The solution of heat equation satisfies $u(x,t)rightarrow 0$ as $|x|+trightarrow infty$
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Suppose $u$ solution of the heat equation $u_{t}=u_{xx}$, where $fin S(mathbb{R})$ belongs to Schwartz space, $u(x,t)=left(f*mathcal{H}_{t}right)(x)$ setting $u(x,0)=f(x)$.
I need to prove that $u$ is continuous on the closure of the upper half-plane, and vanishes at infinity, that is,
$$u(x,t)rightarrow 0quadtextrm{as}quad |x|+trightarrow infty. $$
The hint is to the second part is to prove that:
$displaystyle (i)quad |u(x,t)|leqfrac{C}{sqrt{t}}$
$displaystyle (ii)quad |u(x,t)|leqfrac{C}{left(1+|x|^{2}right)}+Ct^{-1/2}e^{-cx^{2}/t}$
and using $(i)$ when $|x|leq t$, and using $(ii)$ otherwise.
$u$ is continuous because it is a convolution of two continuous function. But the second part is confuse to me.
All I have is
$$displaystyle|u(x,t)|leq int_{-infty}^{infty}|hat{f}(xi)|cdot |e^{-4pi^{2}txi^{2}}|dxi$$
pde fourier-analysis convolution heat-equation
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up vote
0
down vote
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Suppose $u$ solution of the heat equation $u_{t}=u_{xx}$, where $fin S(mathbb{R})$ belongs to Schwartz space, $u(x,t)=left(f*mathcal{H}_{t}right)(x)$ setting $u(x,0)=f(x)$.
I need to prove that $u$ is continuous on the closure of the upper half-plane, and vanishes at infinity, that is,
$$u(x,t)rightarrow 0quadtextrm{as}quad |x|+trightarrow infty. $$
The hint is to the second part is to prove that:
$displaystyle (i)quad |u(x,t)|leqfrac{C}{sqrt{t}}$
$displaystyle (ii)quad |u(x,t)|leqfrac{C}{left(1+|x|^{2}right)}+Ct^{-1/2}e^{-cx^{2}/t}$
and using $(i)$ when $|x|leq t$, and using $(ii)$ otherwise.
$u$ is continuous because it is a convolution of two continuous function. But the second part is confuse to me.
All I have is
$$displaystyle|u(x,t)|leq int_{-infty}^{infty}|hat{f}(xi)|cdot |e^{-4pi^{2}txi^{2}}|dxi$$
pde fourier-analysis convolution heat-equation
add a comment |
up vote
0
down vote
favorite
up vote
0
down vote
favorite
Suppose $u$ solution of the heat equation $u_{t}=u_{xx}$, where $fin S(mathbb{R})$ belongs to Schwartz space, $u(x,t)=left(f*mathcal{H}_{t}right)(x)$ setting $u(x,0)=f(x)$.
I need to prove that $u$ is continuous on the closure of the upper half-plane, and vanishes at infinity, that is,
$$u(x,t)rightarrow 0quadtextrm{as}quad |x|+trightarrow infty. $$
The hint is to the second part is to prove that:
$displaystyle (i)quad |u(x,t)|leqfrac{C}{sqrt{t}}$
$displaystyle (ii)quad |u(x,t)|leqfrac{C}{left(1+|x|^{2}right)}+Ct^{-1/2}e^{-cx^{2}/t}$
and using $(i)$ when $|x|leq t$, and using $(ii)$ otherwise.
$u$ is continuous because it is a convolution of two continuous function. But the second part is confuse to me.
All I have is
$$displaystyle|u(x,t)|leq int_{-infty}^{infty}|hat{f}(xi)|cdot |e^{-4pi^{2}txi^{2}}|dxi$$
pde fourier-analysis convolution heat-equation
Suppose $u$ solution of the heat equation $u_{t}=u_{xx}$, where $fin S(mathbb{R})$ belongs to Schwartz space, $u(x,t)=left(f*mathcal{H}_{t}right)(x)$ setting $u(x,0)=f(x)$.
I need to prove that $u$ is continuous on the closure of the upper half-plane, and vanishes at infinity, that is,
$$u(x,t)rightarrow 0quadtextrm{as}quad |x|+trightarrow infty. $$
The hint is to the second part is to prove that:
$displaystyle (i)quad |u(x,t)|leqfrac{C}{sqrt{t}}$
$displaystyle (ii)quad |u(x,t)|leqfrac{C}{left(1+|x|^{2}right)}+Ct^{-1/2}e^{-cx^{2}/t}$
and using $(i)$ when $|x|leq t$, and using $(ii)$ otherwise.
$u$ is continuous because it is a convolution of two continuous function. But the second part is confuse to me.
All I have is
$$displaystyle|u(x,t)|leq int_{-infty}^{infty}|hat{f}(xi)|cdot |e^{-4pi^{2}txi^{2}}|dxi$$
pde fourier-analysis convolution heat-equation
pde fourier-analysis convolution heat-equation
asked Nov 17 at 22:51
Mateus Rocha
781116
781116
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