663 lines
22 KiB
Plaintext
663 lines
22 KiB
Plaintext
---
|
||
title: "On the Volume of the Platonic Solids"
|
||
description: |
|
||
How big are the Platonic solids in relation to one another?
|
||
format:
|
||
html:
|
||
html-math-method: katex
|
||
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*.
|
||
He describes their "construction" (sans the dodecahedron) from the most basic
|
||
"isosceles and scalene" triangles, or in modern parlance, "45-45-90 and 30-60-90" triangles, respectively.
|
||
However, the construction was not mathematical, and to my knowledge, each solid was first
|
||
rigorously described from first principles in Book XIII of Euclid's Elements.
|
||
|
||
In my teenage years, I recall viewing articles on the solids with their volumes
|
||
proudly displayed next to their surface area.
|
||
While surface area may be troublesome in the case of the dodecahedron
|
||
(as the geometry of regular pentagons is not widely taught),
|
||
it is easy enough for grade schoolers to calculate for cubes,
|
||
and for trigonometry students to calculate for the solids composed of equilateral triangles.
|
||
On the other hand, the volume is somewhat mystical.
|
||
|
||
Fortunately, edge length is the only free variable in a Platonic solid,
|
||
meaning their volumes can be parametrized by this value alone.
|
||
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 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.
|
||
|
||
|
||
A Recap of Geometry
|
||
-------------------
|
||
|
||
For those with only a vague recollection (or perhaps none at all) of geometry,
|
||
this section is intended as a refresher.
|
||
|
||
|
||
### Planar Geometry
|
||
|
||
There are [many centers of a triangle](https://faculty.evansville.edu/ck6/encyclopedia/etc.html),
|
||
but for us, two are of primary interest:
|
||
|
||
- The *circumcenter* is equidistant from every vertex.
|
||
In other words, it is the center of a circle containing all three vertices.
|
||
- It can be constructed by finding the intersection of the edges' perpendicular bisectors.
|
||
- 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
|
||
- 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*).
|
||
|
||

|
||
|
||
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.
|
||
|
||

|
||
|
||
$$
|
||
\begin{align*}
|
||
A &= \left ({e_1 a \over 2} + {e_2 a \over 2} + {e_3 a \over 2} \right)
|
||
= \left ({a \over 2} \right ) (e_1 + e_2 + e_3)
|
||
\\
|
||
&= {Pa \over 2}
|
||
\end{align*}
|
||
$$
|
||
|
||
This gives an expression for the area.
|
||
For an equilateral triangle, these two centers coincide.
|
||
This is because the perpendicular bisectors of the edges *are* the angle bisectors.
|
||
In fact, the bisection of an angle involves constructing a rhombus, which is made up of
|
||
two isosceles triangles (of which the equilateral triangle is a special case).
|
||
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.
|
||
For a square, the center is simply the intersection of the diagonals (i.e., the diagonals' common midpoint).
|
||
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
|
||
|
||
Now we speak of 3D geometry.
|
||
The volume of a prism is equal to the height times the area of the base,
|
||
where the "height" is orthogonal to the plane of the base.
|
||
Pyramids with the same height and base have one-third this area.
|
||
|
||
$$
|
||
V_\text{prism} = Bh,~~ V_\text{pyramid} = {Bh \over 3}
|
||
$$
|
||
|
||
This volume formula can be made more intuitive by considering the cube.
|
||
The pyramid formed by one of the faces and an edge perpendicular to it will contain
|
||
one square and two half-squares, or two squares in total.
|
||
Therefore three pyramids are needed to recreate all six faces of the cube.
|
||
|
||
For a slightly more detailed explanation, consider a point inside the face on top of the cube.
|
||
Its (perpendicular) distance from one edge is *x* and its distance to an edge adjacent to that is *y*.
|
||
Connecting all other bases to this point produces five pyramids, whose bases all have the same area.
|
||
Designate these pyramids as "bottom", "left", "right", "front", and "back",
|
||
where left and right correspond to *x* and front and back correspond to *y*.
|
||
|
||

