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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 16:57:21 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 16:57:21 +0100 |
| commit | 605ca77d47bc39f7a88af6e13535504c57fb7e95 (patch) | |
| tree | 4c1b2c24265b23009744184f725b5704a1c5dd26 /typst | |
| parent | c728891d1bf44ddd908c72ee756d7805d6245230 (diff) | |
| download | phd-fluid_mechanics_report-605ca77d47bc39f7a88af6e13535504c57fb7e95.tar.gz | |
progress
Diffstat (limited to 'typst')
| -rw-r--r-- | typst/main.typ | 4 |
1 files changed, 3 insertions, 1 deletions
diff --git a/typst/main.typ b/typst/main.typ index aa0d5d7..63d224c 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -248,7 +248,9 @@ tanh ( Z e psi / (4k_B T) ) ^2 e^(kappa h_"ij") ) n_"ij" $ ) -with $lambda$ being the characteristic wavelength of the interaction +with $lambda$ being the characteristic wavelength of the interaction, $k_B" the Boltzmann constant, $T$ the absolute temperature, "Z" is the valence +of the electrolyte, "e" is the electron charge, $A_"iLj"$ the Hamaker constant of the particle, i, the particle j and the liquid medium L, +$R_i$,$R_j$ are the particle radii with $h_"ij" << R_i,R_j$ #math.equation( block:true, |