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Conformal Maps and Mobius Transformations

See that an analytic map with nonzero derivative preserves angles, and use Mobius maps to move standard regions onto one another.

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What a learner can do afterwards

  • Explain why a holomorphic map with nonzero derivative preserves oriented angles locally
  • Construct the unique Mobius transformation matching corresponding entries of two ordered triples, each containing three distinct extended-plane points
  • Map the upper half-plane bijectively onto the unit disc and transfer harmonic Dirichlet boundary data and solutions

1 · Read

Let f be holomorphic near a. A tangent vector v at a maps to f'(a)v. If f'(a) is nonzero, this multiplication rotates every tangent by the same angle and scales every length by the same positive factor. It preserves oriented angles between regular curves. This is local conformality. The exponential qualifies at every finite point: its derivative e^z never vanishes.

Try it together

For f(z)=alpha*z+beta, alpha != 0, the multiplier alpha scales lengths by |alpha| and turns directions by arg(alpha). Adding beta translates the image without changing tangents. Multiplication by i turns directions 90 degrees counterclockwise. To evaluate a point image, distribute and use i^2=-1. For f(z)=2iz+1, f(2-i)=4i-2i^2+1=3+4i.

z=2-i2iz+1=4i-2i^2+1f(z)=3+4i

For f(z)=z^2, the derivative 2z vanishes only at 0. Squaring sends a ray of direction theta to direction 2*theta, so it does not preserve angles at 0. Local conformality also differs from global injectivity. The exponential is conformal everywhere, but e^(z+2*pi*i)=e^z. In particular, 0 and 2*pi*i both map to 1.

A Mobius map is T(z)=(az+b)/(cz+d), where ad-bc != 0. Its derivative is T'(z)=(ad-bc)/(cz+d)^2, nonzero wherever cz+d != 0. A zero determinant instead gives a constant ratio where defined, provided the denominator is not identically zero. Multiplying all four coefficients by one nonzero number leaves the map unchanged.

T=(az+b)/(cz+d)ad-bc != 0T'=(ad-bc)/(cz+d)^2

The extended complex plane adds one point, infinity. A Mobius map is a bijection of this plane. If c != 0, its pole -d/c maps to infinity and T(infinity)=a/c, found by a limit. If c=0, infinity maps to infinity and T is affine. Mobius maps send generalized circles to generalized circles: these are circles and lines completed by infinity.

Two ordered triples of distinct extended-plane points determine exactly one Mobius map matching corresponding entries. For finite p,q,r, A(z)=((z-p)/(z-r))*((q-r)/(q-p)) sends p,q,r to 0,1,infinity in that order. Normalize the target triple with B in the corresponding order. Then T=B^-1 composed with A gives the prescribed images. Use limits when infinity occurs. Distinct targets are necessary because the map is injective.

A: source to 0,1,infinityB: target to 0,1,infinityT = B^-1 composed with A
Try it together

Construct T taking (0,4,infinity) to (0,1,3). From T(0)=0, set b=0. The finite image of infinity requires c != 0; rescale to c=1. Then T(infinity)=3 gives a=3. The condition T(4)=1 gives 12/(4+d)=1, so d=8. Thus T(z)=3z/(z+8), with determinant 24 != 0. If infinity instead maps to infinity, use the affine form alpha*z+beta.

T(0)=0: b=0T(infinity)=3: a=3cT(4)=1: d=8cT(z)=3z/(z+8)

Evaluate a ratio by substituting into both numerator and denominator. For R(z)=(z-2)/(z+2), R(4)=2/6=1/3. For a complex denominator, multiply both parts by its conjugate. With C(z)=(z-i)/(z+i) and real x, this gives C(x)=(x-i)^2/(x^2+1)=(x^2-1-2ix)/(x^2+1).

(x-i)/(x+i)multiply by (x-i)/(x-i)(x^2-1-2ix)/(x^2+1)

C(z)=(z-i)/(z+i) maps H={Im z>0} bijectively onto D={|w|<1}, with C(i)=0. For z=x+iy, |C(z)|^2=[x^2+(y-1)^2]/[x^2+(y+1)^2]<1 when y>0. Solving w=C(z) gives C^-1(w)=i(1+w)/(1-w). Its imaginary part is (1-|w|^2)/|1-w|^2>0 on D. Every disc point therefore has a unique inverse in H.

