Neutron Flux Profile in a Spherical Moderator

AI Thread Summary
The discussion focuses on solving the neutron diffusion equation for a spherical moderator with zero absorption cross section. The equation simplifies to D∇²φ = -S, leading to the general solution in spherical coordinates as φ = A/r + B, where A and B are constants determined by boundary conditions. The participants clarify the role of λ, confirming it equals 1/L if absorption were present. The Laplacian in spherical coordinates is also addressed, emphasizing the need for careful application in both homogeneous and inhomogeneous cases. The conversation highlights the mathematical approach to deriving the neutron flux profile in this specific scenario.
Israakaizzy
Messages
2
Reaction score
0
Hello People
I need help with the following assignment:
It states:
Consider an ideal moderator with zero absorption cross section, Ʃa = 0, and a diffusion coefficient, D, which has a spherical shape with an extrapolated radius, R. If neutron sources emitting S neutrons/cm3sec are distributed uniformly throughout the moderator, the steady neutron diffusion equation is given by,
D∇2\phi -Ʃa\phi=-S

a) Simplify the above neutron diffusion equation for this moderator in spherical coordinates and state the appropriate boundary conditions.

By solving the simplified diffusion equation, obtain the neutron flux profile, \phi(r).

I know I need to divided the neutron diffusion equation and cancel out the absorption cross section and end up with something like:
2\phi = -S/D
and the particular solution would be something like S/Ʃa
but what's the general solution to:
D∇2\phi =0
in spherical coordinates?
 
Engineering news on Phys.org
Israakaizzy,

I think it should be something like Asinh(λ.r)/r + Bcosh(λ.r)/r, applying the border conditions B=0.

hope it helps,

Hernán
 
ok
Just explain me what is \lambda equal to? Is it 1/L ?
 
Israakaizzy,

You are right, it should be 1/L if Ʃa were different than 0.

I did the maths for the homogeneous part:
∇^{2}\phi=0

saying that:

\phi=\frac{\widehat{\phi}}{r}

The Lapplacian inspherical coordintates turns:

∇^{2}\phi=\frac{∂^{2}\widehat{\phi}}{∂r^{2}} + \frac{2}{r}\frac{∂\widehat{\phi}}{∂r}

proposing an exponential solution:

λ^{2}e^{λr} + \frac{2}{r}λe^{λr} = 0

So:

λ= -\frac{2}{r}

and finally:

\phi= \frac{A}{r} + B

Don´t forget that for the inhomogeneous part you have to use the Lapplacian in sphericals.

Regards,

Hernán
 
Hello everyone, I am currently working on a burnup calculation for a fuel assembly with repeated geometric structures using MCNP6. I have defined two materials (Material 1 and Material 2) which are actually the same material but located in different positions. However, after running the calculation with the BURN card, I am encountering an issue where all burnup information(power fraction(Initial input is 1,but output file is 0), burnup, mass, etc.) for Material 2 is zero, while Material 1...
Hi everyone, I'm a complete beginner with MCNP and trying to learn how to perform burnup calculations. Right now, I'm feeling a bit lost and not sure where to start. I found the OECD-NEA Burnup Credit Calculational Criticality Benchmark (Phase I-B) and was wondering if anyone has worked through this specific benchmark using MCNP6? If so, would you be willing to share your MCNP input file for it? Seeing an actual working example would be incredibly helpful for my learning. I'd be really...
Back
Top