How do I undo a Fourier cosine transform to solve a heat equation problem?

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SUMMARY

The discussion centers on solving the heat equation problem defined by the partial differential equation (PDE) \( u_t = u_{xx} - 4u \) on a semi-infinite interval. The solution involves applying the Fourier cosine series, resulting in the expression \( C(u) = \frac{2}{\pi(\omega^2 + 4)} + C_1 e^{-(\omega^2 + 4)t} \). The user, Josh, seeks guidance on how to perform the inverse Fourier cosine transform to retrieve the original function \( u(x, t) \) from \( C(u) \). The solution confirms that the inverse transform is the correct approach to obtain \( u(x, t) \).

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Homework Statement


Find the solution ##u(x, t)## to the semi-infinite interval problem

$$ u_t = u_{xx} - 4u, \hspace{2 mm} 0 < x < \infty, \hspace{2 mm} t>0\\
u_x(0,t) = -1, \hspace{2 mm} t>0\\
\lim_{x \to \infty}u(x,t) = 0, \hspace{2 mm} t>0\\
u(x,0) = e^{-x}, \hspace{2 mm} 0 \leq x < \infty.$$

Homework Equations


fourier cosine series, which I shall denote ##C(u)## when in variable ##x## operating over some function ##u##.

The Attempt at a Solution


after taking Fourier cosine series of the governing PDE i arrive at $$
\frac{\partial}{\partial t}C(u) = \frac{2}{\pi} - \omega^2 C(u) -4C(u) \implies\\
C(u) = \frac{2}{\pi(\omega^2 + 4)} + C_1e^{-(\omega^2 +4)t}$$
Notice ##C(u(x,0)) = C(e^{-x}) = \frac{2}{\pi(1+\omega^2)}##. This implies ##C_1 = \frac{2}{\pi(1+\omega^2)} - \frac{2}{\pi(\omega^2 + 4)} ##. Thus we arrive at $$
C(u) = \frac{2}{\pi(\omega^2 + 4)} + \frac{2}{\pi}\left[ \frac{1}{(1+\omega^2)} - \frac{1}{(\omega^2 + 4)} \right] e^{-(\omega^2 +4)t}$$
I have skipped some in-between steps, but I think the idea is here. My question is, how do I undo this Fourier cosine transform, if I have arrived to a correct solution?

Thanks so much!

Josh
 
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Use the inverse Fourier cosine transform
 
Cool, that's what I did! Just wanted to make sure my work was correct. Thanks!
 

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