Solutions of linear PDE in the sense of distributions Announcing the arrival of Valued Associate #679: Cesar Manara Planned maintenance scheduled April 23, 2019 at 00:00UTC (8:00pm US/Eastern)Does multiplication commute with taking of fundamental solution (heat equation)The Dirac impulse and Fourier transformLinearization of Gross-Pitaevskii-EquationDo 3-D vectors of distributions (specifically vectors containing delta functions) have Helmholtz decompositions?Question on Helmholtz Equation in the senes of distributionsConvergence of a certain family of functions in the sense of distributionsShowing a solution of a PDE is bounded.Solving an PDE with the Fourier TransformFormal derivation of the Fourier transform of Dirac delta using a distributionDerivation of the Fourier Transform of a PDE
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Solutions of linear PDE in the sense of distributions
Announcing the arrival of Valued Associate #679: Cesar Manara
Planned maintenance scheduled April 23, 2019 at 00:00UTC (8:00pm US/Eastern)Does multiplication commute with taking of fundamental solution (heat equation)The Dirac impulse and Fourier transformLinearization of Gross-Pitaevskii-EquationDo 3-D vectors of distributions (specifically vectors containing delta functions) have Helmholtz decompositions?Question on Helmholtz Equation in the senes of distributionsConvergence of a certain family of functions in the sense of distributionsShowing a solution of a PDE is bounded.Solving an PDE with the Fourier TransformFormal derivation of the Fourier transform of Dirac delta using a distributionDerivation of the Fourier Transform of a PDE
$begingroup$
Let us consider the wave equation written in the form
$$
partial_ttphi-Deltaphi+phi=0.
$$
By a Fourier transform, this takes the form
$$
(k_0^2-bf k^2-1)phi(k)=0.
$$
This has as a solution, in the sense of distributions,
$$
phi(k)=A(k)delta(k_0^2-bf k^2-1).
$$
It is easy to see that, by Fourier transforming back,
$$
phi(x)=intfracd^3k(2pi)^3left(fracA(bf k,sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x-isqrtbf k^2+1t-fracA(bf k,-sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x+isqrtbf k^2+1tright)
$$
that appears as a general solution of the equation we started from.
My questions are the following:
- Is this approach sound to solve a linear PDE?
- What does it happen to the Dirac equation $(igammacdotpartial-1)psi=0$ using this technique?
pde distribution-theory
$endgroup$
add a comment |
$begingroup$
Let us consider the wave equation written in the form
$$
partial_ttphi-Deltaphi+phi=0.
$$
By a Fourier transform, this takes the form
$$
(k_0^2-bf k^2-1)phi(k)=0.
$$
This has as a solution, in the sense of distributions,
$$
phi(k)=A(k)delta(k_0^2-bf k^2-1).
$$
It is easy to see that, by Fourier transforming back,
$$
phi(x)=intfracd^3k(2pi)^3left(fracA(bf k,sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x-isqrtbf k^2+1t-fracA(bf k,-sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x+isqrtbf k^2+1tright)
$$
that appears as a general solution of the equation we started from.
My questions are the following:
- Is this approach sound to solve a linear PDE?
- What does it happen to the Dirac equation $(igammacdotpartial-1)psi=0$ using this technique?
pde distribution-theory
$endgroup$
1
$begingroup$
As long as $phi$ can be assumed to not grow too fast (so that it is a Fourier transformable distribution), it is sound to use the Fourier transform to solve a linear PDE.
$endgroup$
– md2perpe
Mar 30 at 23:00
$begingroup$
Thanks a lot @md2perpe. Indeed, it appears that the textbook solution comes out naturally, provided I change the integration variable as $bf krightarrow -bf k$ in the second term.
$endgroup$
– Jon
Mar 30 at 23:09
add a comment |
$begingroup$
Let us consider the wave equation written in the form
$$
partial_ttphi-Deltaphi+phi=0.
$$
By a Fourier transform, this takes the form
$$
(k_0^2-bf k^2-1)phi(k)=0.
$$
This has as a solution, in the sense of distributions,
$$
phi(k)=A(k)delta(k_0^2-bf k^2-1).
$$
It is easy to see that, by Fourier transforming back,
$$
phi(x)=intfracd^3k(2pi)^3left(fracA(bf k,sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x-isqrtbf k^2+1t-fracA(bf k,-sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x+isqrtbf k^2+1tright)
$$
that appears as a general solution of the equation we started from.
