Center of mass of spherical shell inside of cone (Apostol Problem).

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Homework Statement
A homogenous spherical shell of radius ##a## is cut by one nappe of a right circular cone whose vertex is at the center of the sphere. If the vertex angle of the cone is ##\alpha##, where ##0<\alpha<\pi##, determine (in terms of ##a## and ##\alpha## the center of mass of the portion of the spherical shell that lies inside the cone.
Relevant Equations
##\iint_S f(x,y,z)dS##
I am asking this question because my solution does not seem to match the solution at the end of the book (Apostol Vol II, section 12.10, problem 9).

Here is my attempt to solve this problem.

If our coordinate system is chosen such that the z-axis lines up with the axis of the cone then by symmetry the ##x## and ##y## coordinates of the center of mass will both be zero.

All that is left is to calculate the z-coordinate of the center of mass.

Using spherical coordinates, the cone is ##\theta=\alpha/2## and the sphere is ##\rho=a##.

The parameterized equation for the sphere is ##\vec{r}=\langle a\sin{\theta}\cos{\phi}, a\sin{\theta}\sin{\phi}a\cos{\theta}\rangle##.

The portion inside the cone is the red area below

1698899239437.png


Just to be clear about the coordinate system, I am using spherical coordinates defined as follows

1698899257952.png


Now, the spherical shell has a constant density of ##d(x,y,z)=\frac{M}{4\pi a^2}##.

Let's define ##f(x,y,z)=z\cdot d(x,y,z)##.

Then our calculation of ##z_{cm}## is

$$z_{cm}=\frac{\int\int_S f(x,y,z) dS}{\int\int_S d(x,y,z)dS}$$

$$=\frac{\int\int_S f(\vec{r}(\theta,\phi))\cdot \lVert \frac{d\vec{r}}{d\theta}\times\frac{d\vec{r}}{d\phi} \rVert d\theta d\phi}{\int\int_S d(\vec{r}(\theta,\phi)) \lVert \frac{d\vec{r}}{d\theta}\times\frac{d\vec{r}}{d\phi} \rVert d\theta d\phi}$$

The denominator is

$$\frac{M}{4\pi a^2}\int_0^{2\pi}\int_0^{\alpha/2} a^2\sin{\theta}d\theta d\phi$$

$$=\frac{M(1-\cos{(\alpha/2)}}{2}$$

And the numerator is

$$\frac{M}{4\pi a^2}a^3\int_0^{2\pi}\int_0^{\alpha/2} \sin{\theta}\cos{\theta} d\theta d\phi$$

$$=\frac{Ma\sin^2{(\alpha/2)}}{4}$$

Thus when we put numerator and denominator together we get

$$\frac{\frac{Ma\sin^2{(\alpha/2)}}{4}}{\frac{M(1-\cos{(\alpha/2)}}{2}}$$

$$=\frac{a\sin^2{(\alpha/2)}}{2(1-\cos{(\alpha/2)})}$$

However, it seems that either I have made a mistake or the solutions manual is wrong, because they have the answer

On the axis of the cone, at a distance ##\frac{1}{4}a\frac{1-\cos{\alpha}}{1-\cos{(\alpha/2)}}## from the center of the sphere.
 
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Are you familiar with the formula for the cosine of a double angle ##\cos(2x) = \ldots##?
 
Orodruin said:
Are you familiar with the formula for the cosine of a double angle ##\cos(2x) = \ldots##?
Ah yes, that is indeed the solution to my woes.

1698903446829.png
 
I will say that your expression looks tidier. The given expression likely originated from using that ##\sin(\theta)\cos(\theta) = \sin(2\theta)/2## before integration.
 
There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
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