Explicit wave-package solution of the Klein Gordon equationTrouble deriving DE for fourier transform from DE of functionIntegration by parts with few regularityIn the numerical solution of the Wave Equation, using finite differences, where do I obtain the spatial values from?Solving a wave equation using Fourier transformWhy can I change the integration unit in Fourier transform>Solving linear dispersive wave equation with Fourier transformSolving a simple Schrodinger equation with Fast Fourier TransformsSpherical Harmonic integration1D scalar wave equation PML finite difference implementationVelocity Auto-correlation on Spinning Disk
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Explicit wave-package solution of the Klein Gordon equation
Trouble deriving DE for fourier transform from DE of functionIntegration by parts with few regularityIn the numerical solution of the Wave Equation, using finite differences, where do I obtain the spatial values from?Solving a wave equation using Fourier transformWhy can I change the integration unit in Fourier transform>Solving linear dispersive wave equation with Fourier transformSolving a simple Schrodinger equation with Fast Fourier TransformsSpherical Harmonic integration1D scalar wave equation PML finite difference implementationVelocity Auto-correlation on Spinning Disk
$begingroup$
I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
beginequation
Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
endequation
an obvious wave-package solution is given by
beginequation
psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
endequation
with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
beginequation
psi(x,0) = e^-fracx^24 +i x cdot k,
endequation
and the time derivative at $t=0$ becomes
beginequation
partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
endequation
And one can recognize this as the Fourier transform of
beginequation
mathcalFleft( omega(k) e^-k^2 right).
endequation
So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)
integration numerical-methods fourier-analysis
$endgroup$
add a comment |
$begingroup$
I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
beginequation
Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
endequation
an obvious wave-package solution is given by
beginequation
psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
endequation
with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
beginequation
psi(x,0) = e^-fracx^24 +i x cdot k,
endequation
and the time derivative at $t=0$ becomes
beginequation
partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
endequation
And one can recognize this as the Fourier transform of
beginequation
mathcalFleft( omega(k) e^-k^2 right).
endequation
So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)
integration numerical-methods fourier-analysis
$endgroup$
add a comment |
$begingroup$
I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
beginequation
Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
endequation
an obvious wave-package solution is given by
beginequation
psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
endequation
with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
beginequation
psi(x,0) = e^-fracx^24 +i x cdot k,
endequation
and the time derivative at $t=0$ becomes
beginequation
partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
endequation
And one can recognize this as the Fourier transform of
beginequation
mathcalFleft( omega(k) e^-k^2 right).
endequation
So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)
integration numerical-methods fourier-analysis
$endgroup$
I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
beginequation
Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
endequation
an obvious wave-package solution is given by
beginequation
psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
endequation
with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
beginequation
psi(x,0) = e^-fracx^24 +i x cdot k,
endequation
and the time derivative at $t=0$ becomes
beginequation
partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
endequation
And one can recognize this as the Fourier transform of
beginequation
mathcalFleft( omega(k) e^-k^2 right).
endequation
So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)
integration numerical-methods fourier-analysis
integration numerical-methods fourier-analysis
edited Mar 22 at 0:03
J. W. Tanner
4,4891320
4,4891320
asked Mar 21 at 23:50
HamilcarHamilcar
404211
404211
add a comment |
add a comment |
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