add images to platonic-volume
BIN
posts/misc/platonic-volume/cube_pyramids.png
Normal file
|
After Width: | Height: | Size: 165 KiB |
BIN
posts/misc/platonic-volume/equilateral_center.png
Normal file
|
After Width: | Height: | Size: 236 KiB |
BIN
posts/misc/platonic-volume/incenter_area.png
Normal file
|
After Width: | Height: | Size: 134 KiB |
@ -5,12 +5,20 @@ description: |
|
||||
format:
|
||||
html:
|
||||
html-math-method: katex
|
||||
date: "TODO"
|
||||
date-modified: "2025-06-03"
|
||||
date: "2021-07-25"
|
||||
date-modified: "2025-06-13"
|
||||
categories:
|
||||
- geometry
|
||||
---
|
||||
|
||||
<style>
|
||||
.figure-img {
|
||||
max-width: 512px;
|
||||
object-fit: contain;
|
||||
height: 100%;
|
||||
}
|
||||
</style>
|
||||
|
||||
|
||||
The Platonic solids have been known for millennia.
|
||||
They bear the name of Plato, who spoke of them in his dialogue *Timaeus*.
|
||||
@ -27,19 +35,18 @@ While surface area may be troublesome in the case of the dodecahedron
|
||||
and for trigonometry students to calculate for the solids composed of equilateral triangles.
|
||||
On the other hand, the volume is somewhat mystical.
|
||||
|
||||
The volume itself is a meaningless quantity for comparison unless put in ratio with another volume.
|
||||
Fortunately, edge length is the only free variable in a Platonic solid,
|
||||
meaning their volumes can be parametrized by this value alone.
|
||||
Further, since the cube has such simple expression for its volume (the edge length cubed),
|
||||
it is a natural choice as a base for the comparison[^1].
|
||||
Therefore, I will derive this ratio for the solids in question.
|
||||
The volume itself is a meaningless quantity for comparison unless put in ratio with another volume,
|
||||
but since the cube has such simple expression for its volume (the edge length cubed),
|
||||
it is a natural choice for this comparison[^1].
|
||||
|
||||
[^1]: Though this is a pure mathematical concept, empirical units use the same convention.
|
||||
For instance, a cubic centimeter is defined as the volume occupied by a cube which is a
|
||||
centimeter long in each dimension, despite being applicable to volumes of any shape.
|
||||
|
||||
This post will calculate the volume without using any trigonometric functions (sine, cosine, tangent),
|
||||
and instead opts for a more compass-and-straightedge approach.
|
||||
This post will calculate this ratio without using any trigonometric functions (sine, cosine, tangent),
|
||||
instead opting for a more compass-and-straightedge approach.
|
||||
Consequently, it becomes more natural to calculate the *square* of the volume to better cooperate
|
||||
with the Pythagorean theorem.
|
||||
|
||||
@ -62,21 +69,21 @@ There are [many centers of a triangle](https://faculty.evansville.edu/ck6/encycl
|
||||
- The distance from a vertex to the circumcenter is called the *circumradius* (*c*).
|
||||
- The *incenter* is equidistant from every edge.
|
||||
It is the center of a circle which lies tangent to every edge
|
||||
(i.e., radii can be drawn which are are perpendicular to the edge).
|
||||
- It is constructed by finding the intersection of the lines which bisect each angle.
|
||||
- It can be constructed by finding the intersection of the lines which bisect each angle.
|
||||
- The perpendicular distance from an edge to the incenter is called the *inradius* (*a*).
|
||||
|
||||
::: {}
|
||||

|
||||

|
||||
|
||||
Constructing the circumcenter and incenter.
|
||||
Angle bisectors in blue, perpendicular bisectors in red, in- and circumradii in green.
|
||||
:::
|
||||
|
||||
The inradius is special because it is also an altitude for a triangle formed by the inradius and an edge of the larger triangle.
|
||||
The inradius is special because it is also an altitude for a triangle formed by the inradius and
|
||||
an edge of the larger triangle.
|
||||
This means that the area of the larger triangle is the sum of these smaller triangles.
|
||||
|
||||

|
||||

|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
@ -95,7 +102,9 @@ In fact, the bisection of an angle involves constructing a rhombus, which is mad
|
||||
In this case, the inradius is also called the *apothem*, and the difference between it and the circumradius
|
||||
is immediately apparent and called the *sagitta* (*s*).
|
||||
|
||||

