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| author | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-12-09 13:13:47 -0500 |
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| committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-12-09 13:13:47 -0500 |
| commit | c418b2f332f924aaed5ca20e0553593a0db565ea (patch) | |
| tree | 0472b0e5d7812f7f0a9f48235adb9334bb5ac522 /faraday_rotation.tex | |
| parent | a9ba4532dfbbad47f80e0176ad0cf5e6e94231d5 (diff) | |
| download | manual_for_Experimental_Atomic_Physics-c418b2f332f924aaed5ca20e0553593a0db565ea.tar.gz manual_for_Experimental_Atomic_Physics-c418b2f332f924aaed5ca20e0553593a0db565ea.zip | |
Ashley's corrections
Diffstat (limited to 'faraday_rotation.tex')
| -rw-r--r-- | faraday_rotation.tex | 2 |
1 files changed, 1 insertions, 1 deletions
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} |