Intro to Inversive Gerometry
Shirleen Stibbe
OPEN UNIVERSITY
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M203 Pure Mathematics Summerschool
Inversion in a circle, centre 0, radius r A' = (X, Y) = (kx, ky), k ≠ 0 t: A → A' OA.OA' = r2
r O
A = (x, y)
NB OA = |A| = x 2 + y 2 ,
|A'| = k|A|
Example: Invert A = (3, 4) in the unit circle (r = 1) r2 = 1 = |(3, 4)| x |(3k, 4k)| = So k =
1/25
and A' =
5 x 5k = 25k (3/25, 4/25)
points outside ⇔ points inside points on the circle fixed t: A' →A , and
t-1 = t (self inverse)
what happens to the centre???? Can't cope - yet. So get rid of it in the meantime. Punctured plane 2
Inversion in the unit circle C (centre 0, radius 1) A = (x, y)
A' = (X, Y) = (kx, ky),
k>0
OA ⋅ OAʹ′ = x 2 + y 2 × k x 2 + y 2 = k( x 2 + y 2 ) = r 2 = 1 so
k=
1 2
x +y
2
and
⎛ x y ⎞ ⎟ ( X, Y ) = ⎜⎜ 2 , 2 2 2 ⎟ x + y ⎠ ⎝ x + y
Strategy: HB p62 To find the image of: a circle: (x - a)2 + (y - b)2 - r = 0 a line: ax + by = 0 under inversion in the unit circle: 1) Replace x by x / (x2 + y2) y by y / (x2 + y2) in the equation 2) Simplify No! Get a life! 3
Inversion in C - the easy way Write the equation of the curve C in the form: d(x2 + y2) + ax + by + c = 0 (*) C is a circle if d ≠! 0, a line if d = 0 C passes through the origin if and only if c = 0 To invert C in the unit circle: interchange c and d in (*) That is: t(C) is the curve with equation c(x2 + y2) + ax + by + d = 0 Images Equation
Curve
Inverts to
c≠0 d≠0
circle not through 0
circle not through 0
c≠0 d=0
line not through 0
circle through 0
c=0 d≠0
circle through 0
line not through 0
c=0 d=0
line through 0
line through 0 4
Oops - we're not doing very well Can't cope with the origin Doesn't preserve circles Doesn't preserve lines Doesn't preserve size
Some good news - at last Angle theorem: Inversion preserves size, reverses direction of angles between curves - just as reflection does
5
Examples: Invert
i) L, the line x = 1/2, and ii) C, the circle centre (1, 0), radius 2
in the unit circle C L Draw a picture
C
C -1
0
1
2
3
Do some algebra:
Equation for L: 0(x2 + y2) - x + 1/2 = 0
Equation for t(L): 1/2(x2 + y2) -x = 0 Simplifies to: (x-1)2 + y2 = 1
Equation for C: 1(x2 + y2) -2x - 3 = 0
Equation for t(C): -3(x2 + y2) -2x +1 = 0 Simplifies to (x+1/3)2 + y2 = 4/9
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Even easier way: L: line not through 0 → circle through 0 symmetric about x axis (right angles preserved) points on the circle fixed (1/2, 0) (nearest to 0) → (2, 0) (furthest from 0) Image: circle centre (1, 0), radius 1 C: circle not through 0 → circle not through 0 symmetric about x axis (right angles preserved) (-1, 0) fixed (3, 0) (furthest from 0) → (1/3, 0) (nearest to 0) Image: circle centre (-1/3, 0), radius 2/3 L C L'
C -1
-1/3
1
2
3
C'
7
Now for the really cunning part Use complex numbers
Inversion in C is a doddle: z → 1/ z
⎛ x y ⎞ ⎟ z = x + iy ~ ( x, y ) → ⎜⎜ 2 , 2 2 2 ⎟ ⎝ x + y x + y ⎠ ~
x + iy x2 + y2
=
x + iy 1 1 = = ( x − iy )( x + iy ) x − iy z
Euclidean transformations in C z+c
Translation:
z
t(z) = z + c, c = a + ib
Reflection in x-axis: t(z) = z
b a
z z
Rotation about 0: t(z) = az a = Cosθ + iSinθ
az θ z
compositions of reflections Scaling: t(z) = kz, k ∈ R, k > 0 8
Rotate through angle θ = reflect in line p, then reflect in line q
q
p
t(z)
θ/2
z
Translate through vector c = reflect in line p, then reflect in line q
q t(z)
p
|c|
z
½|c| 9
Inversion in C, centre c = a +ib, radius r We know how to invert in the unit circle C, so … Abuse the plane to convert C to C Do the inversion in C Conceal the evidence; convert C back to C Convert C to C:
translate through -c, scale by 1/r
z−c , r 1 t:z→ z
t1 : z → Invert in C:
Convert C to C:
scale by r, translate through +c Note: t1 = t2-1
