Chapter 6 Partial Differential Equations
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