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Solutions to problem 1, 2, and 3 from the math 412 group work in spring 2009. The problems involve determining differentiability, finding singular points, and defining v(x, y) for an entire function with given real constants a, b, c, and d.
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Math 412 Group Work #7 Spring 2009 SOLUTIONS
Problem 1. Let f (z) = x^2 + y^2 + i(2xy).
(a): Use the Cauchy-Riemann equations to determine where f is differen- tiable.
SOLUTION: We have
ux(x, y) = 2x, uy(x, y) = 2y, vx(x, y) = 2y, vy(x, y) = 2x.
For all (x, y) ∈ R^2 , we have ux = vy. However, uy = −vx only holds if 2y = − 2 y; that is, uy = −vx if and only if y = 0. Thus, the Cauchy-Riemann equations only hold for points (x, 0) along the real-axis of the complex plane. Thus, f is only differentiable along the real axis: {z ∈ C : Im(z) = 0}.
(b): Evaluate the derivative at the points z 0 where f ′(z 0 ) exists.
SOLUTION: We have
f ′(z) = f ′(x + iy) = ux(x, y) + ivx(x, y) = 2x + i(2y) = 2x,
since y = 0 along the real axis.
(c): Determine all singular points of the function f.
SOLUTION: The only points of differentiability of f lie along the real axis, and no such point possesses a neighborhood centered at it so that all points in the neighbor- hood are differentiable. Thus, there are no points of analyticity of f , which implies that all points of C are singular points of f.
Problem 2. Suppose that f : C → C is an entire, real-valued function. Show that f must be a constant function.
SOLUTION: Since f (x+iy) = u(x, y) is real-valued (i.e. v(x, y) = 0), we know that vx(x, y) = vy(x, y) = 0 for all (x, y) ∈ R^2. Thus, since ux(x, y) = vy(x, y) = 0 and uy(x, y) = −vx(x, y) = 0, we conclude that u(x, y) = c (c ∈ C) must be a constant function. Thus, f (x + iy) = u(x, y) = c is a constant function.
Problem 3. Suppose that f (x + iy) = u(x, y) + iv(x, y). For what relations among the real constants a, b, c, d with
u(x, y) = ax^3 + bx^2 y + cxy^2 + dy^3
can v(x, y) be defined so that f is an entire function?
SOLUTION: An entire function must be differentiable throughout C, which implies that the Cauchy-Riemann equations must hold throughout C. In this case, we have
ux(x, y) = 3ax^2 + 2bxy + cy^2 and uy(x, y) = bx^2 + 2cxy + 3dy^2.
Hence, in order for the Cauchy-Riemann equations to hold, we must have
vy(x, y) = 3ax^2 + 2bxy + cy^2 and vx(x, y) = −bx^2 − 2 cxy − 3 dy^2.
Integrating the required formula for vy(x, y) with respect to y, we obtain
v(x, y) = 3ax^2 y + bxy^2 +
cy^3 + g(x),
and differentiating this with respect to x, we find that
vx(x, y) = 6axy + by^2 + g′(x).
Comparing the two formulas for vx(x, y), we see that
6 a = − 2 c, b = − 3 d,
and g′(x) = −bx^2 , so that g(x) = −^13 bx^3. Hence, the required relations on a, b, c, d are that c = − 3 a and b = − 3 d.