Stubborn rod, it don't wanna move.....

Consider the situation shown in the figure. Uniform rod A B AB of length L L can rotate freely about the hinge A A in vertical plane. Pulleys and strings are light and frictionless. If the rod remains horizontal at rest when the system is released then the mass of rod is ->

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32 M 3 \frac{32M}{3} 8 M 5 \frac{8M}{5} 4 M 5 \frac{4M}{5} 16 M 3 \frac{16M}{3} 8 M 3 \frac{8M}{3} 4 M 3 \frac{4M}{3}

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2 solutions

Aniket Verma
Mar 5, 2015

2 M g T = 2 M a 2Mg - T = 2Ma ----> 1 1

T M g = M a T - Mg = Ma -----> 2 2

where T = T = tension in the string connected two the hanging masses, and a = a = their acceleration.

Adding 1 & 2 1 \& 2

we get a = g 3 a = \dfrac{g}{3} and T = 4 M g 3 T = \dfrac{4Mg}{3}

let mass of the rod A B AB be m m

now balance the torque on the rod A B AB about point A A .

m g L 2 = 2 T L \dfrac{mgL}{2} = 2TL (we have taken 2 T 2T force at end B B because the string connected to the rod is acted upon by T T on the both side of the 2 n d 2_{nd} pulley)

\Rightarrow m g L 2 = 8 M g L 3 \dfrac{mgL}{2} = \dfrac{8MgL}{3}

therefore m = 16 M 3 m = \dfrac{16M}{3}

My working was similar to yours, except that I took the force at end B to be T. Why is it 2T?

Aran Pasupathy - 5 years, 11 months ago

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weight of rod is supported by the second pulley which hangs masses M and 2M, therefore tension will be twice at the peg

Syed Baqir - 5 years, 11 months ago

After proper analysis , we find that both masses move with accelaration of magnitude g / 3 g/3 .

Thus tension T T in the pulley containing rope attatched to rod= 8 M g / 3 8Mg/3 .

Therefore τ n e t = 0 \tau_{net} =0 about hinge.

Hence m = 16 M / 3 m= 16M/3

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