Masteries · Jason GlowneyArithmoí Book 1

Masteries

1.4.1 Matrix Group Conic Sections

Our stud­ies of matrix groups stem­ming from the di­he­dral forms in com­plex geo­met­ric spaces lend them­selves to fur­ther clas­si­fi­ca­tion and group­ing in a com­plex conic space. The analy­sis of conic sec­tions has been around since an­tiq­ui­ty and in­volves cut­ting cones with a plane to obtain curves. The conics sec­tions are typ­i­cal­ly taught to be the in­ter­sec­tions of planes that do not pass through the cone's origin. Each plane can meet the cone in three ways to create in­ter­sect­ing curves: the parabo­la, the el­lipse, and the hy­per­bo­la, as seen in Figure 1.4.1 below.

Figure
Figure 1.4.1 – Parabo­la, el­lipse, and hy­per­bo­la as conic sec­tions.

For real-valued-based conic sec­tions, if a plane aligned with the zz-axis passed through the origin, a null curve would be the result, which is simply the two lines that form the bound­ary of the cone. When con­sid­er­ing a cone ori­ent­ed length­wise along the z-axis, the equa­tion of this cone ∈ℝ3\in \mathbb{R}^{3} can be rep­re­sent­ed as

x2+y2=k2z2,\begin{array}{r} x^{2} + y^{2} = k^{2}z^{2}, \end{array}
(1.4.1)

where kk is a con­stant.1 For the value of x=0x = 0, the above equa­tion of the cone will become

y2=k2z2→y=±kz,\begin{array}{r} y^{2} = k^{2}z^{2} \rightarrow y = \pm kz, \end{array}
(1.4.2)

and this is simply the equa­tion of two lines, which is the null curve as seen in Figure 1.4.2. To con­sid­er the al­ge­bra­ic dif­fer­ences be­tween the parabo­la, el­lipse, and hy­per­bo­la, we take the cone to be sym­met­ric about the z-axis, as­sum­ing a cut­ting plane which is per­pen­dic­u­lar to the y,zy,z-plane, having the equa­tion

cy+dz=e.\begin{array}{r} cy + dz = e. \end{array}
(1.4.3)

Di­vid­ing by the co­ef­fi­cient for zz, or by the co­ef­fi­cient for y,y,and by set­ting for each the re­spec­tive y,z=0y,z = 0, yields the fol­low­ing cut­ting planes

c∙0d+dzd=fd→z=fd,  cyc+d∙0c =fc→ y=fc.\begin{array}{r} \frac{c \bullet 0}{d} + \frac{dz}{d} = \frac{f}{d} \rightarrow z = \frac{f}{d},\ \ \frac{cy}{c} + \frac{d \bullet 0}{c}\ = \frac{f}{c} \rightarrow \ y = \frac{f}{c}. \end{array}
(1.4.4)

Let f/c=ef/c = e. For the cut­ting plane, when y=e,y = e,the plane can move up and down along the yy-axis only as z=0z = 0, and hy­per­bol­ic curves result, except for the null curve when y=0.y = 0.Sub­sti­tut­ing this into our equa­tion of the cone, we find

k2z2−x2=e2,\begin{array}{r} k^{2}z^{2} - x^{2} = e^{2}, \end{array}
(1.4.5)

which is the re­sult­ing hy­per­bo­la. For z≠0z \neq 0, we can solve cy+z=ecy + z = e for zz, find­ing, z=e−cyz = e - cy, which we insert into our orig­i­nal equa­tion of the cone to find

x2+y2=k2(e−cy)2→x^{2} + y^{2} = k^{2}(e - cy)^{2} \rightarrow
x2+y2=k2(e2−2ecy+c2y2)→x^{2} + y^{2} = k^{2}\left( e^{2} - 2ecy + c^{2}y^{2} \right) \rightarrow
x2+y2(1−k2c2)+2k2ecy=k2e2.\begin{array}{r} x^{2} + y^{2}\left( 1 - k^{2}c^{2} \right) + 2k^{2}ecy = k^{2}e^{2}. \end{array}
(1.4.6)
Figure
Figure 1.4.2 – The null curve for x2+y2=k2z2x^{2} + y^{2} = k^{2}z^{2}, where x=0x = 0.

