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authorClaudius "keldu" Holeksa <mail@keldu.de>2025-11-12 16:32:32 +0100
committerClaudius "keldu" Holeksa <mail@keldu.de>2025-11-12 16:32:32 +0100
commitf7a0e48afbb5145ed6824c2147ff7dddc887c118 (patch)
treec191e64a8322e7b396a30b8fb5c7306fa327e6ce /typst
parent1db53b5f6e854415ba485cc52bb5817922382ac0 (diff)
downloadphd-fluid_mechanics_report-f7a0e48afbb5145ed6824c2147ff7dddc887c118.tar.gz
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-rw-r--r--typst/main.typ6
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