From c418b2f332f924aaed5ca20e0553593a0db565ea Mon Sep 17 00:00:00 2001 From: Eugeniy Mikhailov 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} -- cgit v1.2.3