B is:

(Take g=10 m/s2g = 10\text{ m/s}^2).

Figure

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Answer: (c)

  1. Track is frictionless, so loss of PE = gain of KE: v=2g Δhv = \sqrt{2g\,\Delta h}.
  2. Height drop from A (1 m) to B (0.5 m): Δh=0.5 m\Delta h = 0.5\text{ m}.
  3. v=2×10×0.5=10 m/sv = \sqrt{2 \times 10 \times 0.5} = \sqrt{10}\text{ m/s}
  4. So the answer is (c) 10 m/s\sqrt{10}\text{ m/s}.
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Q164MHT CET 2024 · 3 MAY · SHIFT 1Medium

Conservation of Energy · Projectile: KE & PE at the top

A ball ' AA ' is projected vertically upwards with certain initial speed. Another ball 'B' of same mass is projected at an angle of 30∘30^\circ with vertical with the same initial speed. At the highest point, the ratio of potential energy of ball A to that of ball B will be

(sin⁡90∘=1,sin⁡60∘=cos⁡30∘=32,sin⁡30∘=cos⁡60∘=12)\left(\sin 90^\circ = 1, \sin 60^\circ = \cos 30^\circ = \frac{\sqrt{3}}{2}, \sin 30^\circ = \cos 60^\circ = \frac{1}{2}\right)

Show answer and solution

Answer: (a)

  1. PE at the top =mgH= mgH with H=uy22gH = \frac{u_y^2}{2g}, so U∝uy2U \propto u_y^2.
  2. Ball A: uy=uu_y = u. Ball B (at 30∘30^\circ with vertical): uy=ucos⁡30∘=32uu_y = u\cos 30^\circ = \frac{\sqrt{3}}{2}u.
  3. UAUB=u234u2=43\frac{U_A}{U_B} = \frac{u^2}{\frac{3}{4}u^2} = \frac{4}{3}
  4. So the answer is (a) 4:34 : 3.
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Q165JEE Main 2024 · 4 APR · SHIFT 2Medium

Conservation of Energy · Tracks, hills & pulleys

A body of m kgm\text{ kg} slides from rest along the curve of vertical circle from point AA to BB in frictionless path. The velocity of the body at BB is:

Figure

(given, R=14 m,g=10 m/s2R = 14\text{ m}, g = 10\text{ m/s}^2 and 2=1.4\sqrt{2} = 1.4)

Show answer and solution

Answer: (d)

  1. A is Rsin⁡45∘R\sin 45^\circ above the centre and B is RR below it, so the drop is h=R(1+12)h = R\left(1 + \frac{1}{\sqrt{2}}\right).
  2. h=14(1+0.7)=23.8 mh = 14(1 + 0.7) = 23.8\text{ m}
  3. v=2gh=2×10×23.8=476≈21.8 m/sv = \sqrt{2gh} = \sqrt{2 \times 10 \times 23.8} = \sqrt{476} \approx 21.8\text{ m/s}
  4. So the answer is (d) 21.9 m/s.
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Q166MHT CET 2024 · 16 MAY · SHIFT 1Medium

Conservation of Energy · Pendulum & swing

A simple pendulum of length L has mass m and it oscillates freely with amplitude A. At extreme position, its potential energy is ( g=\text{g} = acceleration due to gravity)

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Answer: (d)

  1. Height at the extreme: h=L(1−cos⁡θ)≈Lθ22h = L(1 - \cos\theta) \approx \frac{L\theta^2}{2} for small θ\theta.
  2. Amplitude A=Lθ⇒θ=ALA = L\theta \Rightarrow \theta = \frac{A}{L}, so h=A22Lh = \frac{A^2}{2L}.
  3. U=mgh=mgA22LU = mgh = \frac{mgA^2}{2L}
  4. So the answer is (d) mgA22L\frac{mgA^2}{2L}.
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Q167MHT CET 2024 · 15 MAY · SHIFT 2Medium

Conservation of Energy · Energy conversion & heat

If the work done in blowing a soap bubble of volume ' V ' is ' W ', then the work done in blowing a soap bubble of volume ' 2 V ' will be

Show answer and solution

Answer: (d)

  1. Work in blowing a bubble W=T×2×4πr2∝r2W = T \times 2 \times 4\pi r^2 \propto r^2.
  2. V∝r3⇒r∝V1/3V \propto r^3 \Rightarrow r \propto V^{1/3}, so W∝V2/3W \propto V^{2/3}.
  3. W′=W×22/3=W(4)1/3W' = W \times 2^{2/3} = W(4)^{1/3}
  4. So the answer is (d) W(4)13W(4)^{\frac{1}{3}}.
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Q168MHT CET 2024 · 10 MAY · SHIFT 1Medium

Conservation of Energy · Energy conversion & heat

A lead bullet moving with velocity ' V ' strikes a wall and stops. If 75%75\% of its energy is converted into heat, then the increase in temperature is ( s=\text{s} = specific heat of lead, J=\text{J} = mechanical equivalent of heat)

Show answer and solution

Answer: (a)

  1. Heat produced =75%= 75\% of KE: Q=34⋅12mV2Q = \frac{3}{4} \cdot \frac{1}{2}mV^2 (in joule).
  2. In calories Q=3mV28JQ = \frac{3mV^2}{8J}, and Q=ms ΔTQ = ms\,\Delta T.
  3. ms ΔT=3mV28J⇒ΔT=3V28Jsms\,\Delta T = \frac{3mV^2}{8J} \Rightarrow \Delta T = \frac{3V^2}{8Js}
  4. So the answer is (a).
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Q169MHT CET 2024 · 4 MAY · SHIFT 2Difficult

Conservation of Energy · Chain, cable & carpet

A carpet of mass ' MM ' made of a material is rolled along its length in the form of a cylinder of radius ' RR ' and kept above the rough floor. If the carpet is unrolled without sliding to a radius ' R/2R/2 '. The change in potential energy is ( g=g = acceleration due to gravity)

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Answer: (b)

  1. Mass ∝r2\propto r^2, so the roll of radius R/2R/2 has mass M4\frac{M}{4}; the unrolled 3M4\frac{3M}{4} lies flat on the floor (PE ≈0\approx 0).
  2. Initial PE =MgR= MgR (centre at height RR).
  3. Final PE =M4gR2=MgR8= \frac{M}{4}g\frac{R}{2} = \frac{MgR}{8}
  4. Change =MgR−MgR8=78MgR= MgR - \frac{MgR}{8} = \frac{7}{8}MgR (decrease). So the answer is (b).
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Q170JEE Main 2023 · 29 JAN · SHIFT 1Easy

Conservation of Energy · Projectile: KE & PE at the top

A stone is projected at angle 30∘30^\circ to the horizontal. The ratio of kinetic energy of the stone at point of projection to its kinetic energy at the highest point of flight will be -

Show answer and solution

Answer: (c)

  1. At the top, Ktop=Kcos⁡2θK_{top} = K\cos^2\theta, so KKtop=1cos⁡230∘\frac{K}{K_{top}} = \frac{1}{\cos^2 30^\circ}.
  2. cos⁡230∘=34⇒KKtop=43\cos^2 30^\circ = \frac{3}{4} \Rightarrow \frac{K}{K_{top}} = \frac{4}{3}
  3. So the answer is (c) 4:34:3.
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Q171JEE Main 2023 · 29 JAN · SHIFT 1Medium

Conservation of Energy · Free fall: K and U at a height

A 0.4 kg mass takes 8s to reach ground when dropped from a certain height 'P' above surface of earth. The loss of potential energy in the last second of fall is __________ J.

(Take g = 10 m/s2{}^{2})

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 300

  1. Distance fallen in the nnth second from rest: sn=g2(2n−1)s_n = \frac{g}{2}(2n - 1).
  2. s8=5×15=75 ms_8 = 5 \times 15 = 75\text{ m}
  3. Loss of PE =mgs8=0.4×10×75= mgs_8 = 0.4 \times 10 \times 75
  4. =300 J= 300\text{ J}
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Q172MHT CET 2023 · 9 MAY · SHIFT 1Medium

Conservation of Energy · Projectile: KE & PE at the top

A stone is projected vertically upwards with speed 'vv'. Another stone of same mass is projected at an angle of 60∘60^\circ with the vertical with the same speed 'vv'. The ratio of their potential energies at the highest points of their journey is [sin⁡30∘=cos⁡60∘=0.5,cos⁡30∘=sin⁡60∘=32]\left[\sin 30^\circ = \cos 60^\circ = 0.5, \cos 30^\circ = \sin 60^\circ = \frac{\sqrt{3}}{2}\right]

Show answer and solution

Answer: (a)

  1. PE at the top =mgH= mgH with H=uy22gH = \frac{u_y^2}{2g}, so U∝uy2U \propto u_y^2.
  2. Vertical stone: uy=vu_y = v. Other stone (at 60∘60^\circ with vertical): uy=vcos⁡60∘=v2u_y = v\cos 60^\circ = \frac{v}{2}.
  3. U1U2=v2v2/4=4\frac{U_1}{U_2} = \frac{v^2}{v^2/4} = 4
  4. So the answer is (a) 4:14 : 1.
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Q173JEE Main 2023 · 10 APR · SHIFT 1Medium

Conservation of Energy · Friction: energy lost

A closed circular tube of average radius 15 cm, whose inner walls are rough, is kept in vertical plane. A block of mass 1 kg just fits inside the tube. The speed of block is 22 m/s, when it is introduced at the top of tube. After completing five oscillations, the block stops at the bottom region of tube. The work done by the tube on the block is __________ J. (Given g = 10 m/s2{}^{2}).

