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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 ∣

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