|
||
|
||
$$
|
||
\begin{align*}
|
||
V_\text{cube}
|
||
&= Bh = V_\text{bottom} + V_\text{left} + V_\text{right} + V_\text{front} + V_\text{back}
|
||
\\
|
||
&= rBh + rBx + rB(h-x) + rBy + rB(h-y)
|
||
\\
|
||
&= rBh + rBh + rBh \implies 1 = 3r
|
||
\\
|
||
r &= {1 \over 3}
|
||
\end{align*}
|
||
$$
|
||
|
||
This can be generalized to a pyramid based on any prism, where the top point lies
|
||
in the plane of one of the bases.
|
||
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 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 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.
|
||
|
||
$$
|
||
(2h)^2 = e^2 + e^2 = 2 \cdot 2^2 = 2^3
|
||
$$
|
||
|
||

|
||
|
||
Therefore, the volume of an octahedron is:
|
||
|
||
$$
|
||
\begin{align*}
|
||
B^2
|
||
&= (e^2)^2
|
||
= (2^2)^2 = 2^4
|
||
\\
|
||
(2 V_\text{sq.pyr.})^2
|
||
&= (2^2) \left( {B^2 h^2 \over 3^2} \right)
|
||
= {B^2 (2h^2) \over 3^2}
|
||
= {{2^4 \cdot 2^3} \over 3^2}
|
||
= {2^7 \over 3^2}
|
||
\\
|
||
(2^3 \cdot V_\text{oct})^2
|
||
&= {2^7 \over 3^2}
|
||
\implies V_\text{oct}^2
|
||
= {2 \over 3^2}
|
||
\\
|
||
V_\text{oct}
|
||
&= {\sqrt{2} \over 3}
|
||
\end{align*}
|
||
$$
|
||
|
||
|
||
### Tetrahedron
|
||
|
||
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-valign="center"}
|
||
|
||

|
||
|
||
::: {.column}
|
||
$$
|
||
\begin{align*}
|
||
d_\text{altitude}^2
|
||
&= \textcolor{orange}{2}^2 -\ \textcolor{green}{1}^2 = 3
|
||
\\
|
||
B^2
|
||
&= \left ( {2 \cdot d_\text{altitude} \over 2} \right )^2 = 3
|
||
\end{align*}
|
||
$$
|
||
:::
|
||
|
||
::::
|
||
|
||
Next, bisect this triangle through any edge, then use it to bisect the tetrahedron through
|
||
the plane containing this line and the remaining edge.
|
||
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-valign="center"}
|
||
|
||

|
||
|
||
::: {.column}
|
||
$$
|
||
\begin{align*}
|
||
\textcolor{blue}{d_\text{length}}^2
|
||
&= d_\text{altitude}^2 -\ \textcolor{green}{1}^2 = 2
|
||
\\
|
||
(2A_\text{center})^2
|
||
&= (2d_\text{length})^2 = (\textcolor{red}{h} d_\text{altitude})^2
|
||
\\
|
||
&= 4 \cdot 2 = 3h^2
|
||
\\
|
||
h^2 &= 8 / 3
|
||
\end{align*}
|
||
$$
|
||
:::
|
||
|
||
::::
|
||
|
||
Since *h* is known, we can calculate the volume.
|
||
|
||
$$
|
||
\begin{align*}
|
||
({ 2^3 \cdot V_\text{tet} })^2
|
||
&= {B^2 h^2 \over 3^2} = {3 \cdot (8/3) \over 3^2}
|
||
\\
|
||
V_\text{tet}^2
|
||
&= {8 \over 2^6 \cdot 3^2} = {1 \over 2^3 \cdot 3^2} = {1 \over 2 \cdot 6^2}
|
||
\\
|
||
V_\text{tet}
|
||
&= \sqrt{1 \over 6^2 \cdot 2} = {1 \over 6\sqrt 2}
|
||
\end{align*}
|
||
$$
|
||
|
||
|
||
### Returning to 2D: Regular Pentagons
|
||
|
||
Both of the icosahedron and dodecahedron contain regular pentagons.
|
||
Thus, it is necessary to examine them in detail.
|
||
|
||
The regular pentagon has five diagonals, which form a pentagram.
|
||
Since all angles in a regular pentagon are equal, the trapezoid formed by three consecutive edges
|
||
and one diagonal is isosceles.
|
||
This means the diagonal is parallel to one of the edges, which applies to all diagonals by symmetry.
|
||
|
||
Since the diagonal is parallel to one of the sides, a parallelogram can be formed from
|
||
two sides and segements from two diagonals.
|
||
More specifically, this parallelogram is a rhombus, since the segments must have equal lengths
|
||
to the sides.
|
||
|
||

