Fourier Transform and Shifting in Solving ODEs?

cloud18
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Find the solution (in integral form) of the equation:

<br /> u(x+1,t) - 2u(x,t) + u(x-1,t) = u_t <br />
u(x,0) = f(x)

Hint: Use the shift formula

<br /> F[f(ax-b)] = \frac{\exp{i\omega b/a}}{|a|} \overline{f}(\omega/a)<br />

So I took the Fourier transform of each term using the shift formula:

<br /> \exp{(-i\omega)} \overline{u} - 2\overline{u} + \exp{(i\omega)}\overline{u} = \overline{u}_t<br />

But I don't think this is correct thus far...
 
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Why don't you think it is right? Also, that expression is not fully simplified. Maybe you were expecting something with sinusoids?
 
Well I guess I get stuck on how to solve the ODE:

<br /> (\exp{(-i\omega)} - 2 + \exp{(i\omega)})\overline{u} = \overline{u}_t<br />

So (\exp{(-i\omega)} - 2 + \exp{(i\omega)}) can be treated as a constant with respect to t. But when I solve I get exponents raised to exponents...The answer is suppose to be (limits of integration -inf to +inf):

<br /> \frac{1}{2\pi}\int{e^{-i\omega x-2(1-\cos{\omega})t} \int{e^{i\omega\xi}f(\xi)d\xi}d\omega}<br />
 
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There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
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