From c418b2f332f924aaed5ca20e0553593a0db565ea Mon Sep 17 00:00:00 2001
From: Eugeniy Mikhailov <evgmik@gmail.com>
Date: Tue, 9 Dec 2014 13:13:47 -0500
Subject: Ashley's corrections

---
 faraday_rotation.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

(limited to 'faraday_rotation.tex')

diff --git a/faraday_rotation.tex b/faraday_rotation.tex
index da1d7a0..23cab82 100644
--- a/faraday_rotation.tex
+++ b/faraday_rotation.tex
@@ -39,7 +39,7 @@ this lab, the field at the center is $B=\unit[11.1]{mT/A}$, and our
 material, a special sort of glass, is $\unit[10]{cm}$ long. For a current
 of \unit[0.1]{A}, we expect a rotation of a few$\times10^{-4}$ radians. This is a pretty small angle and it will require a special technique to detect.  
 
-We are going to take polarized laser light and direct it through the glass
+We are going to take the polarized laser light and direct it through the glass
 rod, which is inserted into the center of the solenoid. The beam will then
 pass through a second polarizer with the transmission axis at an angle $\theta$ with respect to the initial polarization of the laser. The intensity of the transmitted light will then depend on the sum of the angle $\theta$ and the additional rotation $\phi$ caused by the magnetic field:
 \begin{eqnarray}
-- 
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