|
||||

|
||||
|
||||
This idea of incenters and circumcenters can be extended to other 2D figures
|
||||
such as the square and regular pentagon.
|
||||
@ -104,7 +113,7 @@ The pentagon is trickier and will be discussed later.
|
||||
Regardless, the expression for the area ${Pa \over 2}$ still works,
|
||||
since the polygon can be triangulated through the center in a similar way.
|
||||
|
||||

|
||||

|
||||
|
||||
|
||||
### Cubes, Prisms, and Pyramids
|
||||
@ -129,12 +138,12 @@ Connecting all other bases to this point produces five pyramids, whose bases all
|
||||
Designate these pyramids as "bottom", "left", "right", "front", and "back",
|
||||
where left and right correspond to *x* and front and back correspond to *y*.
|
||||
|
||||

|
||||

|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
V_\text{cube}
|
||||
&= Bh = V_\text{bottom} + V_\text{left} + V_\text{right} V_\text{front} + V_\text{back}
|
||||
&= Bh = V_\text{bottom} + V_\text{left} + V_\text{right} + V_\text{front} + V_\text{back}
|
||||
\\
|
||||
&= rBh + rBx + rB(h-x) + rBy + rB(h-y)
|
||||
\\
|
||||
@ -149,82 +158,88 @@ This can be generalized to a pyramid based on any prism, where the top point lie
|
||||
However, this is beyond the scope of this post.
|
||||
|
||||
|
||||
### Simplifying Units
|
||||
|
||||
Though it may make sense to use unit lengths for the edges of 3D figures, bisection of edges
|
||||
is easier if the edges are composed of two units.
|
||||
This happens to coincide with Plato's description -- the equilateral triangle is described as
|
||||
being formed from two 30-60-90 triangles.
|
||||
That is, the edge length of the equilateral triangle was twice the "unit" length:
|
||||
the shortest side of the 30-60-90 triangle.
|
||||
|
||||
Thus, ratios to the volume of the *unit* cube must be adjusted by a factor of 8:
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
{ V_\text{solid}[2] \over V_\text{cube}[2] }
|
||||
&= { V_\text{solid}[1] \over V_\text{cube}[1] }
|
||||
\\
|
||||
\implies V_\text{solid}[2]
|
||||
&= { V_\text{cube}[2] \over V_\text{cube}[1] } V_\text{solid}[1]
|
||||
\\
|
||||
&= { 2^3 \over 1 } V_\text{solid}[1]
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
|
||||
Simple Solids: the Octahedron and the Tetrahedron
|
||||
-------------------------------------------------
|
||||
|
||||
While "simple" is a bit of a misnomer, their volumes are easiest to appreciate,
|
||||
since they do not need regular pentagons.
|
||||
While "simple" is a bit of a misnomer, their volumes do not require regular pentagons,
|
||||
and are therefore easiest to appreciate.
|
||||
|
||||
|
||||
### Octahedron
|
||||
|
||||
The octahedron can be thought of as two square pyramids joined end-on-end,
|
||||
with uniform edge length throughout.
|
||||
Since the base is a square, its center is equidistant from the vertices of the base.
|
||||
An alternative, congruent square can be noticed by the symmetry of the octahedron,
|
||||
meaning the center is also equidistant from the top of the square pyramid,
|
||||
and that the segment connecting the two is an altitude of the pyramid.
|
||||
Since the base of the pyramid is a square, its center is equidistant from the vertices of the base.
|
||||
Due to the symmetry of the octahedron, this center is the same no matter which square we pick.
|
||||
Thus, the altitude *h* of the square pyramid is simply half of the diagonal of the square.
|
||||
|
||||
::: {}
|
||||

|
||||
$$
|
||||
(2h)^2 = e^2 + e^2 = 2 \cdot 2^2 = 2^3
|
||||
$$
|
||||
|
||||
Primary square in blue, secondary square in red. Diagonals of both squares shown.
|
||||
:::
|
||||

