Is this triple integral between cylinder and a plane independent of $\pi$?

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Picture of full problem where Dan's share is part of interest:

Picture of full problem where Dan's share is part of interest

The image shows the full problem. The issue is raised when calculating Dan's share of the drink.

(1) Equation of plane in Dan's share must pass through $(x,y,z)=(0,0,0)\space and\space (0,R,h)$. Therefore the CARTESIAN equation of the plane is: $$ z=\frac{hy}{R}$$ and the cylindrical equation is: $$z=\frac{h}{R}r\sin\theta$$

(2) The jacobian in cyldindrical coordinates is $r$, therfoe the volume element is: $$dA=r dr d\theta dz$$

(3) The limits of Dan's portion in cylindrical coordinates are: $$z: 0 \rightarrow \frac{h}{R}r\sin\theta \hspace{0.5cm}\vert\hspace{0.5cm} \theta: 0\rightarrow \pi \hspace{0.5cm}\vert\hspace{0.5cm} r:0\rightarrow R $$

(4)The triple integral for Dan's share is therefore:

$$\LARGE \int_{0}^{R}\int_{0}^{\pi}\int_{0}^{\frac{hr\sin\theta}{R}}r\,\, dz d\theta dr$$

(5) Evaluating: $$\large \int_{0}^{R}\int_{0}^{\pi}\frac{h\sin\theta}{R}r^{2}\,\, d\theta dr$$

$$\large \int_{0}^{R}\left[\frac{-h}{R}r^{2}\cos\theta\right]_{0}^{\pi}\,\, dr$$ $$\large \int_{0}^{R}\frac{2h}{R}r^{2}\,\, dr$$

(6) Final answer is therefore : $$\LARGE \frac{2}{3}hR^{2}$$

This seems very odd to me as a semicircular based shaped has a volume that is independent of $\pi$. Is this true or have I made a mistake?

A related question is why does this shape not count as a pyramid? It has a shape that goes to a point. I thought that was the condition for a pyramid. But that would mean the area should be $\frac{1}{6}\pi R^{2}$.

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Let us calculate the volume of the body in a more straightforward (but by no means a better) way:

Consider horizontal slices of the body. They are circular segments with the area ($\phi$ is one half of $\theta$ from the wikipedia page): $$ A_\phi =R^2\left(\phi-\sin\phi\cos\phi\right), $$ with $\cos\phi=y/R=z/h$.

Therefore: $$ V=\int_0^h A_{\phi(z)}dz=R^2h\int_0^{\pi/2} \left(\phi-\sin\phi\cos\phi\right)\sin\phi\, d\phi\\=R^2h\left[\sin\phi-\phi\cos\phi-\frac{1}{3}\sin^3\phi\right]_0^{\pi/2}=\frac{2}{3}R^2h. $$ This confirms the correctness of the result.