Edge Plasma Physics: Key Considerations for PIC Codes & Simulations

AI Thread Summary
Key considerations for simulating the edge plasma region in devices like tokamaks include understanding the electron sheath dynamics at the walls and diagnostic devices, as well as the presence of a non-Maxwellian distribution of particles. High gradients in temperature and electric potential are critical factors, and when developing a PIC code, it's essential to account for the electron-Larmor radius relative to grid dimensions. Additionally, the increased density of neutrals near the plasma edge can lead to spallation reactions upon contact with the wall, introducing contamination into the plasma. Effective heating methods, such as neutral beam injection and microwave heating, also play a significant role in edge plasma behavior. Overall, these elements are vital for accurate modeling and simulation of edge plasma processes.
LuisVela
Messages
32
Reaction score
0
Hello everybody.
Im starting a project on the basic processed undergoing in the edge plasma region. ( I mean, near the walls of a plasma confining device, like a tokamak or so.)

I was wondering if you could name some ''things'' I should be aware of in order to make a small PIC code or computer simulation.

I came up with these ones:

1.) Electron sheath on the walls, and over diagnostic devices (Probes and so on..).

2.) Non-Maxwellian distribution near the edge.

3.) High gradients on temperature & electric potential.

4.) In case of a PIC code, be awarer that the electron-larmor radius is bigger than the dimensions of the cell composing the grid.

...any suggestions?
 
Engineering news on Phys.org
There would be a greater density of neutrals near the edge of the plasma. If the plasma (neutral) make it to the wall, then there are spallation reactions with the wall, and that is the source of contamination (of higher Z atoms) in the plasma. If the current density is greater in the sheath, then the sheath temperature is higher and the heat must be conducted to the interior.

The heating might also be accomplished by neutral beam injection, microwave heating and compression.
 
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