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 245

  1. Work-energy theorem: Wtube+Wgravity=ΔKW_{tube} + W_{gravity} = \Delta K.
  2. Block goes from top to bottom: Wgravity=mg(2r)=1×10×0.3=3 JW_{gravity} = mg(2r) = 1 \times 10 \times 0.3 = 3\text{ J}.
  3. ΔK=0−12×1×222=−242 J\Delta K = 0 - \frac{1}{2} \times 1 \times 22^2 = -242\text{ J}
  4. Wtube=−242−3=−245 JW_{tube} = -242 - 3 = -245\text{ J}, i.e. magnitude 245 J245\text{ J} (negative work by friction).
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Q174JEE Main 2022 · 29 JUL · SHIFT 1Easy

Conservation of Energy · Projectile: KE & PE at the top

A ball is projected with kinetic energy E, at an angle of 60∘60^\circ to the horizontal. The kinetic energy of this ball at the highest point of its flight will become:

Show answer and solution

Answer: (c)

  1. At the top only the horizontal velocity ucos⁡θu\cos\theta remains, so Ktop=Ecos⁡2θK_{top} = E\cos^2\theta.
  2. Ktop=Ecos⁡260∘=E×14K_{top} = E\cos^2 60^\circ = E \times \frac{1}{4}
  3. So the answer is (c) E4\frac{E}{4}.
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Q175JEE Main 2022 · 29 JUN · SHIFT 2Easy

Conservation of Energy · Tracks, hills & pulleys

In the given figure, the block of mass m is dropped from the point 'A'. The expression for kinetic energy of block when it reaches point 'B' is

Figure

Show answer and solution

Answer: (d)

  1. Block is dropped from rest at A, so KE at B = PE lost.
  2. The block falls through the distance AB=y0AB = y_0.
  3. KB=mgy0K_B = mg y_0
  4. So the answer is (d) mgy0mgy_0.
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Q176JEE Main 2021 · 18 MAR · SHIFT 1Easy

Conservation of Energy · Tracks, hills & pulleys

As shown in the figure, a particle of mass 10 kg is placed at a point A. When the particle is slightly displaced to its right, it starts moving and reaches the point B. The speed of the particle at B is x m/s. (Take g = 10 m/s2)

The value of 'x' to the nearest integer is __________.

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 10

  1. No friction, so 12mv2=mg Δh\frac{1}{2}mv^2 = mg\,\Delta h (mass cancels).
  2. Height drop from A (10 m) to B (5 m): Δh=5 m\Delta h = 5\text{ m}.
  3. v=2×10×5=100=10 m/sv = \sqrt{2 \times 10 \times 5} = \sqrt{100} = 10\text{ m/s}
  4. So x=10x = 10.
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Q177NEET 2021Medium

Conservation of Energy · Free fall: K and U at a height

A particle is released from height S from the surface of the Earth. At a certain height its kinetic energy is three times its potential energy. The height from the surface of earth and the speed of the particle at that instant are respectively -

Show answer and solution

Answer: (a)

  1. Total energy mgS=K+UmgS = K + U and K=3UK = 3U, so 4U=mgS4U = mgS.
  2. mgh=mgS4⇒h=S4mgh = \frac{mgS}{4} \Rightarrow h = \frac{S}{4}
  3. Fall distance =3S4= \frac{3S}{4}: v=2g⋅3S4=3gS2v = \sqrt{2g \cdot \frac{3S}{4}} = \sqrt{\frac{3gS}{2}}
  4. So the answer is (a) S4,3gS2\frac{S}{4}, \sqrt{\frac{3gS}{2}}.
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Q178MHT CET 2021 · 24 SEP · SHIFT 1Medium

Conservation of Energy · Projectile: KE & PE at the top

A stone is projected vertically upwards with velocity 'V'. Another stone of same mass is projected at an angle of 60∘60^\circ with the vertical with the same speed (V)(\text{V}). The ratio of their potential energies at the highest points of their journey, is

[sin⁡30∘=cos⁡60∘=0.5,cos⁡30∘=sin⁡60∘=32]\left[\sin 30^\circ = \cos 60^\circ = 0.5, \cos 30^\circ = \sin 60^\circ = \frac{\sqrt{3}}{2}\right]

Show answer and solution

Answer: (b)

  1. PE at the top =mgH= mgH with H=uy22gH = \frac{u_y^2}{2g}, so U∝uy2U \propto u_y^2.
  2. Vertical stone: uy=Vu_y = V. Other stone (at 60∘60^\circ with vertical): uy=Vcos⁡60∘=V2u_y = V\cos 60^\circ = \frac{V}{2}.
  3. U1U2=V2V2/4=4\frac{U_1}{U_2} = \frac{V^2}{V^2/4} = 4
  4. So the answer is (b) 4:14 : 1.
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Q179JEE Main 2021 · 25 JUL · SHIFT 1Medium

Conservation of Energy · Pendulum & swing

A pendulum bob has a speed of 3 m/s at its lowest position. The pendulum is 50 cm long. The speed of bob, when the length makes an angle of 60 ∘{}^\circ to the vertical will be (g = 10 m/s2) ____________ m/s.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 2

  1. Rise of bob at 60∘60^\circ: h=L(1−cos⁡60∘)=0.5×0.5=0.25 mh = L(1 - \cos 60^\circ) = 0.5 \times 0.5 = 0.25\text{ m}.
  2. v2=u2−2gh=9−2×10×0.25v^2 = u^2 - 2gh = 9 - 2 \times 10 \times 0.25
  3. v2=4v^2 = 4
  4. v=2 m/sv = 2\text{ m/s}
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Q180JEE Main 2021 · 26 AUG · SHIFT 1Medium

Conservation of Energy · Chain, cable & carpet

A uniform chain of length 3 meter and mass 3 kg overhangs a smooth table with 2 meter lying on the table. If k is the kinetic energy of the chain in joule as it completely slips off the table, then the value of k is .................. (Take g = 10 m/s2)

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 40

  1. Smooth table, so KE gained = loss of PE. Take the table top as zero; mass per metre =1 kg/m= 1\text{ kg/m}.
  2. Initially 1 m (1 kg) hangs, CM 0.5 m below: Ui=−1×10×0.5=−5 JU_i = -1 \times 10 \times 0.5 = -5\text{ J}.
  3. Finally all 3 m (3 kg) hangs, CM 1.5 m below: Uf=−3×10×1.5=−45 JU_f = -3 \times 10 \times 1.5 = -45\text{ J}.
  4. k=Ui−Uf=−5+45=40 Jk = U_i - U_f = -5 + 45 = 40\text{ J}
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Q181JEE Main 2020 · 7 JAN · SHIFT 1Medium

Conservation of Energy · Tracks, hills & pulleys

A particle (m = 1 kg) slides down a frictionless track (AOC) starting from rest at a point A (height 2 m). After reaching C, the particle continues to move freely in air as a projectile. When it reaches its highest point P (height 1 m), the kinetic energy of the particle (in J) is:

(Figure drawn is schematic and not to scale; take g = 10 ms-2)

Figure

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 10

  1. No friction or air drag, so total mechanical energy is conserved.
  2. At A (rest, 2 m): E=mghA=1×10×2=20 JE = mgh_A = 1 \times 10 \times 2 = 20\text{ J}.
  3. At P (1 m): UP=1×10×1=10 JU_P = 1 \times 10 \times 1 = 10\text{ J}
  4. KP=20−10=10 JK_P = 20 - 10 = 10\text{ J}
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Q182JEE Main 2020 · 2 SEP · SHIFT 1Medium

Conservation of Energy · Friction: energy lost

Figure

A small block starts slipping down from a point B on an inclined plane AB, which is making an angle θ\theta with the horizontal section BC is smooth and the remaining section CA is rough with a coefficient of friction μ\mu. It is found that the block comes to rest as it reaches the bottom (point A) of the inclined plane. If BC = 2AC, the coefficient of friction is given by μ\mu = ktan θ\theta. The value of k is _________.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 3

  1. Let AC=lAC = l; then BC=2lBC = 2l and AB=3lAB = 3l.
  2. Starts and ends at rest: mg(3l)sin⁡θ=μmgcos⁡θ⋅lmg(3l)\sin\theta = \mu mg\cos\theta \cdot l
  3. μ=3tan⁡θ\mu = 3\tan\theta
  4. So k=3k = 3.
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Q183JEE Main 2020 · 3 SEP · SHIFT 2Difficult

Conservation of Energy · Friction: energy lost

A block starts moving up an inclined plane of inclination 30° with an initial velocity of v0. It comes back to its initial position with velocity v02\frac{v_0}{2}. The value of the coefficient of kinetic friction between the block and the inclined plane is close to I1000\frac{I}{1000}. The nearest integer to I is____.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 346

  1. Up a distance dd: 12mv02=mgd(sin⁡30∘+μcos⁡30∘)\frac{1}{2}mv_0^2 = mgd(\sin 30^\circ + \mu\cos 30^\circ).
  2. Down: 12mv024=mgd(sin⁡30∘−μcos⁡30∘)\frac{1}{2}m\frac{v_0^2}{4} = mgd(\sin 30^\circ - \mu\cos 30^\circ).
  3. Divide: 4=sin⁡30∘+μcos⁡30∘sin⁡30∘−μcos⁡30∘⇒μ=35tan⁡30∘4 = \frac{\sin 30^\circ + \mu\cos 30^\circ}{\sin 30^\circ - \mu\cos 30^\circ} \Rightarrow \mu = \frac{3}{5}\tan 30^\circ
  4. μ=0.63=0.346=3461000\mu = \frac{0.6}{\sqrt{3}} = 0.346 = \frac{346}{1000}, so I=346I = 346.
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Q184JEE Main 2019 · 9 APR · SHIFT 1Easy

Conservation of Energy · Chain, cable & carpet

A uniform cable of mass 'M' and length 'L' is placed on a horizontal surface such that its (1/n)th part is hanging below the edge of the surface. To lift the hanging part of the cable upto the surface, the work done should be:

Show answer and solution

Answer: (c)

  1. Hanging part: mass Mn\frac{M}{n}, length Ln\frac{L}{n}, centre of mass L2n\frac{L}{2n} below the edge.
  2. Work = rise in PE of this part: W=Mng⋅L2nW = \frac{M}{n} g \cdot \frac{L}{2n}
  3. W=MgL2n2W = \frac{MgL}{2n^2}
  4. So the answer is (c) MgL2n2\frac{MgL}{2n^2}.
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Q185JEE Main 2016Medium

Conservation of Energy · Energy conversion & heat

A person trying to lose weight by burning fat lifts a mass of 10 kg10\text{ kg} upto a height of 1 m 10001\text{ m}\ 1000 times. Assume that the potential energy lost each time he lowers the mass is dissipated. How much fat will he use up considering the work done only when the weight is lifted up? Fat supplies 3.8×107 J3.8 \times 10^{7}\text{ J} of energy per kg\text{kg} which is converted to mechanical energy with a 20%20\% efficiency rate. Take g=9.8 ms−2g = 9.8\text{ ms}^{-2}:

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Answer: (b)

  1. Work in lifting: W=1000 mgh=1000×10×9.8×1=9.8×104 JW = 1000\,mgh = 1000 \times 10 \times 9.8 \times 1 = 9.8 \times 10^4\text{ J}.
  2. Only 20% of fat energy becomes work: energy from fat =9.8×1040.2=4.9×105 J= \frac{9.8 \times 10^4}{0.2} = 4.9 \times 10^5\text{ J}.
  3. Fat used =4.9×1053.8×107=1.289×10−2 kg= \frac{4.9 \times 10^5}{3.8 \times 10^7} = 1.289 \times 10^{-2}\text{ kg}
  4. So the answer is (b) 12.89×10−3 kg12.89 \times 10^{-3}\text{ kg}.
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Q186JEE Main 2016Difficult

Conservation of Energy · Friction: energy lost

A point particle of mass m,m, moves along the uniformly rough track PQRPQR as shown in the figure. The coefficient of friction, between the particle and the rough track equals μ.\mu. The particle is released, from rest from the point PP and it comes to rest at point R.R. The energies, lost by the ball, over the parts, PQPQ and QRQR, of the track, are equal to each other, and no energy is lost when particle changes direction from PQPQ to QRQR.

