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-rw-r--r--typst/main.typ9
1 files changed, 8 insertions, 1 deletions
diff --git a/typst/main.typ b/typst/main.typ
index c3aec22..500f619 100644
--- a/typst/main.typ
+++ b/typst/main.typ
@@ -69,6 +69,13 @@ $ μ∇²u + f = ∇p,\
An additional restriction by the creeping flow equations is the selection of boundary criteria where it depends on
an infinite space with a set solid boundary interface.
+#math.equation(
+block: true,
+$ v = U "at" a = r,\
+v arrow 0 "as" a arrow infinity
+$
+)
+
== Solid-Fluid single sphere interaction with Stokes flow
With the previous assumptions a solid sphere of radius $r$ moving with a relative velocity $v$ in an unbounded creeping flow,
@@ -87,7 +94,7 @@ than the possibly more correct value by Proudman and Pearson@proudman_pearson_19
//$ F = F_S ( 1 + (3/8)"Re" + (9/40)("Re")^2 * (log "Re" + gamma + (5/3) log 2 - (323/360)) + (27/80)*"Re"^3 log "Re" ) $
//)
-Do the analitical derivation from sphere here
+Do the analitical derivation from sphere and stokes here TODO
== Lubrication forces between solid particles