Page 37 - Calculus with Complex Numbers
P. 37

Theorem 2  For u + i t? = f(x + iy) with continuous partial derivatives bu/bx
     élu/él y, é) v/bx, g??/i y the function flz) is differentiable at z if and only if the
     Cauchy-lkiemann equations


         bu   gr    bv    gu
         91  by     91    by


     are satislied.
     Proof We proved necessity above. For sufliciency we refer the reader to rigorous
     books on complex analysis.



     3.4  G eom  etri c signifi cance of the com p Iex derivative

     For a real function f @) of a real variable .x the equation of the tangent to the
     graph y = f @) at .x = a is


        )' = f (tz) + (x - tz) f' (J).


     For a complex function f (z) of a complex variable z, the equation of the tangent
     plane (in 4 dimensions) to the graph w = flz) at z = a is


        w = fla) + (z - a)f'(a) = ztz + B,


     where .4 = f (tz), B = fla) - af (tz).
       The geometric effect of the linear function w = ztz + B is a rotatioa a scaling,
     and a translation. The rotation is through the angle arg .4 the scaling is by the

     factor I.4 I. The translation is through a distance IB I in the direction arg B.


       What this tells us about the transformation w = f (z) is that near z = a the
     effect is approximately a rotation through arg f' (tz), and a scaling by I f (tz) I . For
     example, if a = in'/l and flz) = ez, then we have fla) = ein'/l = i. Also
     f' (tz) = cl = ein'/l = i . So the effect near z = a is a rotation through 90O
     anticlockwise (see Figure 3.4). lf b = in'/l + 1, then we have flb) = f'Lb) =
     ei, so the effect locally is now a scaling by c, and again a rotation through 90O
     anticlockwise (see Figtlre 3.4).
       The fact that w = flz) acts locally like a rotation through arg f (z) explains
     why curves which intersect at a certain angle in the z-plane are transformed under
     the action of w = flz) to curves which intersect at the same angle in the w-plane.
     This is the characteristic property of a conformal flll////ïrl,j' which is important for
     the applications to lluid mechanics.
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