|
||||
|
||||
The length of this altitude is simply half of the diagonal of the square.
|
||||
Therefore, the volume of an octahedron (calculated using edge length 1) is:
|
||||
Therefore, the volume of an octahedron is:
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
B^2
|
||||
&= (1^2)^2
|
||||
&= (e^2)^2
|
||||
= (2^2)^2 = 2^4
|
||||
\\
|
||||
(2h)^2
|
||||
&= 4h^2 = 1^2 + 1^2 = 2
|
||||
(2 V_\text{sq.pyr.})^2
|
||||
&= (2^2) \left( {B^2 h^2 \over 3^2} \right)
|
||||
= {B^2 (2h^2) \over 3^2}
|
||||
= {{2^4 \cdot 2^3} \over 3^2}
|
||||
= {2^7 \over 3^2}
|
||||
\\
|
||||
V_\text{sq.pyr.}^2
|
||||
&= {B^2 h^2 \over 3^2} = {1 \cdot {2 / 4} \over 3^2}
|
||||
(2^3 \cdot V_\text{oct})^2
|
||||
&= {2^7 \over 3^2}
|
||||
\implies V_\text{oct}^2
|
||||
= {2 \over 3^2}
|
||||
\\
|
||||
(1^3 \cdot V_\text{oct})^2
|
||||
&= (2V_\text{sq.pyr})^2 = 4V_\text{sq.pyr}^2
|
||||
= 4 \cdot {2 / 4 \over 3^2} = {2 \over 3^2}
|
||||
\\ \\
|
||||
V_\text{oct} &= {\sqrt{2} \over 3}
|
||||
V_\text{oct}
|
||||
&= {\sqrt{2} \over 3}
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
|
||||
### Tetrahedron
|
||||
|
||||
From here on out, it becomes convenient to specify the edge length of every solid to be 2,
|
||||
since this simplifies the bisection of edges.
|
||||
This happens to coincide with Plato's description, where the equilateral triangle is described as
|
||||
being formed from two 30-60-90 triangles.
|
||||
That is, the edge length of the equilateral triangle was twice the "unit" length: the shortest side of the 30-60-90 triangle.
|
||||
|
||||
However, we must remember that volumes need to be put in ratio with a cube volume of 8:
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
{ V_\text{solid[2]} \over V_\text{cube[2]} }
|
||||
&= { V_\text{solid[1]} \over V_\text{cube[1]} }
|
||||
\\
|
||||
\implies V_\text{solid[2]}
|
||||
&= { V_\text{cube[2]} \over V_\text{cube[1]} } V_\text{solid[1]}
|
||||
\\
|
||||
&= { 2^3 \over 1 } V_\text{solid[1]}
|
||||
$$
|
||||
|
||||
Since the tetrahedron is itself a pyramid, its volume follows from the earlier formula.
|
||||
First, we must calculate the (square of the) area of the base of an equilateral triangle.
|
||||
|
||||
:::: {layout-ncol="2"}
|
||||
:::: {layout-ncol="2" layout-valign="center"}
|
||||
|
||||
::: {.column width="49%"}
|
||||

|
||||
:::
|
||||

|
||||
|
||||
::: {.column width="49%"}
|
||||
::: {.column}
|
||||
$$
|
||||
\begin{align*}
|
||||
d_\text{altitude}^2
|
||||
@ -243,13 +258,11 @@ Next, bisect this triangle through any edge, then use it to bisect the tetrahedr
|
||||
This forms an isosceles triangle containing an edge and the altitudes of two faces.
|
||||
Bisecting the angle where the two alittudes meet (perpendicularly) bisects the edge.
|
||||
|
||||
:::: {layout-ncol="2"}
|
||||
:::: {layout-ncol="2" layout-valign="center"}
|
||||
|
||||
::: {.column width="49%"}
|
||||

|
||||
:::
|
||||

|
||||
|
||||
::: {.column width="49%"}
|
||||
::: {.column}
|
||||
$$
|
||||
\begin{align*}
|
||||
\textcolor{blue}{d_\text{length}}^2
|
||||
@ -270,13 +283,14 @@ $$
|
||||
Since *h* is known, we can calculate the volume.
|
||||
|
||||
$$
|
||||
({ 2^3 \cdot V_\text{tet[1]} })^2
|
||||
\begin{align*}
|
||||
({ 2^3 \cdot V_\text{tet} })^2
|
||||
&= {B^2 h^2 \over 3^2} = {3 \cdot (8/3) \over 3^2}
|
||||
\\
|
||||
V_\text{tet[1]}^2
|
||||
V_\text{tet}^2
|
||||
&= {8 \over 2^6 \cdot 3^2} = {1 \over 2^3 \cdot 3^2} = {1 \over 2 \cdot 6^2}
|
||||
\\
|
||||
V_\text{tet[1]}
|
||||
V_\text{tet}
|
||||
&= \sqrt{1 \over 6^2 \cdot 2} = {1 \over 6\sqrt 2}
|
||||
\end{align*}
|
||||
$$
|
||||
@ -297,19 +311,19 @@ Since the diagonal is parallel to one of the sides, a parallelogram can be forme
|
||||
More specifically, this parallelogram is a rhombus, since the segments must have equal lengths
|
||||
to the sides.
|
||||
|
||||
::: {}
|
||||

