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Question

Question: Select the correct alternative(s)....

Select the correct alternative(s).

A

The work done by kinetic friction acting with in system on system is always negative.

B

Work done by static friction may be positive, negative and zero.

C

If a particle moves in a straight line with constant acceleration under a constant force then power developed by this force varies linearly with displacement.

D

If kinetic energy of particle moving in straight line is proportional to time then magnitude of force acting on particle is inversely proportional to speed of particle.

Answer

A, B, D

Explanation

Solution

The question asks us to identify the correct statement(s) among the given alternatives. Let's analyze each statement:

(A) The work done by kinetic friction acting within system on system is always negative.

Consider a system of two bodies in relative motion, say body 1 and body 2. Let f12\vec{f}_{12} be the kinetic friction force exerted by body 2 on body 1, and f21\vec{f}_{21} be the kinetic friction force exerted by body 1 on body 2. By Newton's third law, f12=f21\vec{f}_{12} = -\vec{f}_{21}.

The total work done by these internal kinetic friction forces on the system is Winternal=f12d1+f21d2W_{internal} = \vec{f}_{12} \cdot \vec{d}_1 + \vec{f}_{21} \cdot \vec{d}_2, where d1\vec{d}_1 and d2\vec{d}_2 are the displacements of body 1 and body 2, respectively.

Substituting f21=f12\vec{f}_{21} = -\vec{f}_{12}, we get: Winternal=f12d1f12d2=f12(d1d2)=f12drelW_{internal} = \vec{f}_{12} \cdot \vec{d}_1 - \vec{f}_{12} \cdot \vec{d}_2 = \vec{f}_{12} \cdot (\vec{d}_1 - \vec{d}_2) = \vec{f}_{12} \cdot \vec{d}_{rel}, where drel=d1d2\vec{d}_{rel} = \vec{d}_1 - \vec{d}_2 is the relative displacement of body 1 with respect to body 2.

Kinetic friction always opposes the relative motion between surfaces. This means the kinetic friction force f12\vec{f}_{12} on body 1 is always opposite to the relative velocity vrel=v1v2\vec{v}_{rel} = \vec{v}_1 - \vec{v}_2. Since vrel\vec{v}_{rel} and drel\vec{d}_{rel} are in the same direction, f12\vec{f}_{12} is opposite to drel\vec{d}_{rel}.

Therefore, the angle between f12\vec{f}_{12} and drel\vec{d}_{rel} is 180180^\circ.

So, f12drel=f12drelcos(180)=f12drel\vec{f}_{12} \cdot \vec{d}_{rel} = f_{12} d_{rel} \cos(180^\circ) = -f_{12} d_{rel}.

Since f12>0f_{12} > 0 and drel0d_{rel} \ge 0, the work done WinternalW_{internal} is always negative or zero (if no relative displacement).

Thus, statement (A) is correct.

(B) Work done by static friction may be positive, negative and zero.

  • Zero Work: When a body is at rest on a surface, static friction acts but no displacement occurs, so work done is zero. For a wheel undergoing pure rolling, the point of contact with the ground is instantaneously at rest, so static friction at this point does no work.
  • Positive Work: When a person walks, static friction acts on their feet in the forward direction, propelling them forward. The displacement is in the same direction as the force, so work done is positive.
  • Negative Work: When a car applies brakes and the wheels are still rolling (not skidding), static friction acts on the wheels opposite to the direction of motion. The displacement is in the direction of motion, so work done is negative.

Thus, statement (B) is correct.

(C) If a particle moves in a straight line with constant acceleration under a constant force then power developed by this force varies linearly with displacement.

Let the constant force be FF. Since the acceleration is constant, let it be aa.

The power developed by the force is P=FvP = Fv, where vv is the instantaneous velocity.

For constant acceleration, we have the kinematic equation v2=u2+2asv^2 = u^2 + 2as, where uu is the initial velocity and ss is the displacement.

From this, v=u2+2asv = \sqrt{u^2 + 2as}.

Substituting this into the power equation: P=Fu2+2asP = F\sqrt{u^2 + 2as}.

This relationship is not linear with displacement ss. It varies as the square root of a linear function of ss.

For instance, if u=0u=0, then P=F2as=(F2a)sP = F\sqrt{2as} = (F\sqrt{2a})\sqrt{s}, which shows PsP \propto \sqrt{s}. This is not linear.

Thus, statement (C) is incorrect.

(Note: Power varies linearly with time: P=F(u+at)=Fu+FatP = F(u+at) = Fu + Fat.)

(D) If kinetic energy of particle moving in straight line is proportional to time then magnitude of force acting on particle is inversely proportional to speed of particle.

Given that kinetic energy KK is proportional to time tt: K=ctK = ct, where cc is a constant.

The power developed by the net force acting on the particle is P=dKdtP = \frac{dK}{dt}.

P=ddt(ct)=cP = \frac{d}{dt}(ct) = c.

So, the power developed is constant.

Also, power is related to force and velocity by P=FvP = Fv (since the particle moves in a straight line, and we consider the component of force along the velocity).

Since P=cP = c (constant), we have Fv=cFv = c.

Therefore, the magnitude of the force F=cvF = \frac{c}{v}.

This shows that the magnitude of the force is inversely proportional to the speed of the particle (F1vF \propto \frac{1}{v}).

Thus, statement (D) is correct.

Based on the analysis, statements (A), (B), and (D) are correct.