A real-valued harmonic u satisfies Delta u=u_xx+u_yy=0. A Dirichlet problem prescribes its boundary values. For holomorphic C, Delta(u composed with C)=|C'|^2*(Delta u) composed with C. For C:H to D, set disc data h=g composed with C^-1. Once a harmonic disc solution u with data h is known, v=u composed with C solves the half-plane problem. Apply the forward map C before u.

h = g composed with C^-1solve u on D with data hv = u composed with C

For C(z)=(z-i)/(z+i), finite real x have |C(x)|=1 and C(x) != 1. Their images form the unit circle minus 1; C(infinity)=1 fills the gap. Continuous data on the completed real boundary must have a common limit g(infinity) as x tends to either real infinity. The transformed data then satisfy h(1)=g(infinity). A disc solution continuous on the closed disc pulls back to these boundary values.

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To find g(infinity) for a rational function with equal numerator and denominator degrees, divide both by the highest power of x. Terms with negative powers tend to 0. For g(x)=(5x^2+2)/(x^2+4), rewrite it as (5+2/x^2)/(1+4/x^2). The limit is 5 at both real ends. Thus the transformed boundary data have h(1)=5.

(5x^2+2)/(x^2+4)(5+2/x^2)/(1+4/x^2)g(infinity)=5h(1)=5
Try it together

To evaluate a pulled-back solution, compute w=C(z) first and then apply u. For u(w)=Re w and z=4i, C(4i)=3i/(5i)=3/5, so v(4i)=3/5. Real parts of holomorphic functions are harmonic. Another disc example is u(w)=Re(w^2); evaluate it by squaring C(z) before taking the real part.

z=4iw=C(4i)=3/5u(w)=Re w=3/5
For z=4i, first compute C(4i)=3/5, then apply u(w)=Re w.

A nonzero holomorphic derivative preserves local angles. Distinct ordered triples fix one Mobius map in matching order. Use the inverse for boundary data and the forward map for solutions.

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These readings, extra questions and flashcards were written for this dataset.

More to read

What the derivative says about a map

Suppose f is holomorphic near a. Its local expansion is f(a+h)=f(a)+f'(a)h+o(|h|). The linear term describes how tangent vectors change. If f'(a) has modulus r>0 and argument theta, every tangent length is multiplied by r and every tangent direction turns by theta. Their oriented angle stays unchanged.

For example, multiplication by 3i triples lengths and turns directions 90 degrees counterclockwise. A translation added afterward changes positions but leaves tangent vectors unchanged.

The condition concerns local geometry. It does not promise that distant inputs have different images. The exponential has a nonzero derivative everywhere, yet adding 2*pi*i to an input leaves its image unchanged. Squaring behaves differently at its critical point: rays through 0 have their directions doubled, so angles are not preserved there.

Using three prescribed images

Write a Mobius map as T(z)=(az+b)/(cz+d), with ad-bc nonzero. A common nonzero factor in the four coefficients does not change T. The map acts bijectively on the complex plane completed by one point at infinity.

To send one ordered triple of distinct points to another, first normalize both triples to 0,1,infinity. If A normalizes the sources and B normalizes the targets, use T=B^-1 composed with A. For a finite source triple p,q,r, the normalization is A(z)=((z-p)/(z-r))*((q-r)/(q-p)).

Image constraints can also determine coefficients directly. To send (0,2,infinity) to (0,1,4), start with b=0. Rescale to c=1, then use the image of infinity to get a=4. The remaining condition is 8/(2+d)=1, giving d=6. Thus T(z)=4z/(z+6). Its determinant is 24, and substituting the three sources verifies the images.

If infinity must remain infinity, c=0 and an affine map is enough.

Transferring boundary values with the Cayley map

The Cayley map C(z)=(z-i)/(z+i) takes the upper half-plane bijectively to the unit disc. Its inverse is i(1+w)/(1-w). The inequalities |C(z)|<1 for Im z>0 and Im C^-1(w)>0 for |w|<1 verify both directions.

Finite real inputs map to the unit circle except for 1. The missing point is C(infinity). To give continuous boundary values on the whole circle, start with continuous real-line data g that have the same finite limit at both ends. Assign that limit to g(infinity). The disc data are h(w)=g(C^-1(w)), including h(1)=g(infinity).

For example, if g(x)=(7x^2+1)/(x^2+3), dividing by x^2 shows that g(infinity)=7. Thus h(1)=7.

Once a harmonic disc solution u has these data, define v(z)=u(C(z)). The chain rule gives Delta v=|C'|^2*(Delta u) composed with C, so Delta v=0. This transfers the homogeneous Laplace equation; a nonzero forcing term would acquire a scale factor.

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Conformal Maps and Mobius Transformations · Mathematics, ages 21 to 22 · LightMySky