6.
\begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{86a37170-046f-46e5-9c8c-06d5f98ca4fe-20_497_1337_246_365}
\captionsetup{labelformat=empty}
\caption{Figure 4}
\end{figure}
Two blocks, \(A\) and \(B\), of masses 2 kg and 4 kg respectively are attached to the ends of a light inextensible string.
Initially \(A\) is held on a fixed rough plane. The plane is inclined to horizontal ground at an angle \(\theta\), where \(\tan \theta = \frac { 3 } { 4 }\)
The string passes over a small smooth light pulley \(P\) that is fixed at the top of the plane. The part of the string from \(A\) to \(P\) is parallel to a line of greatest slope of the plane.
Block \(A\) is held on the plane with the distance \(A P\) greater than 3 m .
Block \(B\) hangs freely below \(P\) at a distance of 3 m above the ground, as shown in Figure 4.
The coefficient of friction between \(A\) and the plane is \(\mu\)
Block \(A\) is released from rest with the string taut.
By modelling the blocks as particles,
- find the potential energy lost by the whole system as a result of \(B\) falling 3 m .
Given that the speed of \(B\) at the instant it hits the ground is \(4.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }\) and ignoring air resistance,
- use the work-energy principle to find the value of \(\mu\)
After \(B\) hits the ground, \(A\) continues to move up the plane but does not reach the pulley in the subsequent motion.
Block \(A\) comes to instantaneous rest after moving a total distance of ( \(3 + d\) ) m from its point of release.
Ignoring air resistance, - use the work-energy principle to find the value of \(d\)
\includegraphics[max width=\textwidth, alt={}, center]{86a37170-046f-46e5-9c8c-06d5f98ca4fe-20_2255_50_309_1981}