Consider the HSV model of describing colors. Any color $c$ can be described as an element of $I^3$, where $\pi_1(c)$ describes hue, $\pi_2(c)$ describes saturation, and $\pi_3(c)$ describes brightness. Without thought, one might think the topological shape of the spectrum of colors is just $D^3$. However,
- A hue of zero describes the same color as a hue of one.
- $\ (0, s, b) \thicksim (1, s, b)$ for each $s, b \in I$.
- If a color has no saturation, it is uniquely described only by its brightness.
- $\ (h, 0, b) \thicksim (h', 0, b)$ for each $h, h', b \in I$.
- A brightness of zero or one is black or white respectively.
- $\ (h, s, 0) \thicksim (h', s', 0)$ for each $h, h', s, s' \in I$.
- $\ (h, s, 1) \thicksim (h', s', 1)$ for each $h, h', s, s' \in I$.
I believe there to be no further identifications, for if a color has some saturation, and is not black or white, it should be unique. So, what is the topological structure of $D^3$ after these identifications?
I think the answer is that the identifications $2, 3,$ and $4$ have no effect, and the outcome is a solid torus. But this doesn't make sense because many such "color spheres" exist.
It's not true that the identifications after the first have no effect. For one, the result is that the "loop" of the solid torus - the curve $f(t) = (t,s,b)$ - is homotopic to the identity map $f(t) = (t,s,0)$.
Instead, let's look at the identifications in the reverse order. We start with a cube, which has six faces: the $h=0$ face, the $h=1$ face, the $s=0$ face, the $s=1$ face, the $b=0$ face, and the $b=1$ face.
Identification 4 contracts the $b=1$ face to a point, giving us a pyramid.
Identification 3 contracts the $b=0$ face to a point, giving an awkward thing we can't draw as a polyhedron anymore, but which still has four $2$-sided faces meeting at the $b=0$ and $b=1$ points. (We could call this a hosohedron.)
Identification 2 contracts the $s=0$ face to a segment, so that now we have only the $h=0$, $h=1$, and $s=1$ faces left. They each meet along an edge (the $h=0$ and $h=1$ faces meet along the $s=0$ edge) and all three come together at the $b=0$ and $b=1$ points.
Finally, identification 1 identifies the two $h=0$ and $h=1$ faces. The result is a disk with only the $s=1$ face on the outside.