How can I prove the following integral identity?












0












$begingroup$


The following equation is a solution of a convection-diffusion problem. I want to prove that the resultant solution is simplified to the initial condition when $Delta t$ approaches zero. Consequently, I want to prove the following integral identity.



$$lim_{Delta t rightarrow 0}frac{1}{2 Delta t} int_{0}^infty x F(x) e^ {-frac{x^2 + r^2}{4 Delta t}} I_0(frac{x r}{2 Delta t}) {d}x = F(r)$$



where $F(r)$ is the initial solution of the problem whose solution is displayed by the LHS of the previous equation. $I_0$ is modified Bessel function of the first kind of zeroth order.










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$endgroup$












  • $begingroup$
    Thanks for your comment.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:51






  • 1




    $begingroup$
    What is $I_0$? Is it a Bessel function?
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:53






  • 1




    $begingroup$
    It is the modified Bessel function of the first kind of zero order.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:55










  • $begingroup$
    Thanks for editing the question to address the definition of $I_0$! I guess that the proof will have something to do with the Dirac delta 'function' and its 'sifting' property.
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:58










  • $begingroup$
    I am not sure I understand you. The equation doesn't include Dirac delta function and this solution has not been obtained using it.
    $endgroup$
    – Galal
    Dec 23 '18 at 19:01
















0












$begingroup$


The following equation is a solution of a convection-diffusion problem. I want to prove that the resultant solution is simplified to the initial condition when $Delta t$ approaches zero. Consequently, I want to prove the following integral identity.



$$lim_{Delta t rightarrow 0}frac{1}{2 Delta t} int_{0}^infty x F(x) e^ {-frac{x^2 + r^2}{4 Delta t}} I_0(frac{x r}{2 Delta t}) {d}x = F(r)$$



where $F(r)$ is the initial solution of the problem whose solution is displayed by the LHS of the previous equation. $I_0$ is modified Bessel function of the first kind of zeroth order.










share|cite|improve this question











$endgroup$












  • $begingroup$
    Thanks for your comment.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:51






  • 1




    $begingroup$
    What is $I_0$? Is it a Bessel function?
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:53






  • 1




    $begingroup$
    It is the modified Bessel function of the first kind of zero order.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:55










  • $begingroup$
    Thanks for editing the question to address the definition of $I_0$! I guess that the proof will have something to do with the Dirac delta 'function' and its 'sifting' property.
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:58










  • $begingroup$
    I am not sure I understand you. The equation doesn't include Dirac delta function and this solution has not been obtained using it.
    $endgroup$
    – Galal
    Dec 23 '18 at 19:01














0












0








0





$begingroup$


The following equation is a solution of a convection-diffusion problem. I want to prove that the resultant solution is simplified to the initial condition when $Delta t$ approaches zero. Consequently, I want to prove the following integral identity.



$$lim_{Delta t rightarrow 0}frac{1}{2 Delta t} int_{0}^infty x F(x) e^ {-frac{x^2 + r^2}{4 Delta t}} I_0(frac{x r}{2 Delta t}) {d}x = F(r)$$



where $F(r)$ is the initial solution of the problem whose solution is displayed by the LHS of the previous equation. $I_0$ is modified Bessel function of the first kind of zeroth order.










share|cite|improve this question











$endgroup$




The following equation is a solution of a convection-diffusion problem. I want to prove that the resultant solution is simplified to the initial condition when $Delta t$ approaches zero. Consequently, I want to prove the following integral identity.



$$lim_{Delta t rightarrow 0}frac{1}{2 Delta t} int_{0}^infty x F(x) e^ {-frac{x^2 + r^2}{4 Delta t}} I_0(frac{x r}{2 Delta t}) {d}x = F(r)$$



where $F(r)$ is the initial solution of the problem whose solution is displayed by the LHS of the previous equation. $I_0$ is modified Bessel function of the first kind of zeroth order.







integration improper-integrals indefinite-integrals






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Dec 23 '18 at 18:55







Galal

















asked Dec 23 '18 at 18:44









GalalGalal

344




344












  • $begingroup$
    Thanks for your comment.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:51






  • 1




    $begingroup$
    What is $I_0$? Is it a Bessel function?
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:53






  • 1




    $begingroup$
    It is the modified Bessel function of the first kind of zero order.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:55










  • $begingroup$
    Thanks for editing the question to address the definition of $I_0$! I guess that the proof will have something to do with the Dirac delta 'function' and its 'sifting' property.
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:58










  • $begingroup$
    I am not sure I understand you. The equation doesn't include Dirac delta function and this solution has not been obtained using it.
    $endgroup$
    – Galal
    Dec 23 '18 at 19:01


















  • $begingroup$
    Thanks for your comment.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:51






  • 1




    $begingroup$
    What is $I_0$? Is it a Bessel function?
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:53






  • 1




    $begingroup$
    It is the modified Bessel function of the first kind of zero order.
    $endgroup$
    – Galal
    Dec 23 '18 at 18:55










  • $begingroup$
    Thanks for editing the question to address the definition of $I_0$! I guess that the proof will have something to do with the Dirac delta 'function' and its 'sifting' property.
    $endgroup$
    – rafa11111
    Dec 23 '18 at 18:58










  • $begingroup$
    I am not sure I understand you. The equation doesn't include Dirac delta function and this solution has not been obtained using it.
    $endgroup$
    – Galal
    Dec 23 '18 at 19:01
















$begingroup$
Thanks for your comment.
$endgroup$
– Galal
Dec 23 '18 at 18:51




$begingroup$
Thanks for your comment.
$endgroup$
– Galal
Dec 23 '18 at 18:51




1




1




$begingroup$
What is $I_0$? Is it a Bessel function?
$endgroup$
– rafa11111
Dec 23 '18 at 18:53




$begingroup$
What is $I_0$? Is it a Bessel function?
$endgroup$
– rafa11111
Dec 23 '18 at 18:53




1




1




$begingroup$
It is the modified Bessel function of the first kind of zero order.
$endgroup$
– Galal
Dec 23 '18 at 18:55




$begingroup$
It is the modified Bessel function of the first kind of zero order.
$endgroup$
– Galal
Dec 23 '18 at 18:55












$begingroup$
Thanks for editing the question to address the definition of $I_0$! I guess that the proof will have something to do with the Dirac delta 'function' and its 'sifting' property.
$endgroup$
– rafa11111
Dec 23 '18 at 18:58




$begingroup$
Thanks for editing the question to address the definition of $I_0$! I guess that the proof will have something to do with the Dirac delta 'function' and its 'sifting' property.
$endgroup$
– rafa11111
Dec 23 '18 at 18:58












$begingroup$
I am not sure I understand you. The equation doesn't include Dirac delta function and this solution has not been obtained using it.
$endgroup$
– Galal
Dec 23 '18 at 19:01




$begingroup$
I am not sure I understand you. The equation doesn't include Dirac delta function and this solution has not been obtained using it.
$endgroup$
– Galal
Dec 23 '18 at 19:01










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