Volume of Paraboloid
Theorem
The volume of paraboloid is half the volume of its circumscribing cylinder.
Proof
This article needs to be linked to other articles. You can help $\mathsf{Pr} \infty \mathsf{fWiki}$ by adding these links. To discuss this page in more detail, feel free to use the talk page. When this work has been completed, you may remove this instance of {{MissingLinks}} from the code. |
Consider acylinder of radius $r$ and height $h$, circumscribing a paraboloid $y= h \paren {\dfrac x r}^2$ whose apex is at the center of the bottom base of the cylinder and whose base is the top base of the cylinder.
Also consider the paraboloid $y = h - h \paren {\dfrac x r}^2$, with equal dimensions but with its apex and base flipped.
For every height $0 \le y \le h$, the disk-shaped cross-sectional area $\pi \paren {r \sqrt {1 - \dfrac y h} }^2$ of the flipped paraboloid is equal to the ring-shaped cross-sectional area $\pi r^2 - \pi r^2 \paren {\sqrt {\dfrac y h} }^2$ of the cylinder part outside the inscribed paraboloid.
Indeed:
\(\ds \pi \paren {r \sqrt {1 - \dfrac y h} }^2\) | \(=\) | \(\ds \pi r^2 \paren {\sqrt {1 - \dfrac y h} }^2\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \pi r^2 \paren {1 - \dfrac y h}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \pi r^2 - \pi r^2 \dfrac y h\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \pi r^2 - \pi r^2 \paren {\sqrt {\dfrac y h} }^2\) |
There is believed to be a mistake here, possibly a typo. In particular: discrepancy You can help $\mathsf{Pr} \infty \mathsf{fWiki}$ by reviewing it, and either correcting it or adding some explanatory material as to why you believe it is actually correct after all. To discuss this page in more detail, feel free to use the talk page. When this work has been completed, you may remove this instance of {{Mistake}} from the code.If you would welcome a second opinion as to whether your work is correct, add a call to {{Proofread}} the page. |
Therefore, the volume of the flipped paraboloid is equal to the volume of the cylinder part outside the inscribed paraboloid.
In other words, the volume of the paraboloid is $\dfrac \pi 2 r^2 h$, half the volume of its circumscribing cylinder.
This theorem requires a proof. You can help $\mathsf{Pr} \infty \mathsf{fWiki}$ by crafting such a proof. To discuss this page in more detail, feel free to use the talk page. When this work has been completed, you may remove this instance of {{ProofWanted}} from the code.If you would welcome a second opinion as to whether your work is correct, add a call to {{Proofread}} the page. |