The value of the coefficient of friction μ\mu and the distance x (=QR),x\ (= QR), are, respectively close to:

Figure

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Answer: (a)

  1. Length PQ=hsin⁡30∘=4 mPQ = \frac{h}{\sin 30^\circ} = 4\text{ m}. Loss on PQ =μmgcos⁡30∘×4=23μmg= \mu mg\cos 30^\circ \times 4 = 2\sqrt{3}\mu mg.
  2. Loss on QR =μmgx= \mu mg x. Equal losses ⇒x=23≈3.5 m\Rightarrow x = 2\sqrt{3} \approx 3.5\text{ m}.
  3. Total loss = mghmgh: 2×23μmg=2mg⇒μ=123≈0.292 \times 2\sqrt{3}\mu mg = 2mg \Rightarrow \mu = \frac{1}{2\sqrt{3}} \approx 0.29
  4. So the answer is (a) 0.290.29 and 3.5 m3.5\text{ m}.
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Q187JEE Main 2014 · 11 APR · SHIFT 1Medium

Conservation of Energy · Friction: energy lost

A small ball of mass m starts at a point A with speed vvo and moves along a frictionless track AB as shown. The track BC has coefficient of friction μ\mu. The ball comes to stop at C after travelling a distance L which is:

Figure

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Answer: (b)

  1. From A to C all mechanical energy is used up against friction on BC only.
  2. mgh+12mv02=μmgLmgh + \frac{1}{2}mv_0^2 = \mu mgL
  3. L=hμ+v022μgL = \frac{h}{\mu} + \frac{v_0^2}{2\mu g}
  4. So the answer is (b).
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Q188JEE Main 2014 · 11 APR · SHIFT 1Medium

Conservation of Energy · Energy conversion & heat

The average mass of rain drops is 3.0 ×\times 10−-5 kg and their average terminal velocity is 9 m/s. Calculate the energy transferred by rain to each square meter of the surface at a place which receives 100 cm of rain in a year.

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Answer: (b)

  1. 100 cm of rain on 1 m21\text{ m}^2: volume =1 m3= 1\text{ m}^3, mass =1000 kg= 1000\text{ kg}.
  2. All drops reach the ground at terminal speed 9 m/s9\text{ m/s}; drop size does not matter.
  3. E=12Mv2=12×1000×81E = \frac{1}{2}Mv^2 = \frac{1}{2} \times 1000 \times 81
  4. E=4.05×104 JE = 4.05 \times 10^4\text{ J}. So the answer is (b).
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Q189JEE Main 2007 · AIEEEEasy

Conservation of Energy · Projectile: KE & PE at the top

A particle is projected at 60∘60^\circ to the horizontal with a kinetic energy K. The kinetic energy at the highest point is

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Answer: (d)

  1. At the highest point the speed is ucos⁡θu\cos\theta, so Ktop=Kcos⁡2θK_{top} = K\cos^2\theta.
  2. Ktop=Kcos⁡260∘=K4K_{top} = K\cos^2 60^\circ = \frac{K}{4}
  3. So the answer is (d) K/4K/4.
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Q190JEE Main 2006 · AIEEEMedium

Conservation of Energy · Pendulum & swing

A mass of M kgM\text{ kg} is suspended by a weightless string. The horizontal force that is required to displace it until the string makes an angle of 45∘45^\circ with the initial vertical direction is

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Answer: (d)

  1. A constant horizontal force FF takes the mass from rest at the bottom to rest at 45∘45^\circ: work by FF = gain in PE.
  2. Horizontal shift =Lsin⁡45∘= L\sin 45^\circ, rise =L(1−cos⁡45∘)= L(1 - \cos 45^\circ).
  3. F⋅L2=MgL(1−12)F \cdot \frac{L}{\sqrt{2}} = MgL\left(1 - \frac{1}{\sqrt{2}}\right)
  4. F=Mg(2−1)F = Mg(\sqrt{2} - 1). So the answer is (d).
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Q191JEE Main 2005 · AIEEEEasy

Conservation of Energy · Tracks, hills & pulleys

A spherical ball of mass 20 kg20\text{ kg} is stationary at the top of a hill of height 100 m100\text{ m}. It rolls down a smooth surface to the ground, then climbs up another hill of height 30 m30\text{ m} and finally rolls down to a horizontal base at a height of 20 m20\text{ m} above the ground. The velocity attained by the ball is

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Answer: (b)

  1. Smooth surface: only the net height drop matters, v=2g Δhv = \sqrt{2g\,\Delta h}.
  2. Start at 100 m, end on the base at 20 m: Δh=80 m\Delta h = 80\text{ m} (the 30 m hill is lower than 100 m, so it is crossed).
  3. v=2×10×80=1600=40 m/sv = \sqrt{2 \times 10 \times 80} = \sqrt{1600} = 40\text{ m/s}
  4. So the answer is (b) 40 m/s40\text{ m/s}.
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Q192JEE Main 2005 · AIEEEMedium

Conservation of Energy · Friction: energy lost

The upper half of an inclined plane with inclination ϕ\phi is perfectly smooth while the lower half is rough. A body starting from rest at the top will again come to rest at the bottom if the coefficient of friction for the lower half is given by

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Answer: (d)

  1. Let the full length be ll. Body starts and ends at rest, so loss of PE = work against friction on the lower half.
  2. mg lsin⁡ϕ=μmgcos⁡ϕ⋅l2mg\,l\sin\phi = \mu mg\cos\phi \cdot \frac{l}{2}
  3. μ=2sin⁡ϕcos⁡ϕ=2tan⁡ϕ\mu = \frac{2\sin\phi}{\cos\phi} = 2\tan\phi
  4. So the answer is (d) 2tan⁡ϕ2\tan\phi.
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Q193NEET 2004 · AIPMTEasy

Conservation of Energy · Free fall: K and U at a height

A ball of mass 2 kg and another of mass 4 kg are dropped together from a 60 feet tall building. After a fall of 30 feet each towards earth, their respective kinetic energies will be in the ratio of

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Answer: (c)

  1. After falling the same height hh, KE=mgh∝mKE = mgh \propto m.
  2. K1K2=24\frac{K_1}{K_2} = \frac{2}{4}
  3. So the answer is (c) 1:21:2.
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Q194JEE Main 2004 · AIEEEEasy

Conservation of Energy · Chain, cable & carpet

A uniform chain of length 2 m2\text{ m} is kept on a table such that a length of 60 cm60\text{ cm} hangs freely from the edge of the table. The total mass of the chain is 4 kg.4\text{ kg}. What is the work done in pulling the entire chain on the table?

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Answer: (b)

  1. Mass of hanging part: m=42×0.6=1.2 kgm = \frac{4}{2} \times 0.6 = 1.2\text{ kg}; its centre of mass is 0.3 m0.3\text{ m} below the edge.
  2. W=mgl2=1.2×10×0.3W = mg\frac{l}{2} = 1.2 \times 10 \times 0.3
  3. W=3.6 JW = 3.6\text{ J}
  4. So the answer is (b) 3.6 J3.6\text{ J}.
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Q195JEE Main 2002 · AIEEEEasy

Conservation of Energy · Projectile: KE & PE at the top

A ball whose kinetic energy is E, is projected at an angle of 45∘45^\circ to the horizontal. The kinetic energy of the ball at the highest point of its flight will be

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Answer: (c)

  1. At the highest point the speed is ucos⁡θu\cos\theta, so Ktop=Ecos⁡2θK_{top} = E\cos^2\theta.
  2. Ktop=Ecos⁡245∘=E2K_{top} = E\cos^2 45^\circ = \frac{E}{2}
  3. So the answer is (c) E2\frac{E}{2}.
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Q196NEET 2001 · AIPMTEasy

Conservation of Energy · Projectile: KE & PE at the top

A particle is projected making an angle of 45° with horizontal having kinetic energy K. The kinetic energy at highest point will be

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Answer: (b)

  1. At the top, speed =vcos⁡45∘= v\cos 45^\circ, so KE=Kcos⁡245∘KE = K\cos^2 45^\circ.
  2. KE=K×12KE = K \times \frac{1}{2}
  3. So the answer is (b) K2\frac{K}{2}.
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Q197NEET 2001 · AIPMTEasy

Conservation of Energy · Pendulum & swing

A child is sitting on a swing. Its minimum and maximum heights from the ground 0.75 m and 2 m respectively, its maximum speed will be

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Answer: (b)

  1. Maximum speed at the lowest point: 12mv2=mg(hmax−hmin)\frac{1}{2}mv^2 = mg(h_{max} - h_{min}).
  2. Δh=2−0.75=1.25 m\Delta h = 2 - 0.75 = 1.25\text{ m}
  3. v=2×10×1.25=25=5 m/sv = \sqrt{2 \times 10 \times 1.25} = \sqrt{25} = 5\text{ m/s}
  4. So the answer is (b) 5 m/s.
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Q198NEET 1997 · AIPMTEasy

Conservation of Energy · Projectile: KE & PE at the top

A particle is projected making an angle of 45∘45^\circ with horizontal having kinetic energy KK. The kinetic energy at highest point will be

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Answer: (b)

  1. At the top, speed =vcos⁡45∘= v\cos 45^\circ, so KE=Kcos⁡245∘KE = K\cos^2 45^\circ.
  2. KE=K×12KE = K \times \frac{1}{2}
  3. So the answer is (b) K2\frac{K}{2}.
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Q199NEET 2026Easy

Power · Average power: P = W/t

The power of a crane, which lifts a mass of 1000 kg to a height of 20 m in 10 s is: (g=9.8 m/s2)\left(g = 9.8\text{ m/s}^2\right)

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Answer: (c)

