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Textbook 'Applied Partial Differential Equations Revised Edition' by Jhon Ockenden, Sam Howison, Andrew Lacey, and Alexander

Show that Lespl= 14 + i:(8 – c)]dx = Vesp [.(4.70*] where i = V-1. Hint: (a) Use the Eulers formula exp[it] = cost + i sint;

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Answer #1

a.)

Consider the given integrable function as

exp(t+i-)) ete-) = et (cos(A(-0)+i sin(A(r-) -12t

The integration can be separated as

Atcos(A(r-) dA+i -12t e exp(-t+iX(-) dA = sin(A(r OS dA

Since tcos(A(x-) e is an even function, the first integral is

t cos(A-) dA At cos(A( )) dA 2 COs e

Since sin((-) e is an odd function, the second integral is

t sin((r - ) dA 0 e

So the the integral we need to find is e-t cos(A(r )) dX 2

b.)

Define vdp and A .

By substituting the above transformations into the integral, we get

2 e-At cos(A(r ) d e cos(uz) du 2 COS.

c.)

Let e cos(uz) du

Let us find the derivative of I with respect to z, i.e.,

\frac{dI(z)}{dz}=\int_{0}^{\infty}e^{-\mu^2}\frac{d}{dz}(\cos(\mu z))\;d\mu=-\int_{0}^{\infty}\mu e^{-\mu^2}\sin(\mu z)\;d\mu

Use the integration by parts to I, then we get

eHcos(z) du sin(uz) I (z) sin(uz) ) du e 2 2

()2dI z dz I 0 dz

Solution of this first order ODE is

I(z)=I(0)e^{-\int \frac{z}{2}\;dz}=I(0)e^{-\frac{z^2}{4}}

d.)

I(0)=\int_{0}^{\infty}e^{-\mu^2}\cos(\mu (0))\;d\mu=\int_{0}^{\infty}e^{-\mu^2}\;d\mu

Define w=\mu^2\implies dw=2\mu\;d\mu\implies 2w^{1/2}\;d\mu . Substitute these into the integral to get

I(0)=\frac{1}{2}\int_{0}^{\infty}e^{-w}w^{-1/2}\;dw=\frac{\Gamma(1/2)}{2}=\frac{\sqrt{\pi}}{2}

The integral value is

\frac{2}{\sqrt{t}}\frac{\sqrt{\pi}}{2}e^{-\frac{z^2}{4}}=\sqrt{\frac{\pi}{t}}exp(-\frac{(x-\xi)^2}{4t})

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