14.12.2012 Views

Complex Analysis - Maths KU

Complex Analysis - Maths KU

Complex Analysis - Maths KU

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

v<br />

B′<br />

C′<br />

w 0<br />

∇Φ<br />

N<br />

Φ = c0 u<br />

Figure 7.52 Figure for the proof of<br />

Theorem 7.8<br />

7.5 Applications 435<br />

Proof Assume that f and h satisfythe hypothesis of the theorem. Let<br />

z0 = x0 + iy0 be a point on C and let w0 = u0 + iv0 = f(z0) be its image on<br />

C ′ . Recall from calculus that if N is a normal vector to C ′ at w0, then the<br />

normal derivative at w0 is given bythe dot product<br />

dΦ<br />

dN<br />

= ∇Φ · N,<br />

where ∇Φ is the gradient vector Φu(u0, v0)i +Φv(u0, v0)j. The condition<br />

dΦ/dN = 0 implies that ∇Φ and N are orthogonal, or, equivalently, that<br />

∇Φ is a tangent vector to C ′ at w0. Let B ′ be the level curve Φ(u, v) =c0<br />

containing (u0, v0). In multivariable calculus, you learned that the gradient<br />

vector ∇Φ is orthogonal to the level curve B ′ . Thus, since the gradient is<br />

tangent to C ′ and orthogonal to B ′ , we conclude that C ′ is orthogonal to B ′<br />

at w0. See Figure 7.52.<br />

Now consider the level curve B in the z-plane given by<br />

φ(x, y) =Φ(u(x, y),v(x, y)) = c0.<br />

The point (x0, y0) isonB and the gradient vector ∇φ is orthogonal to B at<br />

this point. Moreover, given anypoint (x, y) onB in the z-plane, we have<br />

that the point (u(x, y), v(x, y)) is on B ′ in the w-plane. That is, the image<br />

of B under w = f(z) isB ′ . The curve C intersects B at z0, and because f<br />

is conformal at z0, it follows that the angle between C and B at z0 is the<br />

same as the angle between C ′ and B ′ at w0. In the preceding paragraph we<br />

found that this angle is π/2, and so C and B are orthogonal at z0. Since<br />

∇φ is orthogonal to B, we must have that ∇φ is tangent to C. If n is a<br />

normal vector to C at z0, then we have shown that ∇φ and n are orthogonal.<br />

Therefore,<br />

dφ<br />

= ∇φ · n =0.<br />

dn<br />

Theorem 7.8 gives us a procedure for solving Nuemann problems associated<br />

with boundaryconditions of the form dφ/dn = 0. Namely, we follow<br />

the same four steps given on page 429 to solve a Dirichlet problem. In Step<br />

1, however, we find a conformal mapping from D onto D ′ . Since conformal<br />

mappings preserve boundaryconditions of the form dφ/dn = 0, solving the<br />

associated Nuemann problem in D ′ will give us a solution of the original<br />

Nuemann problem. Because analytic mappings are conformal at noncritical<br />

points, this approach also works with mixed boundaryconditions. Roughly,<br />

these are boundaryconditions where values of φ are specified on some boundarycurves,<br />

whereas the normal derivative is required to satisfydφ/dn =0on<br />

other boundarycurves.<br />

EXAMPLE 3 A Heat Flow Application<br />

Find the steady-state temperature φ in the first quadrant, shown in color in<br />

Figure 7.53(a), which satisfies the indicated mixed boundaryconditions.<br />

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!