One end of a thin heavy uniform inextensible perfectly flexible rope of length \(2L\)
and mass \(2M\)
is attached to a fixed point \(P\). A particle of mass \(m\) is
attached to the other end. Initially, the particle is held at
\(P\) and the rope hangs vertically in a loop below \(P\). The particle is then released
so that it and a section of the rope (of decreasing length)
fall vertically as shown in the diagram.
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\psline[linewidth=0.1pt,linestyle=dashed,dash=2pt 2pt]{<->}(2.53,3.2)(2.53,5)
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\psline(2.02,0.26)(2.03,0)
\psline(2.03,0)(2.06,0.25)
\rput[tl](1.94,5.45){\(P\)}
\rput[tl](2.6,4.25){\(x\)}
\rput[tl](0.2,2.85){\(L+\frac{1}{2}x\)}
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You may assume that
each point on the moving section of the rope falls at the same speed as the
particle. Given that energy is conserved, show
that, when the particle has fallen a distance \(x\) (where \(x< 2L\)),
its speed \(v\) is given by
\[
v^2 = \frac { 2g x \big( mL +ML - \frac14 Mx)}{mL +ML - \frac12 Mx}\,.
\]
Hence show that the acceleration of the particle is
\[
g +
\frac{ Mgx\big(mL+ML- \frac14 Mx\big)}{2\big(mL +ML -\frac12 Mx\big)^2}\,
\,.\]
Deduce that the acceleration of the particle after it is
released is greater than \(g\).