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Complex Analysis - Maths KU

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3.2 Cauchy-Riemann Equations 153<br />

We now let ∆z → 0 along a vertical line. With ∆x = 0 and ∆z = i∆y,<br />

(3) becomes<br />

f ′ u(x, y +∆y) − u(x, y)<br />

(z) = lim<br />

∆y→0 i∆y<br />

v(x, y +∆y) − v(x, y)<br />

+ i lim<br />

. (6)<br />

∆y→0 i∆y<br />

In this case (6) shows us that ∂u/∂y and ∂v/∂y exist at z and that<br />

f ′ (z) =−i ∂u<br />

∂y<br />

∂v<br />

+ . (7)<br />

∂y<br />

By equating the real and imaginary parts of (5) and (7) we obtain the pair of<br />

equations in (1). ✎<br />

Because Theorem 3.4 states that the Cauchy-Riemann equations (1) hold<br />

at z as a necessary consequence of f being differentiable at z, we cannot use<br />

the theorem to help us determine where f is differentiable. But it is important<br />

to realize that Theorem 3.4 can tell us where a function f does not possess a<br />

derivative. If the equations in (1) are not satisfied at a point z, then f cannot<br />

be differentiable at z. We have already seen in Example 3 of Section 3.1 that<br />

f(z) =x +4iy is not differentiable at any point z. If we identify u = x and<br />

v =4y, then ∂u/∂x =1,∂v/∂y=4, ∂u/∂y =0, and ∂v/∂x =0. In view of<br />

∂u ∂v<br />

=1�=<br />

∂x ∂y =4<br />

the two equations in (1) cannot be simultaneously satisfied at any point z. In<br />

other words, f is nowhere differentiable.<br />

It also follows from Theorem 3.4 that if a complex function f(z) =<br />

u(x, y)+iv(x, y) is analytic throughout a domain D, then the real functions u<br />

and v satisfy the Cauchy-Riemann equations (1) at every point<br />

in D.<br />

EXAMPLE 1 Verifying Theorem 3.4<br />

The polynomial function f(z) =z 2 +z is analytic for all z and can be written as<br />

f(z) =x 2 −y 2 +x+i(2xy+y). Thus, u(x, y) =x 2 −y 2 +x and v(x, y) =2xy+y.<br />

Foranypoint(x, y) in the complex plane we see that the Cauchy-Riemann<br />

equations are satisfied:<br />

∂u<br />

∂v<br />

=2x +1=<br />

∂x ∂y<br />

and<br />

∂u<br />

∂y<br />

= −2y = − ∂v<br />

∂x .

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