My questions are the following:
- Is this approach sound to solve a linear PDE?
- What does it happen to the Dirac equation $(igammacdotpartial-1)psi=0$ using this technique?
pde distribution-theory
$endgroup$
Let us consider the wave equation written in the form
$$
partial_ttphi-Deltaphi+phi=0.
$$
By a Fourier transform, this takes the form
$$
(k_0^2-bf k^2-1)phi(k)=0.
$$
This has as a solution, in the sense of distributions,
$$
phi(k)=A(k)delta(k_0^2-bf k^2-1).
$$
It is easy to see that, by Fourier transforming back,
$$
phi(x)=intfracd^3k(2pi)^3left(fracA(bf k,sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x-isqrtbf k^2+1t-fracA(bf k,-sqrtbf k^2+1)2sqrtbf k^2+1e^ibf kcdotbf x+isqrtbf k^2+1tright)
$$
that appears as a general solution of the equation we started from.
My questions are the following:
- Is this approach sound to solve a linear PDE?
- What does it happen to the Dirac equation $(igammacdotpartial-1)psi=0$ using this technique?
pde distribution-theory
pde distribution-theory
edited Mar 31 at 14:11
Jon
asked Mar 27 at 15:35
JonJon
4,43211223
4,43211223
1
$begingroup$
As long as $phi$ can be assumed to not grow too fast (so that it is a Fourier transformable distribution), it is sound to use the Fourier transform to solve a linear PDE.
$endgroup$
– md2perpe
Mar 30 at 23:00
$begingroup$
Thanks a lot @md2perpe. Indeed, it appears that the textbook solution comes out naturally, provided I change the integration variable as $bf krightarrow -bf k$ in the second term.
$endgroup$
– Jon
Mar 30 at 23:09
add a comment |
1
$begingroup$
As long as $phi$ can be assumed to not grow too fast (so that it is a Fourier transformable distribution), it is sound to use the Fourier transform to solve a linear PDE.
$endgroup$
– md2perpe
Mar 30 at 23:00
$begingroup$
Thanks a lot @md2perpe. Indeed, it appears that the textbook solution comes out naturally, provided I change the integration variable as $bf krightarrow -bf k$ in the second term.
$endgroup$
– Jon
Mar 30 at 23:09
1
1
$begingroup$
As long as $phi$ can be assumed to not grow too fast (so that it is a Fourier transformable distribution), it is sound to use the Fourier transform to solve a linear PDE.
$endgroup$
– md2perpe
Mar 30 at 23:00
$begingroup$
As long as $phi$ can be assumed to not grow too fast (so that it is a Fourier transformable distribution), it is sound to use the Fourier transform to solve a linear PDE.
$endgroup$
– md2perpe
Mar 30 at 23:00
$begingroup$
Thanks a lot @md2perpe. Indeed, it appears that the textbook solution comes out naturally, provided I change the integration variable as $bf krightarrow -bf k$ in the second term.
$endgroup$
– Jon
Mar 30 at 23:09
$begingroup$
Thanks a lot @md2perpe. Indeed, it appears that the textbook solution comes out naturally, provided I change the integration variable as $bf krightarrow -bf k$ in the second term.
$endgroup$
– Jon
Mar 30 at 23:09
add a comment |
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$begingroup$
As long as $phi$ can be assumed to not grow too fast (so that it is a Fourier transformable distribution), it is sound to use the Fourier transform to solve a linear PDE.
$endgroup$
– md2perpe
Mar 30 at 23:00
$begingroup$
Thanks a lot @md2perpe. Indeed, it appears that the textbook solution comes out naturally, provided I change the integration variable as $bf krightarrow -bf k$ in the second term.
$endgroup$
– Jon
Mar 30 at 23:09