  1. Power P=Wt=mghtP = \dfrac{W}{t} = \dfrac{mgh}{t}.
  2. P=1000×9.8×2010=19600 WP = \dfrac{1000 \times 9.8 \times 20}{10} = 19600\text{ W}
  3. So the answer is (c) 19.6 kW19.6\text{ kW}.
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Q200MHT CET 2026 · 19 MAY · SHIFT 2Easy

Power · Constant power: how v and s grow with t

A body is moved along a straight line by a machine delivering constant power. The distance moved by the body in time tt is proportional to

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Answer: (c)

  1. P=Fv=mvdvdtP = Fv = mv\dfrac{dv}{dt} = constant ⇒∫v dv=∫Pmdt\Rightarrow \int v\,dv = \int \dfrac{P}{m}dt.
  2. v22=Pmt⇒v∝t1/2\dfrac{v^2}{2} = \dfrac{P}{m}t \Rightarrow v \propto t^{1/2}
  3. s=∫v dt∝t3/2s = \int v\,dt \propto t^{3/2}
  4. So the answer is (c) t3/2t^{3/2}.
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Q201MHT CET 2026 · 16 APR · SHIFT 2Medium

Power · Power from a force F(t)

A body of mass 1kg begins to move under the action of a time dependent force F⃗=(ti^+3t2j^)\vec{F} = (t\hat{i} + 3t^2\hat{j}) N where i^\hat{i} and j^\hat{j} are the unit vectors along x and y axis. The power developed by the above force at time t=2t = 2 s will be (in watt)

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Answer: (a)

  1. m=1m = 1 kg, so a⃗=ti^+3t2j^\vec{a} = t\hat{i} + 3t^2\hat{j}; from rest v⃗=t22i^+t3j^\vec{v} = \dfrac{t^2}{2}\hat{i} + t^3\hat{j}.
  2. At t=2t = 2: F⃗=2i^+12j^\vec{F} = 2\hat{i} + 12\hat{j}, v⃗=2i^+8j^\vec{v} = 2\hat{i} + 8\hat{j}.
  3. P=F⃗⋅v⃗=4+96=100 WP = \vec{F} \cdot \vec{v} = 4 + 96 = 100\text{ W}
  4. So the answer is (a) 100.
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Q202JEE Main 2026 · 4 APR · SHIFT 1Medium

Power · Power from a force F(t)

A body of mass 2 kg begins to move under the influence of time dependent force F⃗=(2ti^+6t2j^) N\vec{F} = \left(2t\hat{i} + 6t^2\hat{j}\right)\text{ N}, where i^\hat{i} and j^\hat{j} are unit vectors along xx and y -axis respectively. The power produced by the force at t=2 st = 2\text{ s} is ______ W.

Numerical answer type. Work it out, then open the answer.

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Answer: 200

  1. a⃗=F⃗2=ti^+3t2j^\vec{a} = \dfrac{\vec{F}}{2} = t\hat{i} + 3t^2\hat{j}; from rest v⃗=t22i^+t3j^\vec{v} = \dfrac{t^2}{2}\hat{i} + t^3\hat{j}.
  2. At t=2t = 2: F⃗=4i^+24j^\vec{F} = 4\hat{i} + 24\hat{j}, v⃗=2i^+8j^\vec{v} = 2\hat{i} + 8\hat{j}.
  3. P=F⃗⋅v⃗=8+192=200 WP = \vec{F} \cdot \vec{v} = 8 + 192 = 200\text{ W}
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Q203MHT CET 2026 · 15 MAY · SHIFT 2Medium

Power · Constant power: how v and s grow with t

If the force acting on a body is inversely proportional to its speed, the kinetic energy of the body is

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Answer: (b)

  1. F∝1v⇒P=FvF \propto \frac{1}{v} \Rightarrow P = Fv is constant.
  2. By the work-energy theorem, K=∫P dt=PtK = \int P\,dt = Pt (starting from rest).
  3. So K∝tK \propto t.
  4. So the answer is (b) directly proportional to time.
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Q204MHT CET 2025 · 25 APR · SHIFT 2Easy

Power · Average power: P = W/t

A constant force F⃗=3i^−2j^−k^\vec{F} = 3\hat{i} - 2\hat{j} - \hat{k} newton has a displacement r⃗=2i^−3j^−3k^\vec{r} = 2\hat{i} - 3\hat{j} - 3\hat{k} metre in 2 second. The work done and the power are respectively

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Answer: (b)

  1. W=F⃗⋅r⃗=(3)(2)+(−2)(−3)+(−1)(−3)=6+6+3=15 JW = \vec{F} \cdot \vec{r} = (3)(2) + (-2)(-3) + (-1)(-3) = 6 + 6 + 3 = 15\text{ J}
  2. P=Wt=152=7.5 WP = \frac{W}{t} = \frac{15}{2} = 7.5\text{ W}
  3. So the answer is (b) 15 joule, 7.5 watt.
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Q205JEE Main 2025 · 28 JAN · SHIFT 2Medium

Power · Average power: P = W/t

A body of mass 4 kg is placed on a plane at a point PP having coordinates (3,4) m(3, 4)\text{ m}. Under the action of forceF⃗=(2i^+3j^) N\vec{F} = (2\hat{i} + 3\hat{j})\text{ N}, it moves to a new point Q having coordinates (6,10) m(6, 10)\text{ m} in 4 sec. The average power and instantaneous power at the end of 4 sec are in the ratio of:

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Answer: (d)

  1. Displacement s⃗=(6−3)i^+(10−4)j^=3i^+6j^\vec{s} = (6-3)\hat{i} + (10-4)\hat{j} = 3\hat{i} + 6\hat{j} m.
  2. W=F⃗⋅s⃗=6+18=24 JW = \vec{F} \cdot \vec{s} = 6 + 18 = 24\text{ J}, so Pavg=244=6 WP_{avg} = \dfrac{24}{4} = 6\text{ W}.
  3. a⃗=F⃗m=0.5i^+0.75j^\vec{a} = \dfrac{\vec{F}}{m} = 0.5\hat{i} + 0.75\hat{j}; from rest v⃗=a⃗t=2i^+3j^\vec{v} = \vec{a}t = 2\hat{i} + 3\hat{j} m/s at 4 s.
  4. Pinst=F⃗⋅v⃗=4+9=13 WP_{inst} = \vec{F} \cdot \vec{v} = 4 + 9 = 13\text{ W}
  5. So the answer is (d) 6:136:13.
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Q206MHT CET 2025 · 22 APR · SHIFT 1Medium

Power · Power from a force F(t)

A body of mass 1 kg begins to move under the action of a time dependent force F⃗=(ti^+2t2j^) N\vec{F} = \left(t\hat{i} + 2t^2\hat{j}\right)\text{ N}, where i^\hat{i} and j^\hat{j} are unit vectors along xx and yy axis. The power developed by above force at time t=3t = 3 second will be

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Answer: (a)

  1. m=1m = 1 kg, so a⃗=ti^+2t2j^\vec{a} = t\hat{i} + 2t^2\hat{j}; from rest v⃗=t22i^+2t33j^\vec{v} = \dfrac{t^2}{2}\hat{i} + \dfrac{2t^3}{3}\hat{j}.
  2. At t=3t = 3: F⃗=3i^+18j^\vec{F} = 3\hat{i} + 18\hat{j}, v⃗=4.5i^+18j^\vec{v} = 4.5\hat{i} + 18\hat{j}.
  3. P=F⃗⋅v⃗=13.5+324=337.5 WP = \vec{F} \cdot \vec{v} = 13.5 + 324 = 337.5\text{ W}
  4. So the answer is (a) 337.5 W.
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Q207JEE Main 2025 · 7 APR · SHIFT 1Medium

Power · Power from a force F(t)

An object of mass 1000 g experiences a time dependent force F⃗=(2ti^+3t2j^)N\vec{F} = \left(2t\hat{i} + 3t^2\hat{j}\right)N. The power generated by the force at time tt is:

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Answer: (c)

  1. m=1m = 1 kg, so a⃗=2ti^+3t2j^\vec{a} = 2t\hat{i} + 3t^2\hat{j}; from rest v⃗=t2i^+t3j^\vec{v} = t^2\hat{i} + t^3\hat{j}.
  2. P=F⃗⋅v⃗=2t3+3t5P = \vec{F} \cdot \vec{v} = 2t^3 + 3t^5
  3. So the answer is (c) (2t3+3t5)(2t^3 + 3t^5) W.
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Q208JEE Main 2025 · 29 JAN · SHIFT 2Difficult

Power · Conveyors, jets & wind

A sand dropper drops sand of mass m(t) on a conveyer belt at a rate proportional to the square root of speed (v) of the belt, i.e., dmdt∝v\frac{dm}{dt} \propto \sqrt{v}. If P is the power delivered to run the belt at constant speed then which of the following relationship is true?

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Answer: (d)

  1. Belt force F=vdmdtF = v\frac{dm}{dt}, so P=dmdtv2P = \frac{dm}{dt}v^2.
  2. dmdt∝v1/2⇒P∝v5/2\frac{dm}{dt} \propto v^{1/2} \Rightarrow P \propto v^{5/2}
  3. P2∝v5P^2 \propto v^5
  4. So the answer is (d).
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Q209MHT CET 2024 · 15 MAY · SHIFT 1Easy

Power · Average power: P = W/t

A body of mass 1 kg starts from rest and moves with uniform acceleration. In 2 seconds, its velocity is 10 m/s10\text{ m/s}. The power exerted on the body in one second is

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Answer: (b)

  1. a=102=5 m/s2a = \frac{10}{2} = 5\text{ m/s}^2, so F=ma=5 NF = ma = 5\text{ N}.
  2. At t=1 st = 1\text{ s}: v=at=5 m/sv = at = 5\text{ m/s}.
  3. P=Fv=5×5=25 WP = Fv = 5 \times 5 = 25\text{ W}
  4. So the answer is (b) 25 W.
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Q210NEET 2024Easy

Power · Instantaneous power: P = F·v

At any instant of time tt, the displacement of any particle is given by 2t−12t - 1 (SI\text{SI} unit) under the influence of force of 5 N5\text{ N}. The value of instantaneous power is (in SI\text{SI} unit):

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Answer: (a)

  1. x=2t−1⇒v=dxdt=2 m/sx = 2t - 1 \Rightarrow v = \dfrac{dx}{dt} = 2\text{ m/s}.
  2. P=Fv=5×2=10 WP = Fv = 5 \times 2 = 10\text{ W}
  3. So the answer is (a) 10.
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Q211JEE Main 2024 · 5 APR · SHIFT 2Easy

Power · Constant power: how v and s grow with t

A body is moving unidirectionally under the influence of a constant power source. Its displacement in time t is proportional to:

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Answer: (b)

  1. Constant power: mvdvdt=P⇒v2=2Pmtmv\dfrac{dv}{dt} = P \Rightarrow v^2 = \dfrac{2P}{m}t, so v∝t1/2v \propto t^{1/2}.
  2. s=∫v dt∝t3/2s = \int v\,dt \propto t^{3/2}
  3. So the answer is (b) t3/2t^{3/2}.
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Q212MHT CET 2024 · 16 MAY · SHIFT 1Medium

Power · Instantaneous power: P = F·v

The power (P)(P) is supplied to a rotating body having moment of inertia ' I ' and angular acceleration ' α\alpha '. Its instantaneous angular velocity ' ω\omega ' is

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Answer: (a)

  1. Rotational power P=τωP = \tau\omega with τ=Iα\tau = I\alpha.
  2. P=Iαω⇒ω=PIα=P(Iα)−1P = I\alpha\omega \Rightarrow \omega = \dfrac{P}{I\alpha} = P(I\alpha)^{-1}
  3. So the answer is (a).
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Q213JEE Main 2024 · 31 JAN · SHIFT 2Medium

Power · Power from a force F(t)

A body of mass 2 kg2\text{ kg} begins to move under the action of a time dependent force given by F⃗=(6ti^+6t2j^)N\vec{F} = \left(6t\hat{i} + 6t^2\hat{j}\right)N. The power developed by the force at the time tt is given by:

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Answer: (d)

  1. a⃗=F⃗2=3ti^+3t2j^\vec{a} = \dfrac{\vec{F}}{2} = 3t\hat{i} + 3t^2\hat{j}; from rest v⃗=3t22i^+t3j^\vec{v} = \dfrac{3t^2}{2}\hat{i} + t^3\hat{j}.
  2. P=F⃗⋅v⃗=(6t)(3t22)+(6t2)(t3)=9t3+6t5P = \vec{F} \cdot \vec{v} = (6t)\left(\dfrac{3t^2}{2}\right) + (6t^2)(t^3) = 9t^3 + 6t^5
  3. So the answer is (d) (9t3+6t5)(9t^3 + 6t^5) W.
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Q214NEET 2023Easy

Power · Instantaneous power: P = F·v

A particle moves with a velocity (5i^−3j^+6k^) m s−1(5\hat{i} - 3\hat{j} + 6\hat{k})\text{ m s}^{-1} horizontally under the action of constant force (10i^+10j^+20k^) N(10\hat{i} + 10\hat{j} + 20\hat{k})\text{ N}. The instantaneous power supplied to the particle is:

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Answer: (d)

  1. P=F⃗⋅v⃗P = \vec{F} \cdot \vec{v}.
  2. P=(10)(5)+(10)(−3)+(20)(6)=50−30+120=140 WP = (10)(5) + (10)(-3) + (20)(6) = 50 - 30 + 120 = 140\text{ W}
  3. So the answer is (d) 140 W140\text{ W}.
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Q215JEE Main 2023 · 13 APR · SHIFT 1Medium

Power · Average power: P = W/t

The ratio of powers of two motors is 3xx+1\frac{3\sqrt{x}}{\sqrt{x} + 1}, that are capable of raising 300 kg300\text{ kg} water in 5 minutes and 50 kg50\text{ kg} water in 2 minutes respectively from a well of 100 m100\text{ m} deep. The value of xx will be

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Answer: (a)

  1. P=mghtP = \dfrac{mgh}{t}.
  2. P1=300×10×100300=1000 WP_1 = \dfrac{300 \times 10 \times 100}{300} = 1000\text{ W}, P2=50×10×100120=12503 WP_2 = \dfrac{50 \times 10 \times 100}{120} = \dfrac{1250}{3}\text{ W}
  3. P1P2=125=3xx+1⇒15x=12x+12⇒x=4\dfrac{P_1}{P_2} = \dfrac{12}{5} = \dfrac{3\sqrt{x}}{\sqrt{x}+1} \Rightarrow 15\sqrt{x} = 12\sqrt{x} + 12 \Rightarrow \sqrt{x} = 4
  4. So the answer is (a) x=16x = 16.
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Q216JEE Main 2023 · 11 APR · SHIFT 2Medium

Power · Instantaneous power: P = F·v

A block of mass 5 kg5\text{ kg} starting from rest is pulled up on a smooth inclined plane making an angle of 30∘30^\circ with horizontal with an effective acceleration of 1 m s−21\text{ m s}^{-2}. The power delivered by the pulling force at t=10 st = 10\text{ s} from the start is ___________ W.

[use g=10 m s−2g = 10\text{ m s}^{-2} ]

(calculate the nearest integer value)

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 300

  1. Along the incline: F−mgsin⁡30∘=maF - mg\sin 30^\circ = ma.
  2. F=5×1+5×10×0.5=30 NF = 5 \times 1 + 5 \times 10 \times 0.5 = 30\text{ N}
  3. At t=10t = 10 s: v=at=10 m/sv = at = 10\text{ m/s}.
  4. P=Fv=30×10=300 WP = Fv = 30 \times 10 = 300\text{ W}
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Q217JEE Main 2023 · 24 JAN · SHIFT 2Medium

Power · Power from a force F(t)

A body of mass 1kg begins to move under the action of a time dependent force F⃗=(ti^+3t2j^)\vec{F} = \left(t\hat{i} + 3t^2\hat{j}\right) N, where i^\hat{i} and j^\hat{j} are the unit vectors along xx and yy axis. The power developed by above force, at the time t = 2s, will be ____________ W.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 100

  1. m=1m = 1 kg, so a⃗=ti^+3t2j^\vec{a} = t\hat{i} + 3t^2\hat{j}; from rest v⃗=t22i^+t3j^\vec{v} = \dfrac{t^2}{2}\hat{i} + t^3\hat{j}.
  2. At t=2t = 2: F⃗=2i^+12j^\vec{F} = 2\hat{i} + 12\hat{j}, v⃗=2i^+8j^\vec{v} = 2\hat{i} + 8\hat{j}.
  3. P=F⃗⋅v⃗=4+96=100 WP = \vec{F} \cdot \vec{v} = 4 + 96 = 100\text{ W}
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Q218JEE Main 2023 · 10 APR · SHIFT 2Medium

Power · Lifts & vehicles against friction

If the maximum load carried by an elevator is 1400 kg1400\text{ kg} ( 600 kg600\text{ kg} - Passengers + 800 kg\text{kg} - elevator), which is moving up with a uniform speed of 3 m s−13\text{ m s}^{-1} and the frictional force acting on it is 2000 N2000\text{ N}, then the maximum power used by the motor is __________ kW (g=10 m/s2)\text{kW}\ \left(g = 10\text{ m/s}^2\right)

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 48

  1. At uniform speed F=mg+f=1400×10+2000=16000 NF = mg + f = 1400 \times 10 + 2000 = 16000\text{ N}.
  2. P=Fv=16000×3=48000 WP = Fv = 16000 \times 3 = 48000\text{ W}
  3. So P=48 kWP = 48\text{ kW}.
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Q219JEE Main 2023 · 30 JAN · SHIFT 2Medium

Power · Constant power: how v and s grow with t

A body of mass 2 kg2\text{ kg} is initially at rest. It starts moving unidirectionally under the influence of a source of constant power P. Its displacement in 4 s4\text{ s} is 13α2P m\frac{1}{3}\alpha^2\sqrt{P}\text{ m}. The value of α\alpha will be ______.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 4

  1. For constant power from rest, x=(8P9m)1/2t3/2x = \left(\frac{8P}{9m}\right)^{1/2} t^{3/2}.
  2. With m=2m = 2 kg, t=4t = 4 s: x=4P9×8=163Px = \sqrt{\frac{4P}{9}} \times 8 = \frac{16}{3}\sqrt{P}
  3. Compare with 13α2P\frac{1}{3}\alpha^2\sqrt{P}: α2=16\alpha^2 = 16
  4. α=4\alpha = 4
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Q220NEET 2022 · PHASE 1Easy

Power · Average power: P = W/t

The energy that will be ideally radiated by a 100 kW transmitter in 1 hour is

Show answer and solution

Answer: (a)

  1. Energy E=PtE = Pt.
  2. E=(100×103)(3600)=3.6×108 JE = (100 \times 10^3)(3600) = 3.6 \times 10^8\text{ J}
  3. So the answer is (a) 36×107 J36 \times 10^7\text{ J}.
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Q221NEET 2022 · PHASE 1Medium

Power · Lifts & vehicles against friction

An electric lift with a maximum load of 2000 kg (lift + passengers) is moving up with a constant speed of 1.5 ms−1{}^{-1}. The frictional force opposing the motion is 3000 N. The minimum power delivered by the motor to the lift in watts is: (g = 10 ms−2{}^{-2})

Show answer and solution

Answer: (c)

  1. At constant speed, motor force F=mg+fF = mg + f.
  2. F=2000×10+3000=23000 NF = 2000 \times 10 + 3000 = 23000\text{ N}
  3. P=Fv=23000×1.5=34500 WP = Fv = 23000 \times 1.5 = 34500\text{ W}
  4. So the answer is (c) 34500.
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Q222JEE Main 2022 · 27 JUL · SHIFT 1Medium

Power · Conveyors, jets & wind

Sand is being dropped from a stationary dropper at a rate of 0.5 kg s−10.5\text{ kg s}^{-1} on a conveyor belt moving with a velocity of 5 m s−15\text{ m s}^{-1}. The power needed to keep the belt moving with the same velocity will be:

Show answer and solution

Answer: (d)

  1. Sand lands with zero horizontal speed, so the belt must supply force F=vdmdtF = v\frac{dm}{dt}.
  2. Power P=Fv=dmdtv2=0.5×52P = Fv = \frac{dm}{dt}v^2 = 0.5 \times 5^2
  3. P=12.5 WP = 12.5\text{ W}
  4. So the answer is (d) 12.5 W.
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Q223NEET 2021Easy

Power · Average power: P = W/t

Water falls from a height of 60m at the rate of 15 kg/s to operate a turbine. The losses due to frictional force are 10% of the input energy. How much power is generated by the turbine? (g = 10 m/s2)

Show answer and solution

Answer: (c)

  1. Input power =mtgh=15×10×60=9000 W= \dfrac{m}{t}gh = 15 \times 10 \times 60 = 9000\text{ W}.
  2. 10% is lost, so output =0.9×9000=8100 W= 0.9 \times 9000 = 8100\text{ W}.
  3. So the answer is (c) 8.1 kW8.1\text{ kW}.
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Q224JEE Main 2021 · 20 JUL · SHIFT 2Easy