|
||
|
||
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*.
|
||
|
||

|
||
|
||
$$
|
||
\begin{align*}
|
||
\textcolor{orange}{d}^2 + \textcolor{red}{h}^2
|
||
&= \textcolor{blue}{2}^2
|
||
\\
|
||
2\textcolor{darkblue}{A_\text{blue}}
|
||
&= 2\textcolor{green}{g} = h(\textcolor{magenta}{d -\ (2 -\ d)}) = h (2d -\ 2)
|
||
\\
|
||
\implies g &= {h(2d -\ 2) \over 2} = h(d -\ 1)
|
||
\end{align*}
|
||
$$
|
||
|
||
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 gives us enough information to deduce *d*:
|
||
|
||
$$
|
||
\begin{align*}
|
||
{\textcolor{red}{h} \over 2(\textcolor{brown}{2 -\ d})}
|
||
&= {2\textcolor{red}{h} + \textcolor{green}{g} \over \textcolor{blue}{2}}
|
||
= {2h + h(d-1) \over 2} = {h(1 + d) \over 2 }
|
||
\\
|
||
2h &= 2h(1 + d)(2 -\ d)
|
||
\\
|
||
1 &= (1 + d)(2 -\ d) = 2 -\ d + 2d -\ d^2
|
||
\\
|
||
0 &= d^2 -\ d -\ 1
|
||
\end{align*}
|
||
$$
|
||
|
||
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
|
||
).
|
||
|
||
To calculate the apothem, we can calculate the sagitta *s* and height *l* by similar triangles.
|
||
|
||

|
||
|
||
$$
|
||
\begin{align*}
|
||
&\textcolor{blue}{c \over a}
|
||
= \textcolor{brown}{2 \over \phi}
|
||
\\
|
||
l &= c + a = {2a \over \phi} + a = a{2 + \phi \over \phi}
|
||
= a{12_\phi \over 10_\phi}
|
||
= a{2\bar{1}0_\phi \over 10_\phi} = a(2\bar{1}_\phi)
|
||
\\
|
||
s &= c -\ a = {2a \over \phi} -\ a
|
||
= a{2 -\ \phi \over \phi} = a{\bar{1}2_\phi \over 10_\phi}
|
||
= a{2\bar{3}0_\phi \over 10_\phi} = a(2\bar{3}_\phi)
|
||
\end{align*}
|
||
$$
|
||
|
||
Finally, the Pythagorean theorem tells us that the product of these quantities is 1,
|
||
allowing us to calculate *a*.
|
||
|
||
$$
|
||
\begin{align*}
|
||
1 &= c^2 -\ a^2 = (c + a)(c -\ a) = ls
|
||
\\
|
||
&= a^2(2\bar{1}_\phi)(2\bar{3}_\phi)
|
||
= a^2(4\bar{8}3_\phi)
|
||
= a^2(\bar{4}7_\phi) = a^2(3.\bar{4}_\phi)
|
||
\\
|
||
a^2 &= {1 \over 3.\bar{4}_\phi} \cdot {43_\phi \over 43_\phi}
|
||
= {43_\phi \over [12]\bar{7}.[\bar{12}]_\phi}
|
||
= {3 + 4\phi \over 5}
|
||
\\
|
||
\implies l^2 &= a^2(2\bar{1}_\phi)^2
|
||
= {3 + 4\phi \over 5} \cdot (4\bar{4}1_\phi)
|
||
= {3 + 4\phi \over 5} \cdot 5 = 3 + 4\phi
|
||
\end{align*}
|
||
$$
|
||
|
||
The last few steps in solving for $a^2$ are somewhat tricky.
|
||
The conjugate of *φ* is $\varphi^* = -{1 \over \varphi}$.
|
||
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 $[12]\bar{7}.[\bar{12}]_\varphi$ resolves cleanly to 5.
|
||
|
||
The division can also be done explicitly in phinary:
|
||
|
||
$$
|
||
\begin{align*}
|
||
{1 \over 3.\bar{4}_\varphi}
|
||
&= {1 \over 0.\bar{1}3_\varphi}
|
||
= {500_\varphi \over 5 (\bar{1}3_\varphi)}
|
||
= {233_\varphi + (0 = \textcolor{red}{4\bar{4}}\bar{4}0_\varphi
|
||
= \textcolor{red}{26\bar{2}}\bar{4}0_\varphi) \over 5 (\bar{1}3_\varphi)}
|
||
\\
|
||
&= {\bar{2}60\bar{1}3_\varphi \over 5 (\bar{1}3_\varphi)}
|
||
= {2001_\varphi \over 5}
|
||
= {221_\varphi \over 5}
|
||
= {43_\varphi \over 5}
|
||
= {3 + 4\varphi \over 5}
|
||
\end{align*}
|
||
$$
|
||
|
||
|
||
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.
|
||
|
||
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.
|
||
|
||
The altitude (*h*) of any one pyramid is the radius of the *insphere* of the solid,
|
||
which is tangent to the plane of every face.
|
||
Similarly, the *circumsphere* (circumradius, *r*) contains all vertices,
|
||
and the *midsphere* (midradius, *ρ*) is tangent to every edge.
|
||
These will become important shortly.
|
||
|
||
|
||
### The Icosahedron: an Antiprism in Profile
|
||
|
||
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.
|
||
|
||

