Work Power & Energy

NEET Physics · 97 questions · Page 4 of 10 · Click an option or "Show Solution" to reveal answer

Q31
A solid cylinder of mass 3 kg is rolling on a horizontal surface with velocity 4 m s -1 . It collides with a horizontal spring of force constant 200 N m -1 . The maximum compression produced in the spring will be
A 0.5 m
B 0.6 m
C 0.7 m
D 0.2 m
Correct Answer
Option B
Solution

At maximum compression the solid cylinder will stop so loss in K.E. of cylinder = gain in P.E. of spring

12mv2+12Iω2=12kx2\Rightarrow {1 \over 2}m{v^2} + {1 \over 2}I{\omega ^2} = {1 \over 2}k{x^2}
12mv2+12mR22(vR)2=12kx2\Rightarrow {1 \over 2}m{v^2} + {1 \over 2}{{m{R^2}} \over 2}{\left( {{v \over R}} \right)^2} = {1 \over 2}k{x^2}
34mv2=12kx2\Rightarrow {3 \over 4}m{v^2} = {1 \over 2}k{x^2}
34×3×(4)2=12×200x2\Rightarrow {3 \over 4} \times 3 \times {\left( 4 \right)^2} = {1 \over 2} \times 200{x^2}
36100=x2x=0.6m\Rightarrow {{36} \over {100}} = {x^2} \Rightarrow x = 0.6\,m
Q32
The potential energy of a particle in a force field is U=Ar2BrU = {A \over {{r^2}}} - {B \over 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
A B2A{B \over {2A}}
B 2AB{{2A} \over B}
C AB{A \over B}
D BA{B \over A}
Correct Answer
Option B
Solution

Here,

U=Ar2BrU = {A \over {{r^2}}} - {B \over r}

For equilibrium,

dUdr=0{{dU} \over {dr}} = 0
2Ar3+Br2=0\therefore - {{2A} \over {{r^3}}} + {B \over {{r^2}}} = 0
2Ar3=Br2r=2AB\Rightarrow {{2A} \over {{r^3}}} = {B \over {{r^2}}} \Rightarrow r = {{2A} \over B}

For stable equilibrium,

d2Udr2>0{{{d^2}U} \over {d{r^2}}} > 0
d2Udr2=6Ar42Br3{{{d^2}U} \over {d{r^2}}} = {{6A} \over {{r^4}}} - {{2B} \over {{r^3}}}
d2Udr2r=(2A/B)=6AB416A42B48A3=B48A3>0{\left. {{{{d^2}U} \over {d{r^2}}}} \right|_{r = \left( {2A/B} \right)}} = {{6A{B^4}} \over {16{A^4}}} - {{2{B^4}} \over {8{A^3}}} = {{{B^4}} \over {8{A^3}}} > 0

So for stable equilibrium, the distance of the particle is

2AB{{2A} \over B}

.

Q33
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
A 32vi^+14vj^{3 \over 2}v\widehat i + {1 \over 4}v\widehat j
B 14vi^+32vj^{1 \over 4}v\widehat i + {3 \over 2}v\widehat j
C 13vi^+23vj^{1 \over 3}v\widehat i + {2 \over 3}v\widehat j
D 23vi^+13vj^{2 \over 3}v\widehat i + {1 \over 3}v\widehat j
Correct Answer
Option B
Solution

According to conservation of momentum, we get

mvi^+(3m)2vj^=(m+3m)vmv\widehat i + \left( {3m} \right)2v\widehat j = \left( {m + 3m} \right)\overrightarrow {v'}

where

v\overrightarrow {v'}

is the final velocity after collision

v=14vi^+64vj^=14vi^+32vj^\overrightarrow {v'} = {1 \over 4}v\widehat i + {6 \over 4}v\widehat j = {1 \over 4}v\widehat i + {3 \over 2}v\widehat j
Q34
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
A at the highest position of the body
B at the instant just before the body hits the earth.
C it remains constant all through.
D at the instant just after the body is projected.
Correct Answer
Option B
Solution

Power, P =

F.v=Fvcosθ\overrightarrow F .\overrightarrow v = Fv\cos \theta

Just before hitting the earth θ\theta = 0°.