|
||||
|
||||
Left: Pentagram in regular pentagon;
|
||||
Middle: Isosceles trapezoid, with parallel lines marked in blue;
|
||||
Right: Rhombus in regular pentagon
|
||||
:::
|
||||

|
||||
|
||||
Bisect the pentagon vertically and let the length of half of the diagonal of a pentagon be *d*,
|
||||
half the length of the other diagonal of a rhombus be *h*,
|
||||
and the remaining height of the pentagon be *g*.
|
||||
|
||||

|
||||

|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
@ -326,7 +340,7 @@ $$
|
||||
Notice that the center of a pentagram contains a regular pentagon.
|
||||
This means that the ratio of its height to the side is equal to the ratio of
|
||||
the larger pentagon's height to its side.
|
||||
This is enough information to deduce *d*:
|
||||
This gives us enough information to deduce *d*:
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
@ -342,74 +356,78 @@ $$
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
This is the minimal polynomial of the golden ratio *φ*.
|
||||
The (positive) quantity satisfying this polynomial is the golden ratio *φ*.
|
||||
It is half the length of the diagonal, so the ratio of a diagonal to a side is also *φ*.
|
||||
|
||||
To make calculations easier, some conversions will be made to base *φ*, or phinary.
|
||||
If you are not familiar already with phinary, I have already written at length about it [here](
|
||||
/posts/polycount/1
|
||||
).
|
||||
Finally, the apothem *a* and height *l* can be calculated by similar triangles.
|
||||
|
||||
::: {}
|
||||

|
||||
:::
|
||||
To calculate the apothem, we can calculate the sagitta *s* and height *l* by similar triangles.
|
||||
|
||||

