5.4 • TRIGONOMETRIC AND HYPERBOLIC F UNCT IONS 181
y
)
2
I
-K
2
- 1
-2 - 3
.1!. 2
~·=sint
x
Figure 5.7 Vertical segments mapped onto hyperbolas by w = sin(z).
10
show that the images of these vertical segments are hyperbolas in the uv plane,
as Figure 5.7 illustrates. In Chapter 10, we give a more detailed analysis of the
mapping w = sinz.
Figure 5.7 suggests one big difference between the real and complex sine
functions. The real sine has the property that lsin xi ~ 1 for all real x. In Figure
5.7, however, the modulus of the complex sine appears to be unbounded, which
is indeed the case. Using Identity (5-33) gives
lsin zl^2 = lsinzcoshy + icosxsinhyl^2
= sin^2 xcosh^2 y+cos^2 xsinh^2 y
= sin^2 x (cosh^2 y -sinh^2 y) + sinh^2 y (cos^2 x + sin^2 x).
The identities cosh^2 y - sinh^2 y = 1 and cos^2 x + sin^2 x = 1 then yield
lsin zl
2
= sin^2 x + s in h^2 y.
A similar derivation produces
lcoszl^2 = cos^2 x + sinh^2 y.
If we set z = xo + iy in Identity (5-36) and let y -+ oo, we get
lim lsin (xo + ·iy)l^2 = s in^2 xo + lim sinh^2 y = oo.
y -oo y -oo
(5-36)
(5-37)
As advertised, we have shown that sin z is not a bounded function; it is also
evident from Identity (5-37) that cos z is unbounded.
The periodic character of the trigonometric functions makes apparent that
any point in their ranges is actually the image of infinitely many points.