Power · Constant power: how v and s grow with t

A body at rest is moved along a horizontal straight line by a machine delivering a constant power. The distance moved by the body in time 't' is proportional to:

Show answer and solution

Answer: (a)

  1. Constant power: mvdvdt=P⇒v2=2Pmtmv\dfrac{dv}{dt} = P \Rightarrow v^2 = \dfrac{2P}{m}t, so v∝t1/2v \propto t^{1/2}.
  2. s=∫0tv dt∝t3/2s = \int_0^t v\,dt \propto t^{3/2}
  3. So the answer is (a) t3/2t^{3/2}.
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Q225JEE Main 2021 · 18 MAR · SHIFT 1Easy

Power · Constant power: how v and s grow with t

A constant power delivering machine has towed a box, which was initially at rest, along a horizontal straight line. The distance moved by the box in time 't' is proportional to :-

Show answer and solution

Answer: (b)

  1. Constant power: mvdvdt=P⇒v∝t1/2mv\dfrac{dv}{dt} = P \Rightarrow v \propto t^{1/2}.
  2. s=∫0tv dt∝t3/2s = \int_0^t v\,dt \propto t^{3/2}
  3. So the answer is (b) t3/2t^{3/2}.
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Q226MHT CET 2021 · 22 SEP · SHIFT 1Medium

Power · Average power: P = W/t

A car of mass 'mm' moving with velocity 'uu' on a straight road in a straight line, doubles its velocity in time t. The power delivered by the engine of a car for doubling the velocity is

Show answer and solution

Answer: (a)

  1. Work done = change in KE (work-energy theorem).
  2. W=12m(2u)2−12mu2=32mu2W = \dfrac{1}{2}m(2u)^2 - \dfrac{1}{2}mu^2 = \dfrac{3}{2}mu^2
  3. P=Wt=3mu22tP = \dfrac{W}{t} = \dfrac{3mu^2}{2t}
  4. So the answer is (a).
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Q227JEE Main 2021 · 27 JUL · SHIFT 2Medium

Power · Constant power: how v and s grow with t

An automobile of mass 'm' accelerates starting from origin and initially at rest, while the engine supplies constant power P. The position is given as a function of time by:

Show answer and solution

Answer: (d)

  1. Pt=12mv2⇒v=2Pm t1/2Pt = \frac{1}{2}mv^2 \Rightarrow v = \sqrt{\frac{2P}{m}}\,t^{1/2}
  2. x=∫0tv dt=2Pm⋅23t3/2x = \int_0^t v\,dt = \sqrt{\frac{2P}{m}} \cdot \frac{2}{3}t^{3/2}
  3. x=(8P9m)1/2t3/2x = \left(\frac{8P}{9m}\right)^{1/2} t^{3/2}
  4. So the answer is (d).
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Q228JEE Main 2020 · 3 SEP · SHIFT 2Easy

Power · Constant power: how v and s grow with t

A particle is moving unidirectionally on a horizontal plane under the action of a constant power supplying energy source. The displacement (s) - time (t) graph that describes the motion of the particle is (graphs are drawn schematically and are not to scale):

Show answer and solution

Answer: (b)

tss ∝ t^(3/2)
  1. Constant power gives v∝t1/2v \propto t^{1/2}, so s∝t3/2s \propto t^{3/2}.
  2. s∝t3/2s \propto t^{3/2} starts at the origin, and its slope dsdt∝t1/2\dfrac{ds}{dt} \propto t^{1/2} keeps increasing.
  3. So the graph curves upward (concave up) from the origin.
  4. So the answer is (b).
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Q229JEE Main 2020 · 7 JAN · SHIFT 2Medium

Power · Lifts & vehicles against friction

An elevator in a building can carry a maximum of 10 persons, with the average mass of each person being 68 kg. The mass of the elevator itself is 920 kg and it moves with a constant speed of 3 m/s. The frictional force opposing the motion is 6000 N. If the elevator is moving up with its full capacity, the power delivered by the motor to the elevator (g = 10 m/s2) must be at least:

Show answer and solution

Answer: (d)

  1. Total mass =10×68+920=1600 kg= 10 \times 68 + 920 = 1600\text{ kg}.
  2. At constant speed F=mg+f=16000+6000=22000 NF = mg + f = 16000 + 6000 = 22000\text{ N}.
  3. P=Fv=22000×3=66000 WP = Fv = 22000 \times 3 = 66000\text{ W}
  4. So the answer is (d) 66000 W.
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Q230JEE Main 2020 · 7 JAN · SHIFT 1Medium

Power · Lifts & vehicles against friction

A 60 HP electric motor lifts an elevator having a maximum total load capacity of 2000 kg. If the frictional force on the elevator is 4000 N, the speed of the elevator at full load is close to: (1 HP = 746 W, g = 10 ms-2)

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Answer: (d)

  1. P=60×746=44760 WP = 60 \times 746 = 44760\text{ W}.
  2. Force needed F=mg+f=20000+4000=24000 NF = mg + f = 20000 + 4000 = 24000\text{ N}.
  3. v=PF=4476024000≈1.87 m/sv = \dfrac{P}{F} = \dfrac{44760}{24000} \approx 1.87\text{ m/s}
  4. So the answer is (d) 1.9 m s−11.9\text{ m s}^{-1}.
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Q231JEE Main 2020 · 5 SEP · SHIFT 2Medium

Power · Constant power: how v and s grow with t

A body of mass 2 kg is driven by an engine delivering a constant power of 1 J/s. The body starts from rest and moves in a straight line. After 9 seconds, the body has moved a distance (in m) _______.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 18

  1. For constant power from rest, x=(8P9m)1/2t3/2x = \left(\frac{8P}{9m}\right)^{1/2} t^{3/2}.
  2. x=8×19×2×93/2=23×27x = \sqrt{\frac{8 \times 1}{9 \times 2}} \times 9^{3/2} = \frac{2}{3} \times 27
  3. x=18 mx = 18\text{ m}
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Q232NEET 2016 · PHASE 1Medium

Power · Power from a force F(t)

A body of mass 1 kg begins to move under the action of a time dependent force F⃗=(2ti^+3t2j^)N,\vec{F} = \left(2t\hat{i} + 3t^2\hat{j}\right)N, where i^\hat{i} and j^\hat{j} are unit vectors along x and y axis. What power will be developed by the force at the time t?

Show answer and solution

Answer: (b)

  1. m=1m = 1 kg, so a⃗=2ti^+3t2j^\vec{a} = 2t\hat{i} + 3t^2\hat{j}; from rest v⃗=t2i^+t3j^\vec{v} = t^2\hat{i} + t^3\hat{j}.
  2. P=F⃗⋅v⃗=(2t)(t2)+(3t2)(t3)=2t3+3t5P = \vec{F} \cdot \vec{v} = (2t)(t^2) + (3t^2)(t^3) = 2t^3 + 3t^5
  3. So the answer is (b) (2t3+3t5)(2t^3 + 3t^5) W.
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Q233JEE Main 2016 · 9 APR · SHIFT 1Difficult

Power · Lifts & vehicles against friction

A car of weight W is on an inclined road that rises by 100 m over a distance of 1 km and applies a constant frictional force W20\frac{W}{20} on the car. While moving uphill on the road at a speed of 10 ms−1, the car needs power P. If it needs power P2\frac{P}{2} while moving downhill at speed v then value of vv is:

Show answer and solution

Answer: (b)

  1. sin⁡θ=1001000=110\sin\theta = \frac{100}{1000} = \frac{1}{10}, so the gravity component along the road is W10\frac{W}{10}.
  2. Uphill: P=(W10+W20)(10)=1.5WP = \left(\frac{W}{10} + \frac{W}{20}\right)(10) = 1.5W
  3. Downhill (magnitude of net resisting force): P2=(W10−W20)v=W20v\frac{P}{2} = \left(\frac{W}{10} - \frac{W}{20}\right)v = \frac{W}{20}v
  4. 0.75W=W20v⇒v=15 m/s0.75W = \frac{W}{20}v \Rightarrow v = 15\text{ m/s}
  5. So the answer is (b) 15 m/s.
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Q234NEET 2015 · AIPMTMedium

Power · Average power: P = W/t

The heart of a man pumps 5 litres of blood through the arteries per minute at a pressure of 150 mm of mercury. If the density of mercury be 13.6 ×\times 103 kg/m3 and g = 10 m/s2 then the power (in watt) is

Show answer and solution

Answer: (c)

  1. Power of a pump P=p×VtP = p \times \dfrac{V}{t} (pressure × volume flow rate).
  2. p=hρg=0.15×13.6×103×10=2.04×104 Pap = h\rho g = 0.15 \times 13.6 \times 10^3 \times 10 = 2.04 \times 10^4\text{ Pa}
  3. Vt=5×10−360=8.33×10−5 m3/s\dfrac{V}{t} = \dfrac{5 \times 10^{-3}}{60} = 8.33 \times 10^{-5}\text{ m}^3/\text{s}
  4. P=2.04×104×8.33×10−5≈1.70 WP = 2.04 \times 10^4 \times 8.33 \times 10^{-5} \approx 1.70\text{ W}
  5. So the answer is (c) 1.70.
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Q235NEET 2015 · AIPMT · CANCELLED PAPERMedium

Power · Constant power: how v and s grow with t

A particle of mass m is driven by a machine that delivers a constant power k watts. If the particle starts from rest the force on the particle at time t is

Show answer and solution

Answer: (c)

  1. Constant power from rest: kt=12mv2⇒v=2ktmkt = \frac{1}{2}mv^2 \Rightarrow v = \sqrt{\frac{2kt}{m}}
  2. F=Pv=km2ktF = \frac{P}{v} = k\sqrt{\frac{m}{2kt}}
  3. F=mk2 t−1/2F = \sqrt{\frac{mk}{2}}\, t^{-1/2}
  4. So the answer is (c).
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Q236NEET 2013Easy

Power · Average power: P = W/t

One coolie takes 1 minute to raise a suitcase through a height of 2 m but the second coolie takes 30 s to raise the same suitcase to the same height. The powers of two coolies are in the ratio

Show answer and solution

Answer: (d)

  1. Both do the same work mghmgh, so P=mght∝1tP = \dfrac{mgh}{t} \propto \dfrac{1}{t}.
  2. P1P2=t2t1=3060=12\dfrac{P_1}{P_2} = \dfrac{t_2}{t_1} = \dfrac{30}{60} = \dfrac{1}{2}
  3. So the answer is (d) 1:21:2.
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Q237JEE Main 2013 · 25 APR · SHIFT 1Easy