|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
\textcolor{blue}{c \over a}
|
||||
&= \textcolor{brown}{2 \over \phi},~ a^2 + 1^2 = c^2
|
||||
\implies 1 = c^2 -\ a^2 = (c + a)(c -\ a)
|
||||
&\textcolor{blue}{c \over a}
|
||||
= \textcolor{brown}{2 \over \phi}
|
||||
\\
|
||||
l
|
||||
&= c + a = {2a \over \phi} + a = a{2 + \phi \over \phi}
|
||||
l &= c + a = {2a \over \phi} + a = a{2 + \phi \over \phi}
|
||||
= a{12_\phi \over 10_\phi}
|
||||
= a{2\bar{1}0_\phi \over 10_\phi} = a(2\bar{1}_\phi)
|
||||
\\ \\
|
||||
s
|
||||
&= c -\ a = {2a \over \phi} -\ a
|
||||
\\
|
||||
s &= c -\ a = {2a \over \phi} -\ a
|
||||
= a{2 -\ \phi \over \phi} = a{\bar{1}2_\phi \over 10_\phi}
|
||||
= a{2\bar{3}0_\phi \over 10_\phi} = a(2\bar{3}_\phi)
|
||||
\\ \\ \\
|
||||
1
|
||||
&= ls = a^2(2\bar{1}_\phi)(2\bar{3}_\phi)
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
Finally, the Pythagorean theorem tells us that the product of these quantities is 1,
|
||||
allowing us to calculate *a*.
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
1 &= c^2 -\ a^2 = (c + a)(c -\ a) = ls
|
||||
\\
|
||||
&= a^2(2\bar{1}_\phi)(2\bar{3}_\phi)
|
||||
= a^2(4\bar{8}3_\phi)
|
||||
= a^2(\bar{4}7_\phi) = a^2(3.\bar{4}_\phi)
|
||||
\\
|
||||
a^2
|
||||
&= {1 \over 3.\bar{4}_\phi} \cdot {43_\phi \over 43_\phi}
|
||||
a^2 &= {1 \over 3.\bar{4}_\phi} \cdot {43_\phi \over 43_\phi}
|
||||
= {43_\phi \over [12]\bar{7}.[\bar{12}]_\phi}
|
||||
= {3 + 4\phi \over 5}
|
||||
\\ \\
|
||||
\implies l^2
|
||||
&= a^2(2\bar{1}_\phi)^2
|
||||
\\
|
||||
\implies l^2 &= a^2(2\bar{1}_\phi)^2
|
||||
= {3 + 4\phi \over 5} \cdot (4\bar{4}1_\phi)
|
||||
= {3 + 4\phi \over 5} \cdot 5 = 3 + 4\phi
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
The last few steps in solving for $a^2$ are somewhat tricky.
|
||||
The conjugate of *φ* is $-{1 \over \phi}$.
|
||||
Since the digit in the *φ*^^-1^^ place value is negative, its conjugate has a positive value in the *φ* place value,
|
||||
i.e., $3.\bar{4}_{\phi^*} = 43_\phi$.
|
||||
The conjugate of *φ* is $\varphi^* = -{1 \over \varphi}$.
|
||||
Since the digit in the *φ*^-1^ place value is negative, its conjugate has a positive value in the *φ* place value,
|
||||
i.e., $3.\bar{4}_{\varphi^*} = 43_\varphi$.
|
||||
Multiplying a quadratic root by its conjugate produces an integer value,
|
||||
which means that the scary quantity $[12]\bar{7}.[\bar{12}]_\phi$ resolves cleanly to 5.
|
||||
which means that the scary quantity $[12]\bar{7}.[\bar{12}]_\varphi$ resolves cleanly to 5.
|
||||
|
||||
The division can also be done explicitly in phinary:
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
{1 \over 3.\bar{4}_\phi}
|
||||
&= {1 \over 0.\bar{1}3_\phi}
|
||||
= {500_\phi \over 5 (\bar{1}3_\phi)}
|
||||
= {233_\phi + (0 = \textcolor{red}{4\bar{4}}\bar{4}0_\phi
|
||||
= \textcolor{red}{26\bar{2}}\bar{4}0_\phi) \over 5 (\bar{1}3_\phi)}
|
||||
{1 \over 3.\bar{4}_\varphi}
|
||||
&= {1 \over 0.\bar{1}3_\varphi}
|
||||
= {500_\varphi \over 5 (\bar{1}3_\varphi)}
|
||||
= {233_\varphi + (0 = \textcolor{red}{4\bar{4}}\bar{4}0_\varphi
|
||||
= \textcolor{red}{26\bar{2}}\bar{4}0_\varphi) \over 5 (\bar{1}3_\varphi)}
|
||||
\\
|
||||
&= {\bar{2}60\bar{1}3_\phi \over 5 (\bar{1}3_\phi)}
|
||||
= {2001_\phi \over 5}
|
||||
= {221_\phi \over 5}
|
||||
= {43_\phi \over 5}
|
||||
= {3 + 4\phi \over 5}
|
||||
&= {\bar{2}60\bar{1}3_\varphi \over 5 (\bar{1}3_\varphi)}
|
||||
= {2001_\varphi \over 5}
|
||||
= {221_\varphi \over 5}
|
||||
= {43_\varphi \over 5}
|
||||
= {3 + 4\varphi \over 5}
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
@ -419,7 +437,6 @@ The Remaining Solids
|
||||
|
||||
With the diagonal length and apothem of a regular pentagon in tow, the geometry of
|
||||
the final two solids may be explored.
|
||||
As a reminder, these solids will have edge length 2, so they will be put in ratio with a cube volume of 8.
|
||||
|
||||
The icosahedron and dodecahedron are easiest to dissect as many pyramids joined to a single center.
|
||||
This is reminiscent of the area formula which uses the triangulation of a regular polygon its center.
|
||||
@ -433,47 +450,44 @@ These will become important shortly.
|
||||
|
||||
### The Icosahedron: an Antiprism in Profile
|
||||
|
||||
The icosahedron may also be thought of as two pentagonal pyramids connected to
|
||||
The icosahedron can be decomposed into two pentagonal pyramids connected to
|
||||
either base of a pentagonal *antiprism*.
|
||||
An antiprism is a figure similar to a prism, but with the one of the bases twisted relative
|
||||
to the other and with (equilateral) triangles joining them.
|
||||
|
||||
:::: {layout-ncol="2"}
|
||||
|
||||
::: {.column width="49%"}
|
||||

