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Material Type: Assignment; Class: Introduction to Complex Analysis; Subject: Mathematics; University: University of California - Berkeley; Term: Fall 2006;
Typology: Assignments
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Prof. W. Kahan Math. 185 Page 1/
Exercise 19: By integrating derivatives of a harmonic function g(x, y) we recover one of its harmonic conjugates h(x, y) and then set ƒ(x + ı y) := g(x, y) + ı h(x, y) to recover an analytic function ƒ(z). The recovery of an analytic expression ƒ from a harmonic expression g that is also a real analytic function of each of its arguments can be achieved more easily by setting ƒ(z) := 2g((zo +z)/2, ı (zo –z)/2) for any zo = x (^) o + ı yo inside the domain of g ; explain why. If
this procedure fails to recover a function ƒ analytic throughout the domain of g , explain why.
Explanation: A well-formed expression provides a formula to evaluate an analytic function by means of finitely many operations of addition, subtraction, multiplication, division, roots, log,
for the harmonic function g that satisfies ƒ(x + ı y) = g(x, y) + ı h(x, y) when x and y are real. This g(x, y) is a formula also for a real analytic function of each of x and y when they are reinterpreted as complex variables. And after suitable complex expressions are substituted for x and y in the formula 2g((w+z)/2, ı (w–z)/2) it simplifies to ƒ(z) + (an expression in w) , which recovers ƒ from g within a “constant” without integrating derivatives. Does this always work?
The complex conjugate of ƒ(x + ı y) := g(x, y) + ı h(x, y) is ƒ(x + ı y) := g(x, y) – ı h(x, y) when x and y are real. This ƒ(z) is generally not an analytic function of z because g and –h violate the Cauchy-Riemann conditions. However Φ(z) := ƒ(z) is an analytic function of z because Φ(x + ı y) = g(x, –y) – ı h(x, –y) for real x and y has real and imaginary parts g(x, –y) and –h(x, –y) that inherit satisfaction of the Cauchy-Riemann conditions from g(x, y) and h(x, y). For later reference note that the domain of Φ(z) is the complex conjugate of the domain of ƒ.
We are given a harmonic g and wish to recover ƒ (within a constant) without first constructing g ’s harmonic conjugate h (within a constant). Eliminating h from foregoing formulas yields 2g(x, y) = ƒ(x + ı y) + Φ (x – ı y). This relation among functions is also, presumably, a relation among expressions (formulas), and as such is a relation among formulas into which independent complex variables may be substituted for x and y because all three functions are analytic in their arguments no matter whether real or complex. An apt substitution is suggested by the equations x = (z+z)/2 and y = ı (z–z)/2 in which z is replaced by an independent complex variable w , say. Thus 2g((w+z)/2, ı (w–z)/2) = ƒ(z) + Φ(w) = ƒ(z) + ƒ(w) provided w is chosen in the domain of Φ , which puts w in the domain of ƒ and of ƒ. The last equation delivers a formula for ƒ(z) within a constant when w is held constant. Almost.
This formula for ƒ can malfunction in two ways. One way occurs when w does not lie in the
domain of ƒ ; for example when g(x, y) = x^2 – y 2 – y/(x^2 + y^2 ) the choice w := 0 ± ı 0 makes
because g(x, y) misbehaves around (0, 0) in the (x, y)-plane, so ƒ(z) must be expected to have a singularity at z = 0 ± ı 0 in the z-plane. The second kind of malfunction is more subtle.
If not simply connected, the domain in the (x, y)-plane whereon g(x, y) is harmonic may extend beyond the domain in the z-plane whereon ƒ(z) is differentiable. Try the Principal Value of
2g((w+z)/2, ı (w–z)/2) = log(w·z) is discontinuous across the ray z/w < 0 instead of z < 0.
In general 2g((w+z)/2, ı (w–z)/2) – ƒ(z) may take several “constant” values. Try ƒ(z) := √(2z).