Chapter 6 Partial Differential Equations
Chapter 6 Partial Differential Equations
Chapter 6 Partial Differential Equations
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6.3. CHARACTERISTICS AND HIGHER ORDER EQUATIONS 35<br />
where v could represent either ϕ or ψ. We note that (6.3.11) can be factored into<br />
[ ( √ ) ][ ( √ ) ]<br />
−b + b2 − ac<br />
−b − b2 − ac<br />
a v x −<br />
v y v x −<br />
v y . (6.3.12)<br />
a<br />
a<br />
Thus from (6.3.12) we seek ϕ and ψ so that, for example,<br />
[ ( √ ) ]<br />
−b + b2 − ac<br />
ϕ x −<br />
ϕ y =0, (6.3.13)<br />
a<br />
and<br />
[<br />
ψ x −<br />
( √ ) ]<br />
−b − b2 − ac<br />
ψ y =0. (6.3.14)<br />
a<br />
With these choices (6.3.11) is satisfied with v given by ϕ and ψ. In addition we must<br />
impose a noncharacteristic solvability condition<br />
∣<br />
∂(ϕ, ψ) ∣∣∣∣<br />
∂(x, y) = ϕ x<br />
ψ x<br />
ϕ y<br />
ψ y<br />
∣ ∣∣∣∣<br />
( √ )<br />
−b + b2 − ac<br />
=<br />
ϕ y ψ y −<br />
a<br />
( −b −<br />
√<br />
b2 − ac<br />
a<br />
)<br />
ϕ y ψ y<br />
= 2 a<br />
√<br />
b2 − ac ϕ y ψ y ≠0. (6.3.15)<br />
A solution of (6.3.13) is found by solving<br />
dx<br />
dt =1,<br />
( √ )<br />
dy −b +<br />
dt = − b2 − ac<br />
,<br />
a<br />
dϕ<br />
dt =0.<br />
For this problem we take the initial conditions<br />
x 0 (s) =x 0 ,y 0 (s) =y 0 + s,<br />
ϕ 0 (s) =s.<br />
With this choice we find (in our earlier notation we used a and b which are not the<br />
same as those occuring in the present problem)<br />
∣ ∣∣∣∣∣∣ a x ′ 1 0<br />
0(s)<br />
∣b<br />
y 0(s)<br />
′ ∣ = ( √ )<br />
b − b2 − ac<br />
≠0. (6.3.16)<br />
1<br />
a ∣