|
||||
|
||||
Icosahedron with pentagonal antiprism in blue
|
||||
:::
|
||||
|
||||
::: {.column width="49%"}
|
||||

|
||||
|
||||
Construction showing $2a = c$
|
||||
:::
|
||||
|
||||
::::
|
||||
|
||||
A segment connecting the centers of two antipodal faces is a diameter of the insphere.
|
||||
The altitude of one of these faces will be cut into circumradius and inradius.
|
||||
By similar triangles, the circumradius of an equilateral triangle is
|
||||
exactly twice the length of the inradius.
|
||||
This means the inradius is 1/3 of the altitude, or 1/9 of the square of the altitude.
|
||||
With edge length 2, the square of the altitude is 3, so the square of the inradius is
|
||||
${3 \over 9} = {1 \over 3}$ .
|
||||

|
||||
|
||||
The pentagonal antiprism may be bisected bisected along the plane containing the altitudes
|
||||
of two triangles opposite one another.
|
||||
of two antipodal triangles.
|
||||
This forms a parallelogram with side lengths of the altitude of an equilateral triangle
|
||||
and height of a pentagon.
|
||||
and height of a pentagon (*l*).
|
||||
|
||||

|
||||
A segment connecting the centers of two antipodal faces is a diameter of the insphere (2*h*).
|
||||
This diameter can be translated along the parallelogram by *a*, the apothem of an equilateral trangle.
|
||||
This forms a right triangle with *a* and 2*h* as legs and *l* as the hypotenuse.
|
||||
|
||||
::: {layout-ncol="2" layout-valign="center"}
|
||||

|
||||
|
||||

|
||||
:::
|
||||
|
||||
For an edge length of 2, we know from the tetrahedron that $d_{altitude}^2 = (a + c)^2 = 3$.
|
||||
From the above construction, $(3a)^2 = 3 \implies a^2 = 1 / 3$.
|
||||
So,
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
(\textcolor{green}{2h})^2
|
||||
&= \textcolor{red}{l}^2 -\ {1 \over 3}
|
||||
= 3 + 4\phi -\ {1 \over 3}
|
||||
&= \textcolor{red}{l}^2 - a^2
|
||||
= \textcolor{red}{3 + 4\phi}
|
||||
-\ {1 \over 3}
|
||||
= {3(3 + 4\phi) -\ 1 \over 3}
|
||||
\\
|
||||
h^2
|
||||
@ -484,17 +498,23 @@ $$
|
||||
32_\phi
|
||||
&= 210_\phi = 1100_\phi = 10000_\phi
|
||||
= \phi^4
|
||||
\\ \\
|
||||
(2^3 \cdot V_\text{ico[1]})^2
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
With the inradius in tow, we can calculate the volume of the icosahedron.
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
(2^3 \cdot V_\text{ico})^2
|
||||
&= \left ( 20 \cdot {Bh \over 3} \right )^2
|
||||
= {20^2 B^2 h^2 \over 3^2} = {5^2 \cdot 4^2 \cdot 3 \cdot {\phi^4 \over 3} \over 3^2}
|
||||
= {5^2 \cdot 2^4 \cdot \phi^4 \over 3^2}
|
||||
\\
|
||||
V^2
|
||||
V_\text{ico}^2
|
||||
&= {5^2 \cdot 2^4 \cdot \phi^4 \over 2^6 \cdot 3^2}
|
||||
= {5^2 \cdot \phi^4 \over 2^2 \cdot 3^2}
|
||||
\\
|
||||
V &= {5 \phi^2 \over 6}
|
||||
V_\text{ico} &= {5 \phi^2 \over 6}
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
@ -503,31 +523,40 @@ $$
|
||||
|
||||
The dodecahedron is a bit trickier.
|
||||
It belongs to a class of polyhedra known as *truncated trapezohedra*.
|
||||
However, the bisection trick from the icosahedron still works.
|
||||
|
||||
The bisection trick from the icosahedron mostly still works.
|
||||
Begin by bisecting the solid through antipodal altitudes.
|
||||
This produces an oblong hexagon made up of four pentagon heights and two edges.
|
||||
|
||||

