Question
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 m can move on a long plank of mass M 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 v with respect to the plank. Coefficient of friction between the plank and the floor is μ and acceleration of free fall is g. How will velocity of the car with respect to the floor vary with time t after it is switched on?

v
Solution
Let vc,f be the velocity of the car with respect to the floor, and vp,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=v. The velocities are related by vc,f=vc,p+vp,f. Assuming motion along a line, vc,f=v+vp,f.
Differentiating with respect to time, the accelerations are related by ac,f=dtdv+ap,f. Since v is constant, dtdv=0. Thus, ac,f=ap,f.
Let a=ac,f=ap,f.
The net external horizontal force on the car-plank system is the friction force on the plank from the floor, fk.
By Newton's second law for the system, fk=(m+M)ACM, where ACM is the acceleration of the center of mass.
ACM=m+Mmac,f+Map,f=m+Mma+Ma=a.
So, fk=(m+M)a.
The kinetic friction force is fk=−μ(M+m)g∣vp,f∣vp,f for vp,f=0.
Thus, (M+m)a=−μ(M+m)g∣vp,f∣vp,f, which simplifies to a=−μg∣vp,f∣vp,f.
Since a=ap,f=dtdvp,f, we have dtdvp,f=−μg∣vp,f∣vp,f for vp,f=0.
Given the initial condition vp,f(0)=0, this differential equation can only be satisfied for t>0 if vp,f(t)=0. Any attempt for vp,f to become non-zero leads to a contradiction in the sign of acceleration and velocity.
Therefore, vp,f(t)=0 for all t≥0.
The velocity of the car with respect to the floor is vc,f(t)=v+vp,f(t)=v+0=v.
The velocity of the car with respect to the floor is a constant v.
The final answer is v.