|
||
|
||
The pentagonal antiprism may be bisected bisected along the plane containing the altitudes
|
||
of two antipodal triangles.
|
||
This forms a parallelogram with side lengths of the altitude of an equilateral triangle
|
||
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,
|
||
|
||
$$
|
||
\begin{align*}
|
||
(\textcolor{green}{2h})^2
|
||
&= \textcolor{red}{l}^2 - a^2
|
||
= \textcolor{red}{3 + 4\phi}
|
||
-\ {1 \over 3}
|
||
= {3(3 + 4\phi) -\ 1 \over 3}
|
||
\\
|
||
h^2
|
||
&= {8 + 12\phi \over 3 \cdot 4}
|
||
= {2 + 3\phi \over 3}
|
||
= {32_\phi \over 3}
|
||
\\
|
||
32_\phi
|
||
&= 210_\phi = 1100_\phi = 10000_\phi
|
||
= \phi^4
|
||
\end{align*}
|
||
$$
|
||
|
||
With the inradius in tow, we can calculate the volume of the icosahedron.
|
||
|
||
$$
|
||
\begin{align*}
|
||
(2^3 \cdot V_\text{ico})^2
|
||
&= \left ( 20 \cdot {Bh \over 3} \right )^2
|
||
= {20^2 B^2 h^2 \over 3^2} = {5^2 \cdot 4^2 \cdot 3 \cdot {\phi^4 \over 3} \over 3^2}
|
||
= {5^2 \cdot 2^4 \cdot \phi^4 \over 3^2}
|
||
\\
|
||
V_\text{ico}^2
|
||
&= {5^2 \cdot 2^4 \cdot \phi^4 \over 2^6 \cdot 3^2}
|
||
= {5^2 \cdot \phi^4 \over 2^2 \cdot 3^2}
|
||
\\
|
||
V_\text{ico} &= {5 \phi^2 \over 6}
|
||
\end{align*}
|
||
$$
|
||
|
||
|
||
### The Dodecahedron
|
||
|
||
The dodecahedron is a bit trickier.
|
||
It belongs to a class of polyhedra known as *truncated trapezohedra*.
|
||
|
||
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.
|
||
It is parallel to the two edges, so dropping an altitude from this edge to the diameter
|
||
produces a midradius.
|
||
|
||

