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Question: The centre of mass of given system is at a distance x from geometrical centre of bigger body....

The centre of mass of given system is at a distance x from geometrical centre of bigger body.

A

x = 0 or x > R

B

Centre of mass lies outside the bigger body

C

0 < x < R

D

Centre of mass lies within bigger body

E

None

Answer

0 < x < R

Explanation

Solution

The center of mass of a system can be calculated using the formula RCM=mirimi\vec{R}_{CM} = \frac{\sum m_i \vec{r}_i}{\sum m_i}. For a continuous body with mass density ρ(r)\rho(\vec{r}), the formula is RCM=rdmdm=rρ(r)dVρ(r)dV\vec{R}_{CM} = \frac{\int \vec{r} dm}{\int dm} = \frac{\int \vec{r} \rho(\vec{r}) dV}{\int \rho(\vec{r}) dV}.

When dealing with a body with a cavity, we can use the concept of negative mass. The system is treated as a complete body of positive mass minus the mass of the cavity. If the density is uniform, ρ=σ\rho = \sigma (mass per unit area for a thin disk).

Let the geometrical center of the bigger disk be the origin (0, 0). The radius of the bigger disk is R.

(I) Disk with one circular cavity: A circular cavity of radius r is removed, with its center at a distance d from the origin. The figure shows the cavity is off-center, so d>0d > 0. The cavity is inside the disk, so d+rRd+r \le R. Mass of the complete disk M=σπR2M = \sigma \pi R^2. Its center of mass is at (0, 0). Mass of the cavity m=σπr2m = \sigma \pi r^2. Its center of mass is at a position d\vec{d} from the origin, with d=d|\vec{d}| = d. The center of mass of the system with the cavity is XCM=M0mdMm=mdMm\vec{X}_{CM} = \frac{M \cdot \vec{0} - m \vec{d}}{M - m} = \frac{-m \vec{d}}{M - m}. The distance of the center of mass from the origin is x=XCM=mdMm=σπr2dσπR2σπr2=r2dR2r2x = |\vec{X}_{CM}| = \frac{m d}{M - m} = \frac{\sigma \pi r^2 d}{\sigma \pi R^2 - \sigma \pi r^2} = \frac{r^2 d}{R^2 - r^2}. Since the cavity is off-center, d>0d > 0, so x>0x > 0. Since the cavity is inside the disk, dRrd \le R-r. So xr2(Rr)R2r2=r2(Rr)(Rr)(R+r)=r2R+rx \le \frac{r^2 (R-r)}{R^2 - r^2} = \frac{r^2 (R-r)}{(R-r)(R+r)} = \frac{r^2}{R+r}. Since r<Rr < R, R+r>2rR+r > 2r, so r2R+r<r22r=r2\frac{r^2}{R+r} < \frac{r^2}{2r} = \frac{r}{2}. Also r<Rr < R. So x<Rx < R. Thus, for case (I), 0<x<R0 < x < R. This corresponds to option (R). Since x<Rx < R, the center of mass is within the bigger body, so it also corresponds to option (S). However, (R) is a more specific range for x.