A carpet of mass $m$ made of inextensible material is rolled along its length in the form of a cylinder of radius $r$ and kept on a rough floor. The decrease in the potential energy of the system, when the carpet is unrolled to a radius $\frac{r}{2}$
without sliding is $(g=$ acceleration due to gravity)
The centre of mass of the whole carpet is originally at a height R above the floor. When the carpet unrolls itself and has a radius R/2, the centre of mass is at a height R/2. The mass left over unrolled is $\frac{M\pi\left(R / 2\right)^{2}}{\pi R^{2}}=\frac{M}{4}$
Decrease in potential energy
$MgR-\left(\frac{M}{4}\right)g\left(\frac{R}{2}\right)=\frac{7}{8}MgR$Density $\sigma=\frac{M}{\pi r_{2}}=\frac{M_{1}}{\pi\left(\frac{r}{2}\right)^{2}}$
or $ M_{1}=\frac{M}{4} $
Potential energy $ U_{1}=$M g r
and $U_{2}=M_{1} g \frac{r}{2}=\frac{M}{4} g \frac{r}{2}$
The decrease in the potential energy of the system
$\Delta U =U_{1}-U_{2} $$=M g r-\frac{M g r}{8} $$=\frac{7 M g r}{8}$
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.