|
||
|
||
The inradius *h* is the altitude of a triangle formed by the length of a pentagon (its base),
|
||
a midradius, and a circumradius.
|
||
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.
|
||
|
||
$$
|
||
\begin{align*}
|
||
\textcolor{orange}{l}\textcolor{green}{h}
|
||
&= \textcolor{blue}{\rho \rho} \implies \textcolor{orange}{l}^2\textcolor{green}{h}^2
|
||
= (\textcolor{orange}{(2\bar{1}_\phi) a})^2 h^2
|
||
= 5a^2h^2
|
||
= \textcolor{blue}{\rho}^4
|
||
\\
|
||
5a^2h^2
|
||
&= (a^2 + h^2)^2
|
||
= a^4 + 2a^2h^2 + h^4
|
||
\end{align*}
|
||
$$
|
||
|
||
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.
|
||
|
||
$$
|
||
\begin{align*}
|
||
0 &= h^4 -\ 3a^2h^2 + a^4
|
||
= (h^2 -\ x)^2 - y^2
|
||
\\
|
||
&= h^4 -\ 2xh^2 + x^2 - y^2
|
||
\\
|
||
-2x &= -3a^2
|
||
\implies x = {3a^2 \over 2}
|
||
\\
|
||
x^2 - y^2 &= {9a^4 \over 4} - y^2 = a^4
|
||
\\
|
||
\implies y^2 &= {9a^4 \over 4} - {4a^4 \over 4}
|
||
= {5a^4 \over 4}
|
||
= {(2\bar{1}_\phi)^2 a^4 \over 4}
|
||
= \left ( {(2\bar{1}_\phi) a^2 \over 2} \right )^2
|
||
\\ \\
|
||
h^2 -\ {3a^2 \over 2}
|
||
&= y
|
||
= {(2\bar{1}_\phi) a^2 \over 2}
|
||
\\
|
||
h^2
|
||
&= {(2\bar{1}_\phi) a^2 \over 2} + {3a^2 \over 2}
|
||
= {(22_\phi) a^2 \over 2} = (11_\phi) a^2
|
||
\\
|
||
&= {(11_\phi)(43_\phi) \over 5}
|
||
= {473_\phi \over 5}
|
||
= {[11]7_\phi \over 5} = {7 + 11\phi \over 5}
|
||
\end{align*}
|
||
$$
|
||
|
||
With the square of the inradius known, all that is left to do is find the volume.
|
||
|
||
$$
|
||
\begin{align*}
|
||
B^2
|
||
&= \left( {Pa \over 2} \right)^2
|
||
= (5a)^2 = 25a^2 = 5(43_\phi)
|
||
\\
|
||
5h^2
|
||
&= [11]7_\phi = 740_\phi = 4300_\phi
|
||
= (43_\phi)(100_\phi)
|
||
\\
|
||
(2^3 \cdot V_\text{dodec})^2
|
||
&= \left (12 \cdot {Bh \over 3} \right )^2 = 4^2 B^2 h^2
|
||
= 2^4 \cdot 5(43_\phi) \cdot {(43_\phi)(100_\phi) \over 5}
|
||
\\
|
||
V_\text{dodec}^2
|
||
&= {2^4 \cdot (43_\phi)^2 \cdot (100_\phi) \over 2^6}
|
||
= {(43_\phi)^2(10_\phi)^2 \over 2^2}
|
||
\\
|
||
V_\text{dodec}
|
||
&= {(43_\phi)(10_\phi) \over 2} = {(430_\phi) \over 2} = {(74_\phi) \over 2}
|
||
= {4 + 7\phi \over 2}
|
||
\end{align*}
|
||
$$
|
||
|
||
|
||
Closing
|
||
-------
|
||
|
||
Since each of these volumes has been calculated algebraically, there have been no approximate decimal forms.
|
||
Ordered by size, the volumes of each of the solids are:
|
||
|
||
| Solid | Volume | Approximation | Length of Side with Unit Volume |
|
||
|--------------|-----------------------|-----------------|---------------------------------|
|
||
| Tetrahedron | ${1 \over 6\sqrt 2}$ | 0.1178511302... | 2.039648903... |
|
||
| Octahedron | ${\sqrt{2} \over 3}$ | 0.4714045208... | 1.284898293... |
|
||
| Cube | $1^3$ | 1 | 1 |
|
||
| Icosahedron | ${5\phi^2 \over 6}$ | 2.181694991... | 0.7710253465... |
|
||
| Dodecahedron | ${4 + 7\phi \over 2}$ | 7.663118961... | 0.5072220724... |
|
||
|
||
The dodecahedron being so much larger than the icosahedron surprised me, to be honest.
|
||
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 (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 having written this post, I feel much more competent with compass-and-straightedge constructions.
|
||
|
||
All diagrams made with GeoGebra.
|