Consider the situation shown in the figure. Uniform rod
of length
can rotate freely about the hinge
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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2 M g − T = 2 M a ----> 1
T − M g = M a -----> 2
where T = tension in the string connected two the hanging masses, and a = their acceleration.
Adding 1 & 2
we get a = 3 g and T = 3 4 M g
let mass of the rod A B be m
now balance the torque on the rod A B about point A .
2 m g L = 2 T L (we have taken 2 T force at end B because the string connected to the rod is acted upon by T on the both side of the 2 n d pulley)
⇒ 2 m g L = 3 8 M g L
therefore m = 3 1 6 M