|
||||

|
||||
|
||||
The segment connecting the antipodal midpoints bisects the hexagon into two (isosceles) trapezoids,
|
||||
and is a diameter of the midsphere.
|
||||
Additionally, it is parallel to the two edges. A second midradius is perpendicular to this one,
|
||||
bisecting the trapezoid.
|
||||
It is parallel to the two edges, so dropping an altitude from this edge to the diameter
|
||||
produces a midradius.
|
||||
|
||||

|
||||

|
||||
|
||||
The inradius is the altitude of a triangle formed by the length of a pentagon (its base),
|
||||
The inradius *h* is the altitude of a triangle formed by the length of a pentagon (its base),
|
||||
a midradius, and a circumradius.
|
||||
However, the altitude with respect to the midradius is another midradius.
|
||||
This means that the height can be found by equating areas and completing the square.
|
||||
The inradius meets the pentagon at its center, so we can use its apothem to relate
|
||||
the inradius and midradius.
|
||||
|
||||
$$
|
||||
a^2 + \textcolor{green}{h}^2 = \textcolor{blue}{\rho}^2
|
||||
$$
|
||||
|
||||
From the trapezoid, we know that the altitude with respect to the midradius is another midradius.
|
||||
This means that the height can be found by equating areas.
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
a^2 + \textcolor{green}{h}^2
|
||||
&= \textcolor{blue}{\rho}^2,~~
|
||||
\textcolor{orange}{l}\textcolor{green}{h}
|
||||
= \textcolor{blue}{\rho \rho} \implies \textcolor{orange}{l}^2\textcolor{green}{h}^2
|
||||
\textcolor{orange}{l}\textcolor{green}{h}
|
||||
&= \textcolor{blue}{\rho \rho} \implies \textcolor{orange}{l}^2\textcolor{green}{h}^2
|
||||
= (\textcolor{orange}{(2\bar{1}_\phi) a})^2 h^2
|
||||
= 5a^2h^2
|
||||
= \textcolor{blue}{\rho}^4
|
||||
@ -535,28 +564,32 @@ $$
|
||||
5a^2h^2
|
||||
&= (a^2 + h^2)^2
|
||||
= a^4 + 2a^2h^2 + h^4
|
||||
\\ \\
|
||||
0
|
||||
&= a^4 -\ 3a^2h^2 + h^4
|
||||
= (h^2 -\ x)^2 + y
|
||||
= h^4 -\ 2xh^2 + x^2 + y
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
All terms in this polynomial are square, so we can solve for *h* in terms of *a* by completing the square.
|
||||
Note that *x* and *y* are auxiliary terms in this process.
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
0 &= h^4 -\ 3a^2h^2 + a^4
|
||||
= (h^2 -\ x)^2 - y^2
|
||||
\\
|
||||
-2x
|
||||
&= -3a^2
|
||||
\implies x = {3a^2 \over 2},~~
|
||||
x^2 + y = {9a^4 \over 4} + y = a^4
|
||||
&= h^4 -\ 2xh^2 + x^2 - y^2
|
||||
\\
|
||||
y
|
||||
&= {4a^4 \over 4} -\ {9a^4 \over 4} = -{5a^4 \over 4}
|
||||
= -{(2\bar{1}_\phi)^2 a^4 \over 4}
|
||||
= -\left ( {(2\bar{1}_\phi) a^2 \over 2} \right )^2
|
||||
\\ \\
|
||||
(h^2 -\ {3a^2 \over 2})^2
|
||||
&= -y
|
||||
-2x &= -3a^2
|
||||
\implies x = {3a^2 \over 2}
|
||||
\\
|
||||
x^2 - y^2 &= {9a^4 \over 4} - y^2 = a^4
|
||||
\\
|
||||
\implies y^2 &= {9a^4 \over 4} - {4a^4 \over 4}
|
||||
= {5a^4 \over 4}
|
||||
= {(2\bar{1}_\phi)^2 a^4 \over 4}
|
||||
= \left ( {(2\bar{1}_\phi) a^2 \over 2} \right )^2
|
||||
\\
|
||||
\\ \\
|
||||
h^2 -\ {3a^2 \over 2}
|
||||
&= {(2\bar{1}_\phi) a^2 \over 2}
|
||||
&= y
|
||||
= {(2\bar{1}_\phi) a^2 \over 2}
|
||||
\\
|
||||
h^2
|
||||
&= {(2\bar{1}_\phi) a^2 \over 2} + {3a^2 \over 2}
|
||||
@ -568,7 +601,7 @@ $$
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