Power · Conveyors, jets & wind

A wind-powered generator converts wind energy into electrical energy. Assume that the generator converts a fixed fraction of the wind energy intercepted by its blades into electrical energy. For wind speed vv, the electrical power output will be most likely proportional to

Show answer and solution

Answer: (d)

  1. Mass of air hitting blades per second =ρAv= \rho A v.
  2. KE carried per second =12(ρAv)v2=12ρAv3= \dfrac{1}{2}(\rho A v)v^2 = \dfrac{1}{2}\rho A v^3.
  3. Output is a fixed fraction of this, so P∝v3P \propto v^3.
  4. So the answer is (d) v3v^3.
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Q238JEE Main 2013 · 23 APR · SHIFT 1Difficult

Power · Instantaneous power: P = F·v

A 70 kg man leaps vertically into the air from a crouching position. To take the leap the man pushes the ground with a constant force F to raise himself. The center of gravity rises by 0.5 m before he leaps. After the leap the c.g. rises by another 1 m. The maximum power delivered by the muscles is: (Take g = 10 ms−2-2)

Show answer and solution

Answer: (b)

  1. Work-energy over the whole motion: F(0.5)=mg(0.5+1)⇒F=3mg=2100 NF(0.5) = mg(0.5 + 1) \Rightarrow F = 3mg = 2100\text{ N}, net upward force F−mg=1400 NF - mg = 1400\text{ N}.
  2. Take-off speed (rises 1 m after leaving ground): v=2g×1=20=4.47 m/sv = \sqrt{2g \times 1} = \sqrt{20} = 4.47\text{ m/s}
  3. Speed is largest at take-off, so power is maximum there: P=(F−mg)v=1400×4.47≈6.26×103 WP = (F - mg)v = 1400 \times 4.47 \approx 6.26 \times 10^3\text{ W}
  4. So the answer is (b) 6.26×1036.26 \times 10^3 W at take off.
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Q239NEET 2012 · AIPMT · MAINSEasy

Power · Constant power: how v and s grow with t

A car of mass m starts from rest and accelerates so that the instantaneous power delivered to the car has a constant magnitude P0. The instantaneous velocity of this car is proportional to

Show answer and solution

Answer: (b)

  1. P0=mvdvdt⇒∫0vv dv=P0m∫0tdtP_0 = mv\dfrac{dv}{dt} \Rightarrow \int_0^v v\,dv = \dfrac{P_0}{m}\int_0^t dt.
  2. v2=2P0tm⇒v=2P0m t1/2v^2 = \dfrac{2P_0 t}{m} \Rightarrow v = \sqrt{\dfrac{2P_0}{m}}\,t^{1/2}
  3. So the answer is (b) t1/2t^{1/2}.
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Q240NEET 2011 · AIPMT · PRELIMSMedium

Power · Instantaneous power: P = F·v

A body projected vertically from the earth reaches a height equal to earth's radius before returning to the earth. The power exerted by the gravitational force is greatest

Show answer and solution

Answer: (b)

  1. Power of gravity P=F⃗⋅v⃗=mgvcos⁡θP = \vec{F} \cdot \vec{v} = mgv\cos\theta.
  2. Speed is largest at the earth's surface (and gg is also largest there).
  3. Just after projection v⃗\vec{v} is opposite to gravity, so PP is negative; just before hitting, v⃗\vec{v} is along gravity, so PP is maximum positive.
  4. So the answer is (b).
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Q241NEET 2010 · AIPMT · MAINSMedium

Power · Instantaneous power: P = F·v

A particle of mass M, starting from rest, undergoes uniform acceleration. If the speed acquired in time T is V, the power delivered to the particle is

Show answer and solution

Answer: (d)

  1. Work done =ΔKE=12MV2= \Delta KE = \dfrac{1}{2}MV^2.
  2. Average power P=WT=MV22TP = \dfrac{W}{T} = \dfrac{MV^2}{2T}
  3. So the answer is (d).
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Q242NEET 2010 · AIPMT · PRELIMSMedium

Power · Conveyors, jets & wind

An engine pumps water through a hose pipe. Water passes through the pipe and leaves it with a velocity of 2 m/s. The mass per unit length of water in the pipe is 100 kg/m. What is the power of the engine?

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Answer: (a)

  1. Mass leaving per second =λv= \lambda v (λ\lambda = mass per unit length).
  2. P=12(λv)v2=12λv3P = \dfrac{1}{2}(\lambda v)v^2 = \dfrac{1}{2}\lambda v^3
  3. P=12×100×23=400 WP = \dfrac{1}{2} \times 100 \times 2^3 = 400\text{ W}
  4. So the answer is (a) 400 W.
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Q243NEET 2009 · AIPMTMedium

Power · Conveyors, jets & wind

An engine pumps water continuously through a hose. Water leaves the hose with a velocity v and m is the mass per unit length of the water jet. What is the rate at which kinetic energy is imparted to water?

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Answer: (d)

  1. Mass leaving per second =mv= mv.
  2. Rate of KE given =12(mv)v2=12mv3= \dfrac{1}{2}(mv)v^2 = \dfrac{1}{2}mv^3
  3. So the answer is (d) 12mv3\dfrac{1}{2}mv^3.
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Q244NEET 2008 · AIPMTEasy

Power · Average power: P = W/t

Water falls from a height of 60 m at the rate of 15 kg/s to operate a turbine. The losses due to frictional forces are 10% of energy. How much power is generated by the turbine? (g = 10 m/s2)

Show answer and solution

Answer: (c)

  1. Input power =mtgh=15×10×60=9000 W= \dfrac{m}{t}gh = 15 \times 10 \times 60 = 9000\text{ W}.
  2. 10% is lost, so output =0.9×9000=8100 W= 0.9 \times 9000 = 8100\text{ W}.
  3. So the answer is (c) 8.1 kW8.1\text{ kW}.
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Q245JEE Main 2005 · AIEEEEasy

Power · Instantaneous power: P = F·v

A body of mass mm is accelerated uniformly from rest to a speed vv in a time T.T. The instantaneous power delivered to the body as a function of time is given by

Show answer and solution

Answer: (b)

  1. Uniform acceleration a=vTa = \dfrac{v}{T}, so force F=mvTF = \dfrac{mv}{T}.
  2. Speed at time tt: v(t)=vTtv(t) = \dfrac{v}{T}t.
  3. P=F v(t)=mv2T2 tP = F\,v(t) = \dfrac{mv^2}{T^2}\,t
  4. So the answer is (b).
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Q246JEE Main 2004 · AIEEEEasy

Power · Instantaneous power: P = F·v

A body of mass ’m’,\text{'}m\text{'}, accelerates uniformly from rest to ’v1’\text{'}v_1\text{'} in time TT. The instantaneous power delivered to the body as a function of time is given by

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Answer: (b)

  1. a=v1Ta = \dfrac{v_1}{T}, so F=mv1TF = \dfrac{mv_1}{T} and v(t)=v1tTv(t) = \dfrac{v_1 t}{T}.
  2. P=F v(t)=mv12 tT2P = F\,v(t) = \dfrac{mv_1^2\,t}{T^2}
  3. So the answer is (b).
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Q247JEE Main 2003 · AIEEEEasy

Power · Constant power: how v and s grow with t

A body is moved along a straight line by a machine delivering a constant power. The distance moved by the body in time ’t’\text{'}t\text{'} is proportional to

Show answer and solution

Answer: (b)

  1. Constant power: mvdvdt=P⇒v∝t1/2mv\dfrac{dv}{dt} = P \Rightarrow v \propto t^{1/2}.
  2. s=∫v dt∝t3/2s = \int v\,dt \propto t^{3/2}
  3. So the answer is (b) t3/2t^{3/2}.
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Q248NEET 2000 · AIPMTEasy

Power · Instantaneous power: P = F·v

If F⃗=(60i^+15j^−3k^)\vec{F} = \left(60\hat{i} + 15\hat{j} - 3\hat{k}\right) N andv⃗=(2i^−4j^+5k^)\vec{v} = \left(2\hat{i} - 4\hat{j} + 5\hat{k}\right) m/s, then instantaneous power is

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Answer: (b)

  1. P=F⃗⋅v⃗P = \vec{F} \cdot \vec{v}.
  2. P=(60)(2)+(15)(−4)+(−3)(5)=120−60−15=45 WP = (60)(2) + (15)(-4) + (-3)(5) = 120 - 60 - 15 = 45\text{ W}
  3. So the answer is (b) 45 watt.
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Q249NEET 1990 · AIPMTEasy

Power · Average power: P = W/t

How much water a pump of 2 kW2\text{ kW} can raise in one minute to a height of 10 m10\text{ m}? (take g=10 m/s2g = 10\text{ m/s}^2)

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Answer: (b)

  1. Work done in time tt: Pt=mghPt = mgh.
  2. m=Ptgh=2000×6010×10=1200 kgm = \dfrac{Pt}{gh} = \dfrac{2000 \times 60}{10 \times 10} = 1200\text{ kg}
  3. 1 kg of water is 1 litre, so the answer is (b) 1200 litres.
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Q250NEET 2024Easy

Collisions · Rebound from the ground

An object falls from a height of 10 m10\text{ m} above the ground. After striking the ground it loses 50%50\% of its kinetic energy. The height upto which the object can rebound from the ground is:

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Answer: (d)

  1. KE just before impact =mgh=mg(10)= mgh = mg(10).
  2. After losing 50%, KE =12mg(10)=mg(5)= \frac{1}{2}mg(10) = mg(5)
  3. This KE lifts it to h′=5 mh' = 5\text{ m}
  4. So the answer is (d) 5 m.
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Q251JEE Main 2024 · 4 APR · SHIFT 1Easy

Collisions · Rebound from the ground

If a rubber ball falls from a height hh and rebounds upto the height of h/2h/2. The percentage loss of total energy of the initial system as well as velocity of ball before it strikes the ground, respectively, are:

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Answer: (a)

  1. Initial energy mghmgh, final energy mgh2mg\frac{h}{2}, so loss =50%= 50\%.
  2. Speed before striking: 12mv2=mgh⇒v=2gh\frac{1}{2}mv^2 = mgh \Rightarrow v = \sqrt{2gh}
  3. So the answer is (a) 50%,2gh50\%, \sqrt{2gh}.
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Q252JEE Main 2023 · 6 APR · SHIFT 2Medium

Collisions · Rebound from the ground

A body is dropped on ground from a height 'h1h_1 ' and after hitting the ground, it rebounds to a height 'h2h_2'. If the ratio of velocities of the body just before and after hitting ground is 4, then percentage loss in kinetic energy of the body is x4\frac{x}{4}. The value of xx is ____________.