t 2 : z → rz + c tC:
z
t 2−1
⎯⎯ ⎯→
z−c r
t C ( z) =
t
⎯⎯→
t 2 t t 2−1( z)
r z−c
t2
⎯⎯→
r2 +c z−c
r2 = +c z−c
Discovery! tC and t are conjugates 10
A late arrival at the Inversion Ball Introducing the very lovely
Point at Infinity
∞
extend the plane: C ∪ {∞} = Ĉ solves (nearly) all our problems 0 → ∞ and ∞ → 0 under inversion define a line as a (generalised) circle with infinite radius generalised circles
→ generalised circles
we're back in business inversion (nearly) back in line with reflection
Generalised Circle: Ordinary circle if it doesn't contain ∞ Extended line if it contains ∞ 11
Inversion in Ĉ C a generalised circle in Ĉ t = inversion in C If C is a 'proper' circle, centre 0, radius r: t(0) = ∞ t(∞ ) = 0 t(z) = normal inversion, z ≠ 0,
z≠∞
If C is an extended line L ∪ {∞}: t(∞ ) = ∞ t(z) = reflection in L,
z≠∞
Inversive Group Elements:
set of inversive transformations
Operations:
composition of functions
Properties:
a) map gen circles to gen circles b) preserve magnitude of angles 12
Möbius Functions
M:C →Ĉ
M(z) :
az + b az + b M( z ) = cz + d cz + d a, b, c, d ∈ C, ad – bc ≠ 0
M( z) =
direct - preserves orientation of angles composite of even number of inversions
M( z ) :
indirect - reverses orientation of angles composite of odd number of inversions
⎧∞ if c = 0 M(∞) = ⎨ ⎩a / c if c ≠ 0
Working form
M( −d / c ) = ∞
⎛ z − α ⎞ M( z) = K ⎜ ⎟ ⎝ z − β ⎠ K = a / c, α = −b / a, β = −d / c
r2 Example1: Express + c as a Möbius transformation z−c r2 r 2 + c( z − c ) cz + (r 2 − cc ) z−α +c = = = c z−c z−c z−c z−c where α = c − r 2 / c
13
M( z) =
Möbius and Matrices
Associated matrix:
⎛ a b ⎞ A = ⎜ ⎟, ⎝ c d ⎠
az + b cz + d
A
−1
⎛ d − b ⎞ = ⎜ ⎟ ⎝ − c a ⎠
Composition of transformations = matrix multiplication
Example2:
M( z) =
z −i z−2
i) calculate M(2), M(i) and M( ∞ ) ii) show that M-1M(z) = z
i)
M(2) = ∞,
M(i) = 0
1− i / z = 1 |z|→∞ 1 − 2 / z
M(∞ ) = lim
ii)
A
−1
Matrix is
⎛1 − i ⎞ A = ⎜ ⎟ ⎝1 − 2 ⎠
⎛ − 2 i ⎞ = ⎜ ⎟ so ⎝ − 1 1⎠
ad − bc = −2 + i ≠ 0
0 ⎞ ⎛ − 2 i ⎞ ⎛1 − i ⎞ ⎛ − 2 + i A A = ⎜ ⎟ ⎜ ⎟ = ⎜ ⎟ − 2 + 1⎠ ⎝ − 1 1⎠ ⎝1 − 2 ⎠ ⎝ 0 −1
14
Fundamental Theorem
Given any 3 points in C, there exists a Möbius transformation that maps these to any other three given points. Note: Two points do not fix a generalised circle:
But three do:
∞
∞
15
Putting Möbius to work To determine whether four points, a, b, c, d, all lie on the same generalised circle: 1
The first 3 points (a, b and c) determine a generalised circle, C.
2
Find a Möbius transformation M(z) that takes a, b and c to the real axis [ Easiest way: send them to 0, 1 and ∞ ]
3
The M you found maps the C, the whole C and nothing but the C to the real axis, and M-1 maps the real axis back to the generalised circle, C.
4
Apply M to the 4th point, d. If M(d) is real, say M(d) = x ∈ R, then M-1(x) = d lies on the generalised circle C.
5
If not, then it doesn't.
6
If M(∞) is real, then ∞ lies on C, so C is an extended line. Otherwise, C is a 'proper' circle. 16
Example 1 Find a Möbius transformation that maps 1 - i to ∞ 4 + 4i to 0, and 5 to 1.
z−a M( z) = K , z −b
M( 4 + 4i) = 0 M(1 − i) = ∞
⎛ z − ( 4 + 4i) ⎞ ⇒ M( z) = K⎜ ⎟ ⎝ z − (1 − i) ⎠
⎛ 5 − ( 4 + 4i) ⎞ ⎛ 1 − 4i ⎞ M(5) = K⎜ = K ⎟ ⎜ ⎟ = 1 ⎝ 4 + i ⎠ ⎝ 5 − (1 − i) ⎠
So K =
4+i i (1 − 4i) = = i 1 − 4i 1 − 4i
iz + 4 − 4i ⎛ z − ( 4 + 4i) ⎞ Therefore M( z) = i ⎜ = ⎟ z − ( 1 − i ) z − 1+ i ⎝ ⎠ 2 Do the points 1 - i, 4 + 4i, 5 and 3i all lie on the same generalised circle, and if so, what kind of circle is it? 1 - i, 4 + 4i, 5 lie on a generalised circle, C, which is mapped by M to the real axis.
M(3i) =
− 3 + 4 − 4i 1 − 4i = = −1 3i − 1 + i − 1 + 4i
which is real, so 3i must lie on C M(∞) = K = i, which is not on the real axis, so ∞ is not on C So C is a 'proper' circle and not an extended line. 17