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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 16:32:32 +0100 |
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| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 16:32:32 +0100 |
| commit | f7a0e48afbb5145ed6824c2147ff7dddc887c118 (patch) | |
| tree | c191e64a8322e7b396a30b8fb5c7306fa327e6ce /typst | |
| parent | 1db53b5f6e854415ba485cc52bb5817922382ac0 (diff) | |
| download | phd-fluid_mechanics_report-f7a0e48afbb5145ed6824c2147ff7dddc887c118.tar.gz | |
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Diffstat (limited to 'typst')
| -rw-r--r-- | typst/main.typ | 6 |
1 files changed, 6 insertions, 0 deletions
diff --git a/typst/main.typ b/typst/main.typ index 9a4add2..8e47953 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -248,6 +248,12 @@ tanh ( Z e psi / (4k_B T) ) ^2 e^(kappa h_"ij") ) n_"ij" $ ) +#math.equation( +block:true, +$ F_"ij"^"DLVO"_"pw" = ( - A_"iLj" R_"i" ) 1+28 h_"ij" / lambda ) / (6h^2_"ij" ( 1 + 14 h_"ij" / lambda )^2) +$ +) + == Discussion The particles forming arches are often inherently unstable. Slight fluctuations in flow rate, local velocity gradients or the particle shape |
