
- A(R2 + R – 1) (2 – R) = 1
- B(R2 – R – 1) (2 – R) = 1
- C(R2 – R + 1) (2 – R) = 1
- D(R2 + R + 1) (2 – R) = 1
View written solutionFree
Correct answer: D
- Set up the geometry
Let the big sphere have:
- radius
- center
A smaller spherical cavity of radius is removed, with center .
From the figure/context, the cavity is internally tangent to the outer sphere, so the distance between centers is
The center of mass of the remaining body lies on the line and is given to be on the surface of the cavity.
Since the cavity surface is at distance from , and from the usual figure lies on the far side of from , we have Hence So the COM of the remaining part is at distance from .
- Use negative mass method
Treat the removed cavity as a sphere of negative mass.
Let density be .
Then
- mass of full sphere:
- mass of removed cavity:
So effectively, a mass is removed from point , whose distance from is .
Take as origin and positive direction toward . Then COM of remaining body is
= -\frac{m(R-1)}{M-m}.$$ Thus its distance from $C$ is $$CG = \frac{m(R-1)}{M-m}.$$ Substitute $M = mR^3$: $$CG = \frac{m(R-1)}{m(R^3-1)} = \frac{R-1}{R^3-1}.$$ But this is only the dimensionless fraction if cavity radius were scaled out incorrectly. Let us write it carefully including actual masses: Since $$M = kR^3,\qquad m=k$$ with $k=\frac{4}{3}\pi\rho$, we get $$CG = \frac{k(R-1)}{k(R^3-1)} = \frac{R-1}{R^3-1}.$$ This simplifies to $$CG = \frac{1}{R^2+R+1}.$$ This is the shift from $C$ toward the side opposite the cavity, so the point $G$ lies on the side away from $O$. Hence distance from $O$ to $G$ is $$OG = CO + CG = (R-1) + \frac{1}{R^2+R+1}.$$ Given that $G$ is on the cavity surface, $$OG = 1.$$ Therefore, $$(R-1) + \frac{1}{R^2+R+1} = 1.$$ So $$\frac{1}{R^2+R+1} = 2-R.$$ Rearranging, $$(R^2+R+1)(2-R)=1.$$ --- 3. **Match with options** This is exactly: $$\boxed{(R^2+R+1)(2-R)=1}$$ So the correct option is **D**. --- 4. **Comparison with stored answer** Stored correct answer: **D** Our derived answer: **D** They agree.More from Center of Mass
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