bob321
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Hi folks,
Given the following heat equation
u_t = u_{xx} + t - x^2,
I'd like to find all solutions u(x,t)\in C^2(\mathbb{R}^2) such that the quotient
|u(x,t)| / (|x|^5 + |t|^5)
goes to zero as the sum |x| + |t| goes to infinity.
I know how to do the same problem with the usual heat equation u_t = u_{xx}, but I'm not entirely sure how to deal with this extra t - x^2 term. I suspect I can still start by taking the Fourier transform (in x) of each side to get something like:
\partial_t \hat{u}(\xi,t) = \widehat{\partial_t u}(\xi, t) = -|\xi|^2 \hat{u}(\xi,t) + \widehat{t-x^2}(\xi) = -|\xi|^2\hat{u}(\xi, t) + t\delta(\xi) - \delta^{\prime\prime}(\xi),
which gives me an ODE in t that is easy enough to solve. The issue is that I think this method only gives me smooth (by which I mean infinitely differentiable) solutions. Are there other C^2 solutions that I am missing with this approach?
Thanks in advance for any help.
Given the following heat equation
u_t = u_{xx} + t - x^2,
I'd like to find all solutions u(x,t)\in C^2(\mathbb{R}^2) such that the quotient
|u(x,t)| / (|x|^5 + |t|^5)
goes to zero as the sum |x| + |t| goes to infinity.
I know how to do the same problem with the usual heat equation u_t = u_{xx}, but I'm not entirely sure how to deal with this extra t - x^2 term. I suspect I can still start by taking the Fourier transform (in x) of each side to get something like:
\partial_t \hat{u}(\xi,t) = \widehat{\partial_t u}(\xi, t) = -|\xi|^2 \hat{u}(\xi,t) + \widehat{t-x^2}(\xi) = -|\xi|^2\hat{u}(\xi, t) + t\delta(\xi) - \delta^{\prime\prime}(\xi),
which gives me an ODE in t that is easy enough to solve. The issue is that I think this method only gives me smooth (by which I mean infinitely differentiable) solutions. Are there other C^2 solutions that I am missing with this approach?
Thanks in advance for any help.