With the square of the height known, all that is left to do is find the volume.
|
||||
With the square of the inradius known, all that is left to do is find the volume.
|
||||
|
||||
$$
|
||||
\begin{align*}
|
||||
@ -580,15 +613,15 @@ $$
|
||||
&= [11]7_\phi = 740_\phi = 4300_\phi
|
||||
= (43_\phi)(100_\phi)
|
||||
\\
|
||||
(2^3 \cdot V_\text{dodec[1]})^2
|
||||
(2^3 \cdot V_\text{dodec})^2
|
||||
&= \left (12 \cdot {Bh \over 3} \right )^2 = 4^2 B^2 h^2
|
||||
= 2^4 \cdot 5(43_\phi) \cdot {(43_\phi)(100_\phi) \over 5}
|
||||
\\
|
||||
V^2
|
||||
V_\text{dodec}^2
|
||||
&= {2^4 \cdot (43_\phi)^2 \cdot (100_\phi) \over 2^6}
|
||||
= {(43_\phi)^2(10_\phi)^2 \over 2^2}
|
||||
\\
|
||||
V
|
||||
V_\text{dodec}
|
||||
&= {(43_\phi)(10_\phi) \over 2} = {(430_\phi) \over 2} = {(74_\phi) \over 2}
|
||||
= {4 + 7\phi \over 2}
|
||||
\end{align*}
|
||||
@ -613,13 +646,14 @@ The dodecahedron being so much larger than the icosahedron surprised me, to be h
|
||||
When one glances at a set of dice (as one does), it seems like the d20 is larger than the d12,
|
||||
albeit with smaller edges.
|
||||
However, at least in one of my sets, the edges of the d20 are in fact about 1.5 times as long
|
||||
as those of the d12, implying their volumes are roughly equal.
|
||||
as those of the d12, implying their volumes are roughly equal (which would be handy for a manufacturer).
|
||||
|
||||
***
|
||||
|
||||
I tried to use as much coordinate-free geometry as I could in producing these diagrams.
|
||||
GeoGebra lacks a tool for producing Platonic solids other than cubes and tetrahedra,
|
||||
so I ended up cheating in coordinates for the octahedron and icosahedron diagrams.
|
||||
|
||||
On the other hand, the hexagon I described in the dodecahedron is of such importance to
|
||||
its construction that I ended up constructing it from scratch.
|
||||
I am rather proud of this because I did so without looking up someone else's.
|
||||
|
After Width: | Height: | Size: 61 KiB |
BIN
posts/misc/platonic-volume/no-pentagons/octahedron_squares.png
Normal file
|
After Width: | Height: | Size: 71 KiB |
BIN
posts/misc/platonic-volume/no-pentagons/tetrahedron_bisect.png
Normal file
|
After Width: | Height: | Size: 52 KiB |
BIN
posts/misc/platonic-volume/pentagon_apothem.png
Normal file
|
After Width: | Height: | Size: 132 KiB |
BIN
posts/misc/platonic-volume/pentagon_measurements.png
Normal file
|
After Width: | Height: | Size: 181 KiB |
BIN
posts/misc/platonic-volume/pentagons/antiprism_measures.png
Normal file
|
After Width: | Height: | Size: 149 KiB |
BIN
posts/misc/platonic-volume/pentagons/bisected_dodecahedron.png
Normal file
|
After Width: | Height: | Size: 82 KiB |
BIN
posts/misc/platonic-volume/pentagons/dodecahedron_measures.png
Normal file
|
After Width: | Height: | Size: 167 KiB |
BIN
posts/misc/platonic-volume/pentagons/equilateral_triangles.png
Normal file
|
After Width: | Height: | Size: 100 KiB |
|
After Width: | Height: | Size: 122 KiB |
BIN
posts/misc/platonic-volume/pentagram_rhombus.png
Normal file
|
After Width: | Height: | Size: 353 KiB |
BIN
posts/misc/platonic-volume/square_pentagon_circles.png
Normal file
|
After Width: | Height: | Size: 245 KiB |
BIN
posts/misc/platonic-volume/triangle_centers.png
Normal file
|
After Width: | Height: | Size: 334 KiB |