Chapter 6 Partial Differential Equations
Chapter 6 Partial Differential Equations
Chapter 6 Partial Differential Equations
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6.2. LINEAR AND QUASILINEAR EQUATIONS OF FIRST ORDER 15<br />
fact that ∂s k<br />
∂t = 0, since s k and t are functionally independent, and ∂t<br />
∂t<br />
(<br />
n∑ ∂u<br />
n∑ n−1<br />
)<br />
∑ ∂u ∂s k<br />
a j = a j + ∂u ∂t<br />
∂x<br />
j=1 j ∂s<br />
j=1<br />
k ∂x j ∂t ∂x j<br />
k=1<br />
This completes the proof.<br />
=<br />
=<br />
=<br />
∑n−1<br />
k=1<br />
∑n−1<br />
k=1<br />
∑n−1<br />
k=1<br />
∂u<br />
∂s k<br />
∂u<br />
∂s k<br />
n∑<br />
j=1<br />
n∑<br />
j=1<br />
∂u<br />
∂s k<br />
∂s k<br />
=0+ ∂u<br />
∂t = b.<br />
∂s k<br />
a j + ∂u<br />
∂x j ∂t<br />
∂s k ∂x j<br />
∂x j ∂t + ∂u<br />
∂t<br />
∂t + ∂u ∂t<br />
∂t ∂t<br />
n∑<br />
j=1<br />
a j<br />
∂t<br />
∂x j<br />
n∑<br />
j=1<br />
∂x j<br />
∂t<br />
∂t<br />
∂x j<br />
= 1 we have<br />
Example 6.2.9. In R 3 solve the linear initial value problem Lu = x 1 ∂ 1 u+2x 2 ∂ 2 +∂ 3 u =3u<br />
with u = ϕ(x 1 ,x 2 ) on the plane x 3 =0.<br />
Solvability: We could observe that the solvability condition is satisfied by considering The<br />
vector field A(x) =(x 1 , 2x 2 , 1) and the characteristic manifold<br />
Char x (L) ={ξ =(ξ 1 ,ξ 2 ,ξ 3 ) ≠0:A(x) · ξ =0}.<br />
We note that the initial surface S in this case is x 3 = 0 with constant normal vector ν =<br />
(0, 0, 1). In the present case we see that<br />
A(x) · ν =1≠0<br />
so the surface is non-characteristic.<br />
We could also note that with s =(s 1 ,s 2 ) ∈ R 3−1 and<br />
g(s) =(g 1 (s),g 2 (s),g 3 (s))=(s 1 ,s 2 , 0)<br />
paramterizing the surface S we have for (6.2.7)<br />
⎛<br />
1 0 s 1<br />
⎞<br />
det ⎝0 1 2s 2<br />
⎠ = ϕ(s 1 ,s 2 ).<br />
0 0 ϕ(s 1 ,s 2 )