From: W. Trevor King <wking@drexel.edu>
Date: Tue, 13 Sep 2011 15:15:07 +0000 (-0400)
Subject: Fix omega -> \omega in manual's timescale discussion.
X-Git-Url: http://git.tremily.us/?p=sawsim.git;a=commitdiff_plain;h=1994aa886096a81d2ef73aa40c97c57cded6cc35;hp=e2d5d015420d83c8fa04a864783035f7fb351e6e

Fix omega -> \omega in manual's timescale discussion.
---

diff --git a/src/sawsim.nw b/src/sawsim.nw
index b83faa5..5f89121 100644
--- a/src/sawsim.nw
+++ b/src/sawsim.nw
@@ -685,7 +685,7 @@ along the chain.  The quality of this assumption depends on your
 particular chain.  For example, a damped spring thermalizes on a
 timescale of order $\tau = 1/\gamma$ where the damping ratio $\gamma
 \equiv \omega_0(-\zeta \pm \sqrt{\zeta^2-1}$, the natural angular
-frequency $omega_0 \equiv \sqrt{k/m}$, $\zeta \equiv b/2\sqrt{km}$,
+frequency $\omega_0 \equiv \sqrt{k/m}$, $\zeta \equiv b/2\sqrt{km}$,
 and $b$ sets the drag $F_b = -bv$.  For our cantilevers $\tau$ is
 on the order of milliseconds, which is longer than a timestep.
 However, the approximation is still reasonable, because there is