It is im­por­tant to note that the co­ef­fi­cient of y2y^{2} will depend on the slope of −c- c, for the cut­ting plane, and the fol­low­ing re­la­tion­ships hold for that slope

  • Less than 0 for c2>k2c^{2} > k^{2} - occurs for conics that are hy­per­bo­lae.
  • Greater than 0 for c2<k2c^{2} < k^{2} - occurs for conics that are el­lipses.
  • Equal to 0 for c2=k2c^{2} = k^{2} - occurs for conics that are parabo­la.

The equa­tion x2+y2(1−k2c2)+2k2ecy=k2e2x^{2} + y^{2}\left( 1 - k^{2}c^{2} \right) + 2k^{2}ecy = k^{2}e^{2} rep­re­sents the re­la­tion­ship be­tween xx and yy on the conic sec­tion and is the curve's pro­jec­tion in the x,yx,y-plane. Taking, (1−k2c2)\left( 1 - k^{2}c^{2} \right), as equal to zero or not, we can sim­pli­fy the equa­tion as

x2+Dy=C2 for z=0,\begin{array}{r} x^{2} + Dy = C^{2}\ for\ z = 0, \end{array}
 x2+A(y2−2By)=C2 for z≠0,\begin{array}{r} {\ x^{2} + A{(y}^{2} - 2By) = C}^{2}\ for\ z \neq 0, \end{array}
(1.4.7)

where, D=2k2ecD = 2k^{2}ec, C=keC = ke, A=(1−k2c2), B=k2ec1−k2c2.A = \left( 1 - k^{2}c^{2} \right),\ B = \frac{k^{2}ec}{1 - k^{2}c^{2}}.Next, by re­plac­ing y=(y−C2D)y = \left( y - \frac{C^{2}}{D} \right), for x2=Dy+C2x^{2} = Dy + C^{2}, and y=(y+B)y = (y + B), for  x2+A(y2+2By)=C2\ x^{2} + A{(y}^{2} + 2By) = C^{2}, the above become

x2=Dy,\begin{array}{r} x^{2} = Dy, \end{array}
(1.4.8)
x2+Ay2=C2+AB2.\begin{array}{r} x^{2} + Ay^{2} = C^{2} + AB^{2}. \end{array}
(1.4.9)

For x2=Dyx^{2} = Dy, we divide both sides by DD, set, 1D=a\frac{1}{D} = a, and find the fa­mil­iar equa­tion of the parabo­la

y=ax2.y = ax^{2}.

For x2+Ay2=C2−AB2x^{2} + Ay^{2} = C^{2} - AB^{2}, mul­ti­ply­ing by 1/A1/A, and di­vid­ing by (C2A−B2)\left( \frac{C^{2}}{A} - B^{2} \right), yields

x2(C2−B2A)+y2(C2A−B2)=1,\begin{array}{r} \frac{x^{2}}{\left( C^{2} - \frac{B^{2}}{A} \right)} + \frac{y^{2}}{\left( \frac{C^{2}}{A} - B^{2} \right)} = 1, \end{array}
(1.4.10)

and by sub­sti­tut­ing a2=(C2−B2A), b2=(C2A−B2)a^{2} = \left( C^{2} - \frac{B^{2}}{A} \right),\ b^{2} = \left( \frac{C^{2}}{A} - B^{2} \right), for C2A>B2\frac{C^{2}}{A} > B^{2}, and −b2=(C2A−B2)- b^{2} = \left( \frac{C^{2}}{A} - B^{2} \right), for C2A<B2\frac{C^{2}}{A} < B^{2}, we have equa­tions for the el­lipse

x2a2+y2b2=1,\begin{array}{r} \frac{x^{2}}{a^{2}} + \frac{y^{2}}{b^{2}} = 1, \end{array}
(1.4.11)

and the hy­per­bo­la

x2a2−y2b2=1.\begin{array}{r} \frac{x^{2}}{a^{2}} - \frac{y^{2}}{b^{2}} = 1. \end{array}
(1.4.12)

As we con­tin­ue, we will find the "null curve", rep­re­sent­ing the side of the cone in com­plex space, plays a piv­otal role math­e­mat­i­cal­ly in con­trast to the real conics, the in­ter­sec­tion of the top and bottom points of cones is not a zero-di­men­sion­al point but in­stead our U(3)U(3) sphere, and we ap­proach these conics by using the frame­works of tan­gent spaces and com­plex-valued angles.

  1. Still­well, John– "Num­bers and Geom­e­try", Springer, 2000