Numerical answer type. Work it out, then open the answer.

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Answer: 375

  1. v1v2=4⇒K2K1=116\frac{v_1}{v_2} = 4 \Rightarrow \frac{K_2}{K_1} = \frac{1}{16}
  2. Fractional loss =1−116=1516=93.75%= 1 - \frac{1}{16} = \frac{15}{16} = 93.75\%
  3. x4=93.75⇒x=375\frac{x}{4} = 93.75 \Rightarrow x = 375
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Q253JEE Main 2023 · 8 APR · SHIFT 2Medium

Collisions · Perfectly inelastic: bullet in a block

A bullet of mass 0.1 kg0.1\text{ kg} moving horizontally with speed 400 m s−1400\text{ m s}^{-1} hits a wooden block of mass 3.9 kg3.9\text{ kg} kept on a horizontal rough surface. The bullet gets embedded into the block and moves 20 m20\text{ m} before coming to rest. The coefficient of friction between the block and the surface is __________. (Given g=10 m/s2g = 10\text{ m/s}^2)

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Answer: (b)

  1. Momentum: 0.1×400=4 v⇒v=10 m/s0.1 \times 400 = 4\,v \Rightarrow v = 10\text{ m/s}
  2. Friction stops it: v2=2μgs⇒100=2μ(10)(20)v^2 = 2\mu g s \Rightarrow 100 = 2\mu(10)(20)
  3. μ=100400=0.25\mu = \frac{100}{400} = 0.25
  4. So the answer is (b) 0.25.
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Q254JEE Main 2022 · 25 JUL · SHIFT 2Easy

Collisions · Perfectly inelastic: bullet in a block

A bag of sand of mass 9.8 kg is suspended by a rope. A bullet of 200 g travelling with speed 10 ms−1{}^{-1} gets embedded in it, then loss of kinetic energy will be:

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Answer: (b)

  1. Momentum: 0.2×10=10 v⇒v=0.2 m/s0.2 \times 10 = 10\,v \Rightarrow v = 0.2\text{ m/s}
  2. Ki=12(0.2)(10)2=10 JK_i = \frac{1}{2}(0.2)(10)^2 = 10\text{ J}, Kf=12(10)(0.2)2=0.2 JK_f = \frac{1}{2}(10)(0.2)^2 = 0.2\text{ J}
  3. Loss =10−0.2=9.8 J= 10 - 0.2 = 9.8\text{ J}
  4. So the answer is (b) 9.8 J.
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Q255JEE Main 2021 · 31 AUG · SHIFT 2Medium

Collisions · Explosion & splitting

A block moving horizontally on a smooth surface with a speed of 40 m/s splits into two parts with masses in the ratio of 1: 2. If the smaller part moves at 60 m/s in the same direction, then the fractional change in kinetic energy is :-

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Answer: (c)

  1. Masses mm and 2m2m: 3m(40)=m(60)+2m v⇒v=30 m/s3m(40) = m(60) + 2m\,v \Rightarrow v = 30\text{ m/s}
  2. Ki=12(3m)(40)2=2400mK_i = \frac{1}{2}(3m)(40)^2 = 2400m
  3. Kf=12m(60)2+12(2m)(30)2=1800m+900m=2700mK_f = \frac{1}{2}m(60)^2 + \frac{1}{2}(2m)(30)^2 = 1800m + 900m = 2700m
  4. ΔKKi=3002400=18\frac{\Delta K}{K_i} = \frac{300}{2400} = \frac{1}{8}
  5. So the answer is (c) 18\frac{1}{8}.
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Q256JEE Main 2021 · 31 AUG · SHIFT 1Medium

Collisions · Explosion & splitting

A block moving horizontally on a smooth surface with a speed of 40 ms−1{}^{-1} splits into two equal parts. If one of the parts moves at 60 ms−1{}^{-1} in the same direction, then the fractional change in the kinetic energy will be x: 4 where x = ___________.

Numerical answer type. Work it out, then open the answer.

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Answer: 1

  1. Equal parts mm each: 2m(40)=m(60)+m v⇒v=20 m/s2m(40) = m(60) + m\,v \Rightarrow v = 20\text{ m/s}
  2. Ki=12(2m)(40)2=1600mK_i = \frac{1}{2}(2m)(40)^2 = 1600m, Kf=12m(602+202)=2000mK_f = \frac{1}{2}m(60^2 + 20^2) = 2000m
  3. ΔKKi=4001600=14=x:4\frac{\Delta K}{K_i} = \frac{400}{1600} = \frac{1}{4} = x : 4
  4. x=1x = 1
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Q257JEE Main 2017 · 8 APR · SHIFT 1Medium

Collisions · Rebound from the ground

An object is dropped from a height h from the ground. Every time it hits the ground it loses 50% of its kinetic energy. The total distance covered as t →∞\to \infty is:

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Answer: (a)

  1. Each bounce keeps half the KE, so each rebound height is half the previous: h,h2,h4,…h, \frac{h}{2}, \frac{h}{4}, \dots
  2. Distance =h+2(h2+h4+… )=h+2h= h + 2\left(\frac{h}{2} + \frac{h}{4} + \dots\right) = h + 2h
  3. =3h= 3h
  4. So the answer is (a) 3h.
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Q258NEET 2015 · AIPMTMedium

Collisions · Head-on collisions & restitution

Two particles A and B, move with constant velocities v⃗1\vec{v}_1 and v⃗2\vec{v}_2. At the initial moment their position vectors are r⃗1\vec{r}_1 and r⃗2\vec{r}_2 respectively. The condition for particles A and B for their collision is

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Answer: (c)

  1. Collision at time tt: r⃗1+v⃗1t=r⃗2+v⃗2t\vec r_1 + \vec v_1 t = \vec r_2 + \vec v_2 t
  2. r⃗1−r⃗2=(v⃗2−v⃗1)t\vec r_1 - \vec r_2 = (\vec v_2 - \vec v_1)t with t>0t > 0, so the two vectors point the same way.
  3. Equal unit vectors: r⃗1−r⃗2∣r⃗1−r⃗2∣=v⃗2−v⃗1∣v⃗2−v⃗1∣\frac{\vec r_1 - \vec r_2}{|\vec r_1 - \vec r_2|} = \frac{\vec v_2 - \vec v_1}{|\vec v_2 - \vec v_1|}
  4. So the answer is (c).
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Q259NEET 2015 · AIPMTMedium

Collisions · Oblique collision

On a frictionless surface, a block of mass M moving at speed v collides elastically with another block of same mass M which is initially at rest. After collision the first block moves at an angle θ\theta to its initial direction and has a speed v3.\frac{v}{3}. The second block's speed after the collision is

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Answer: (c)

  1. Elastic collision: kinetic energy is conserved, 12Mv2=12M(v3)2+12Mv22\frac{1}{2}Mv^2 = \frac{1}{2}M\left(\frac{v}{3}\right)^2 + \frac{1}{2}Mv_2^2
  2. v22=v2−v29=89v2v_2^2 = v^2 - \frac{v^2}{9} = \frac{8}{9}v^2
  3. v2=223vv_2 = \frac{2\sqrt{2}}{3}v
  4. So the answer is (c).
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Q260NEET 2015 · AIPMTMedium

Collisions · Rebound from the ground

A ball is thrown vertically downwards from a height of 20 m with an initial velocity v0. It collides with the ground, losses 50 percent of its energy in collision and rebounds to the same height. The initial velocity v0 is

(Take g = 10 m s−2{}^{-2})

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Answer: (d)

  1. Energy at ground before impact: 12mv02+mgh\frac{1}{2}mv_0^2 + mgh
  2. Half is lost and the rest lifts it back to hh: 12(12mv02+mgh)=mgh\frac{1}{2}\left(\frac{1}{2}mv_0^2 + mgh\right) = mgh
  3. 12v02=gh⇒v0=2×10×20\frac{1}{2}v_0^2 = gh \Rightarrow v_0 = \sqrt{2 \times 10 \times 20}
  4. So the answer is (d) 20 m/s.
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Q261NEET 2011 · AIPMT · MAINSMedium

Collisions · Perfectly inelastic: bullet in a block

A mass m moving horizontally (along the x-axis) with velocity vv collides and sticks to a mass of 3m moving vertically upwards (along the y-axis) with velocity 2vv. The final velocity of the combination is

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Answer: (b)

  1. Momentum is conserved in each direction; total mass 4m4m.
  2. xx: mv=4m vx⇒vx=v4mv = 4m\,v_x \Rightarrow v_x = \frac{v}{4}
  3. yy: 3m(2v)=4m vy⇒vy=3v23m(2v) = 4m\,v_y \Rightarrow v_y = \frac{3v}{2}
  4. So the answer is (b) 14vi^+32vj^\frac{1}{4}v\hat i + \frac{3}{2}v\hat j.
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Q262NEET 2010 · AIPMT · PRELIMSMedium

Collisions · Head-on collisions & restitution

A ball moving with velocity 2 m/s collides head on with another stationary ball of double the mass. If the coefficient of restitution is 0.5, then their velocities (in m/s) after collision will be

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Answer: (a)

  1. Momentum: m(2)=mv1+2mv2⇒v1+2v2=2m(2) = m v_1 + 2m v_2 \Rightarrow v_1 + 2v_2 = 2
  2. Restitution: v2−v1=e(2)=1v_2 - v_1 = e(2) = 1
  3. Solving: 3v2=3⇒v2=13v_2 = 3 \Rightarrow v_2 = 1, v1=0v_1 = 0
  4. So the answer is (a) 0, 1.
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Q263NEET 2000 · AIPMTMedium

Collisions · Explosion & splitting

A mass of 1 kg is thrown up with a velocity of 100 m/s. After 5 seconds, it explodes into two parts. One part of mass 400 g comes down with a velocity 25 m/s. The velocity of other part is (Take g = 10 ms−2{}^{-2})

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Answer: (c)

  1. Velocity after 5 s: v=100−10×5=50 m/sv = 100 - 10 \times 5 = 50\text{ m/s} upward.
  2. Momentum (up positive): 1×50=0.4(−25)+0.6 v′1 \times 50 = 0.4(-25) + 0.6\,v'
  3. 0.6 v′=60⇒v′=100 m/s0.6\,v' = 60 \Rightarrow v' = 100\text{ m/s} upward
  4. So the answer is (c) 100 m/s.
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