An Asymptotic Solution of Linear Second Order Hyperbolic Differential Equations

Cover An Asymptotic Solution of Linear Second Order Hyperbolic Differential Equations
An Asymptotic Solution of Linear Second Order Hyperbolic Differential Equations
Morris Kline
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In performing the differentiation with respect to x. First and then with respect to t one does end up with the term U. (x, 0) f(t)in addition to the other terms in (3. 6). However since 'J(x, t) = for t = except on S, we conclude that Uj(x, 0) = .
- 11 - tt a' a ; at' (3. -?) J u(x. T-r)f(V)d'r'= a** I J U^^(x, t-y)f('r)dY+ [U(x. T^)]f' (t-t^) * [nt(x, ti)]f(t-t^) r .
To perform the differentia tiocs called for in the first-order terms in (3.^) we may use the results already ohtained. For k = l
..., 2, ... , n-l, (3. 8) h^^ jTiu, t-r)f(Y)d'T' = •b'^l J u^Cx. T-iOf (Y)d'y - [u(^. Til]f (t-t^vj i .
For k = n v/e have (3. 9) b*^ f n(x, t-V)f(Y)dy= h* J U^U, t-'Y)f(V)dV+ [U(x, t^i]f(t-t^) I .
I ° J Tor the remsininf term in (3.^) we merely restate that (3. 10) c J u(x, t-r)f(r)dr = c I" uCx. T-T^f (r)dr .
To verify the correctness of the Duhamel principle, that is, that (3.^^) is correct, we must now pdd up the terms in equations (3. 5) to (3. 10). We find on the right side th8. T the terms involving integrals amount to J L(u(x, t-'0) f(r)dV, Since U(j', t) is required to satisfy L(u) = for t-Y t^, these terms add up to zero.


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