Difference between revisions of "Hauptseminar Porous Media SS 2021/Random walk models diffusion in porous media"
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{{Seminartopic | {{Seminartopic | ||
|number=5 | |number=5 | ||
− | |topic=Random | + | |topic=Random walks in porous media: Diffusion at the pore and at the pore-network scale |
|speaker= TBD | |speaker= TBD | ||
|date=TBA | |date=TBA | ||
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== Contents == | == Contents == | ||
− | + | Diffusion in confined geometries - in contrast to transport - refers to the case where no driving force (chemical potential gradient, e.g. density/pressure/electric field) is applied, or where the transport due to the driving force can be neglected due to the vanishing gradients (which is typically the case in smallest pores). | |
+ | |||
== Literature == | == Literature == | ||
TBA | TBA |
Revision as of 10:12, 11 February 2021
- Date
- TBA"TBA" contains an extrinsic dash or other characters that are invalid for a date interpretation.
- Time
- TBA
- Topic
- Random walks in porous media: Diffusion at the pore and at the pore-network scale
- Speaker
- TBD
- Tutor
- Alexander Schlaich
Contents
Diffusion in confined geometries - in contrast to transport - refers to the case where no driving force (chemical potential gradient, e.g. density/pressure/electric field) is applied, or where the transport due to the driving force can be neglected due to the vanishing gradients (which is typically the case in smallest pores).
Literature
TBA