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Question

A board of mass \(m=11~kg\) is placed on the floor and a man of mass \(m=70~kg\) is standing on the board as shown (Case\(−I\)). The coefficient of friction between the board and the floor is \(\mu=0.25\). The maximum force that the man can exert on the rope so that the board does not slip on the floor is:

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Solution


For man \(+\) board system,
\(f=2T\)

\(T+N=(M+m)g\)

\(N=(M+m)g-T\)

If board is not sliding

\(f\leq \mu N\)

\(2T\leq \mu[(M+m)g-T)]\)

\([2+\mu]T\leq \mu(M+m)g\)

\(T\leq \dfrac{\mu(M+m)g}{(2+\mu)}\)
Hence,

\(T_{max}=\dfrac{\mu(M+m)g}{2+\mu}\)

After substituting the values:

\(T_{max}=\dfrac{0.25(70+11)}{(2+0.25)}\times10\)

\(=\dfrac{0.25\times81\times10}{2.25}=90~N\)


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