A pulley fixed to the ceiling carries a string with blocks of masses $m$ and $3m$ attached to its ends. The masses of string and pulley are negligible. When the system is released, the acceleration of centre of mass will be
Let T be the tension in the string carrying the masses m and 3m. Let a be the acceleration, then $\hspace10mm $ T-mg=ma $\hspace5mm $ ...(i) $\hspace10mm $ 3mg-T=3ma $\hspace5mm ...(ii) $ $\hspace10mm $ 2mg=4ma $\Rightarrow \hspace10mm a= \frac {g}{2} $ $a_{cm} = -g/4$
Was this answer helpful?
0
0
Top Questions on System of Particles & Rotational Motion
The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.