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Question: A remote controlled car of mass \(m\) can move on a long plank of mass \(M\) that rests on a horizon...

A remote controlled car of mass mm can move on a long plank of mass MM that rests on a horizontal floor. The mechanism of the car is so designed that it always moves on the plank with a constant velocity vv with respect to the plank. Coefficient of friction between the plank and the floor is μ\mu and acceleration of free fall is gg. How will velocity of the car with respect to the floor vary with time tt after it is switched on?

Answer

v

Explanation

Solution

Let vc,fv_{c,f} be the velocity of the car with respect to the floor, and vp,fv_{p,f} be the velocity of the plank with respect to the floor. The velocity of the car with respect to the plank is given as vc,p=vv_{c,p} = v. The velocities are related by vc,f=vc,p+vp,fv_{c,f} = v_{c,p} + v_{p,f}. Assuming motion along a line, vc,f=v+vp,fv_{c,f} = v + v_{p,f}.

Differentiating with respect to time, the accelerations are related by ac,f=dvdt+ap,fa_{c,f} = \frac{dv}{dt} + a_{p,f}. Since vv is constant, dvdt=0\frac{dv}{dt} = 0. Thus, ac,f=ap,fa_{c,f} = a_{p,f}.

Let a=ac,f=ap,fa = a_{c,f} = a_{p,f}.

The net external horizontal force on the car-plank system is the friction force on the plank from the floor, fkf_k.

By Newton's second law for the system, fk=(m+M)ACMf_k = (m+M)A_{CM}, where ACMA_{CM} is the acceleration of the center of mass.

ACM=mac,f+Map,fm+M=ma+Mam+M=aA_{CM} = \frac{m a_{c,f} + M a_{p,f}}{m+M} = \frac{m a + M a}{m+M} = a.

So, fk=(m+M)af_k = (m+M)a.

The kinetic friction force is fk=μ(M+m)gvp,fvp,ff_k = -\mu(M+m)g \frac{v_{p,f}}{|v_{p,f}|} for vp,f0v_{p,f} \ne 0.

Thus, (M+m)a=μ(M+m)gvp,fvp,f(M+m)a = -\mu(M+m)g \frac{v_{p,f}}{|v_{p,f}|}, which simplifies to a=μgvp,fvp,fa = -\mu g \frac{v_{p,f}}{|v_{p,f}|}.

Since a=ap,f=dvp,fdta = a_{p,f} = \frac{dv_{p,f}}{dt}, we have dvp,fdt=μgvp,fvp,f\frac{dv_{p,f}}{dt} = -\mu g \frac{v_{p,f}}{|v_{p,f}|} for vp,f0v_{p,f} \ne 0.

Given the initial condition vp,f(0)=0v_{p,f}(0)=0, this differential equation can only be satisfied for t>0t>0 if vp,f(t)=0v_{p,f}(t)=0. Any attempt for vp,fv_{p,f} to become non-zero leads to a contradiction in the sign of acceleration and velocity.

Therefore, vp,f(t)=0v_{p,f}(t) = 0 for all t0t \ge 0.

The velocity of the car with respect to the floor is vc,f(t)=v+vp,f(t)=v+0=vv_{c,f}(t) = v + v_{p,f}(t) = v + 0 = v.

The velocity of the car with respect to the floor is a constant vv.

The final answer is v\boxed{v}.