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Chapter 6 Partial Differential Equations

Chapter 6 Partial Differential Equations

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22 CHAPTER 6. PARTIAL DIFFERENTIAL EQUATIONS<br />

Proof. Our regularity assumptions guarantee that the initial value problem<br />

dx<br />

dt<br />

dy<br />

dt<br />

du<br />

dt<br />

= a(x, y, u), x(s,<br />

= b(x, y, u), y(s,<br />

= c(x, y, u), u(s,<br />

0) = x 0(s)<br />

0) = y 0(s)<br />

0) = u 0(s)<br />

has a unique local solution that is C 1 in t and s. By our hypotheses<br />

⎛ ⎞<br />

∂x ∂x<br />

|J| = det ⎜ ∂t ∂s<br />

⎟<br />

⎝∂y<br />

∂y⎠<br />

=<br />

∣ a(x 0(s),y 0 (s),u 0 (s)) x ′ 0(s)<br />

b(x 0 (s),y 0 (s),u 0 (s)) y 0(s)<br />

′<br />

∣<br />

∂t ∂s t=0<br />

∣ ≠0<br />

Thus |J| ≠ 0 in a neighborhood of the initial curve C 0 and by the inverse function theorem<br />

we can solve for<br />

s = s(x, y), t = t(x, y)<br />

and s = s(x 0 (s),y 0 (s)),<br />

0=t(x 0 (s),y 0 (s)), so we can define<br />

u = u(x, y) =u(s(x, y),t(x, y)).<br />

We first note that u satisfies the initial conditions:<br />

u(x 0 (s),y 0 (s)) = u(s, 0) = u 0 (s).<br />

Furthermore, by the chain rule<br />

(<br />

)<br />

∂s<br />

au x + bu y = a u s<br />

∂x + u ∂t<br />

t<br />

∂x<br />

(<br />

∂s<br />

+ b u s<br />

=(as x + bs y )u s +(at x + bt y ))u t .<br />

)<br />

∂y + u ∂t<br />

t<br />

∂y<br />

Now by our construction of x, y, and since x t = a, y t = b, wehave<br />

and<br />

as x + bs y = s x x t + s y y t = ∂s<br />

∂t =0,<br />

at x + bt y = s x x t + t y y t = ∂t<br />

∂t =1

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