0c27b98e2e
n_e as boundary condition
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Now n_e is given as the density at the boundary and n_i at the boundary
is calculated once Z is known.
This aims to eliminate the iterative process.
2025-04-10 08:49:01 +02:00
052a4dc05e
Corrections to tag v2.5
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Small set of corrections to the tag v2.5.
Includes changes to python scripts to plot data.
Includes new 'fast' setup conditions that allow to output cases in an
hour or so with still a good CFL condition and grid resolution.
2025-04-08 16:32:59 +02:00
1c7bdde8f0
Preparation to push to git
2024-12-12 10:05:35 +01:00
db7077efc0
Smaller grid size and BC to ensure reaching a quasi-steady state after 80 ns in the domain
2024-11-28 10:57:27 +01:00
c0c10c9cb1
Changes in plotting scripts
2024-11-18 12:52:31 +01:00
e82d4378c6
Update python scripts.
2024-10-09 16:31:25 +02:00
c39e9ab3fc
Trying to implement floating potential
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These things are never easy.
2024-09-27 17:56:03 +02:00
8eab3b5610
I'm stupid and I deleted the previous repository...
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So, code is working, this case reproduce a Diko's peak with Poisson
equation by changing the boundary conditions over time.
2024-09-26 17:58:45 +02:00