Hence, the power exerted by the gravitational force is greatest at the instant just before the body hits the earth.

Q35
Force F on a particle moving in a straight line varies with distance d as shown in figure. The work done on the particle during its displacement of 12 m is
A 18 J
B 21 J
C 26 J
D 13 J
Correct Answer
Option D
Solution

Work done = Area under (F-d) graph = Area of rectangle ABCD + Area of triangle DCE =

2×(73)+12×2×(127)=8+5=13J2 \times \left( {7 - 3} \right) + {1 \over 2} \times 2 \times \left( {12 - 7} \right) = 8 + 5 = 13J
Q36
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
A MV2T{{M{V^2}} \over T}
B 12MV2T2{1 \over 2}{{M{V^2}} \over {{T^2}}}
C MV2T2{{M{V^2}} \over {{T^2}}}
D 12MV2T{1 \over 2}{{M{V^2}} \over T}
Correct Answer
Option D
Solution

Power delivered in time T is P = F·V = MaV or

P=MVdVdTPdT=MVdVP = MV{{dV} \over {dT}} \Rightarrow PdT = MVdV
PT=MV22\Rightarrow PT = {{M{V^2}} \over 2}

or

P=12MV2TP = {1 \over 2}{{M{V^2}} \over T}
Q37
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?
A 400 W
B 200 W
C 100 W
D 800 W
Correct Answer
Option D
Solution

Here, Mass per unit length of water, μ\mu = 100 kg/m Velocity of water, v = 2 m/s Power of the engine, P = μ\muv 3 = (100 kg/m) (2 m/s) 3 = 800 W

Q38
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
A 0, 1
B 1, 1
C 1, 0.5
D 0, 2
Correct Answer
Option A
Solution

Here, m 1 = m, m 2 = 2m, u 1 = 2 m/s, u 2 = 0 Coefficient of restitution, e = 0.5 Let v 1 and v 2 be their respective velocities after collision.

Applying the law of conservation of linear momentum, we get m 1 u 1 + m 2 u 2 = m 1 v 1 + m 2 v 2 \therefore m × 2 + 2m × 0 = m × v 1 + 2m × v 2 or 2m = mv 1 + 2mv 2 or 2 = (v 1 + 2v 2 ) ...(i) By definition of coefficient of restitution,

e=v2v1u1u2e = {{{v_2} - {v_1}} \over {{u_1} - {u_2}}}

or e(u 1 – u 2 ) = v 2 – v 1 \Rightarrow 0.5(2 – 0) = v 2 – v 1 ...(ii) Solving equations (i) and (ii), we get v 1 = 0 m/s, v 2 = 1 m/s

Q39
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
A 2Mg/k
B 4Mg/k
C Mg/2k
D Mg/k
Correct Answer
Option A
Solution

When the mass attached to a spring fixed at the other end is allowed to fall suddenly, it extends the spring by x.

Potential energy lost by the mass is gained by the spring.

Mgx=12kx2x=2MgkMgx = {1 \over 2}k{x^2} \Rightarrow x = {{2Mg} \over k}
Q40
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/s 2 )
A 30 J
B 40 J
C 10 J
D 20 J
Correct Answer
Option D
Solution

Initial velocity u = 20 m/s; m = 1 kg Kinetic energy = maximum potential energy Initial kinetic energy =

12×1×202=200J{1 \over 2} \times 1 \times {20^2} = 200\,J

Mgh (max) = 200 J \therefore h = 20 m The height travelled by the body, h' = 18 m \therefore Loss of energy due to air friction = mgh – mgh' \Rightarrow Energy lost = 200 J – 1 × 10 × 18 J = 20 J.

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