Analytical solution of the Photon Diffusion Equation

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SUMMARY

The discussion focuses on solving the photon diffusion equation analytically without employing the Monte Carlo technique. The primary equation integrated over time is given by the integral of the form int(c*exp(-r^2/(4*D*c*t)-a*c*t)/(4*Pi*D*c*t)^(3/2), t = 0 .. infinity). The user successfully derived a time-independent solution for flux and is attempting to find the transmission by converting to Cartesian coordinates and integrating over x while keeping y constant. The conversation highlights the need for further exploration of integral solutions, potentially involving Bessel functions, and emphasizes the importance of correctly identifying the direction of propagation in optics problems.

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  • Understanding of photon diffusion equations
  • Familiarity with integral calculus and integration techniques
  • Knowledge of Bessel functions and their applications
  • Basic principles of optics and coordinate transformations
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  • Study the derivation of photon transmission equations in optical media
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Students and researchers in physics, particularly those focused on optics and diffusion processes, as well as mathematicians interested in integral calculus applications in physical problems.

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Homework Statement


Hello, I am currently working on photon diffusion equation and trying to do it without using Monte Carlo technique.

Homework Equations


Starting equation integrated over t:
int(c*exp(-r^2/(4*D*c*t)-a*c*t)/(4*Pi*D*c*t)^(3/2), t = 0 .. infinity) (1)
Result:
sqrt(r^2/(D*c))*exp(-sqrt(a*c)*sqrt(r^2/(D*c)))*D*c^2/(4*r^2*Pi*sqrt(D^3*c^3)) (2)
Integral to find transmission:
int(exp(-sqrt(a*c*(1/(D*c)))*sqrt(x^2+y^2))/(4*Pi*D*sqrt(x^2+y^2)), x = -infinity .. infinity) (3)

The Attempt at a Solution


I have started with homogeneous solution calculating flux at a given point and a given time (1).
First, I integrated it over the time to get the time independent solution as it can be seen above. It gave me the flux at any given point independent of time (2).
The second thing I wanted to obtain from it is transmission, which I think should be obtainable by converting to Cartesian coordinates (r^2 = x^2+y^2) and integrating over x while keeping y constant (slab thickness) (3).
Here I am a bit stuck. I was trying to find table integrals or alternative solutions (I think there is a way to represent it using Bessel function). I would be very grateful if someone could help with this integral or point me towards the textbook with good derivation.
 
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:welcome:
## \\ ## Equation (3) looks incorrect to me. ## \\ ##Why don't you simply integrate equation (2) over ## dx dy=2 \pi r \, dr ## to get the final result?
 
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Charles Link said:
:welcome:
## \\ ## Equation (3) looks incorrect to me. ## \\ ##Why don't you simply integrate equation (2) over ## dx dy=2 \pi r \, dr ## to get the final result?
Thank you for reply
I am integrating only over dx because y is thickness of the slab and I want to find number of photons on output facet.
 
I'll need to study it further. Usually in these Optics problems, "z" is the direction of propagation, and that is evidenced by your equation for the intensity ## I(x,y) ## as the number of photons (or energy) per unit time per unit area is symmetric in "x" and "y". Check your equation again and see if the slab thickness isn't in the "z" direction.
 
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