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Those would be convenient to generate MGXS for 2D-RZ calculations mostly. Those could remain common for cylindrical reactors with highly heterogeneous geometries (TMSR, PB-FHR for example).
Also for …
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inspired by the recent storage and delivery box I was wondering if we should have a custom Plasma box
Plasma is a bit unique as it has a ```generation_term``` of the burn faction * the amount of pl…
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This came from an audit #548.
Reviewers for step 2 need to be added to the following:
- [x] Advanced Projects (sub-community)
- [x] Other Projects
- [x] Stellarators
- [x] System Studies
…
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The tokamak Pegasus-III is missing properties such as major and minor radii, plasma current, etc.
These properties can be easily added by modifying the Pegasus-III entry in tokamaks.json and then r…
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Start implementing new configurations from other tokamaks, e.g.: AUG, COMPASS, EAST, JET, JT60-SA, KSTAR, MAST, TCV and other toroidal or linear devices
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In GitLab by @jlion on Dec 8, 2020, 11:57
_Merges stellarator_develop -> develop_
This merge updates the stellarator branch of PROCESS in several points:
### Read in stellarator effective paramete…
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Unsure why, but after committing, I'm unable to push the changes I've made (some issues with 2-Factor authentication). Figured, to notify at least.
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In GitLab by @pc6783 on Oct 11, 2021, 15:31
The PF placement is limited to 3 location-categories. This works well for designing new tokamaks, but for modeling existing designs it can be restrictive. …
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We currently only have one voxel type implemented: an axisymmetric voxel. This is fine for tokamaks, but Cherab's strength lies in being able to treat emitters and observers as fully 3D objects. We sh…
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In GitLab by @skahn on Jan 31, 2020, 11:27
## Description
If there is no hole in the TF midle, the $`\sigma_{rr}(R=0) = 0`$ should be normally modified to $`u_{r}(R=0) = 0`$.
## Discussion
Howeve…