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authorEugeniy Mikhailov <evgmik@gmail.com>2013-09-03 15:42:19 -0400
committerEugeniy Mikhailov <evgmik@gmail.com>2013-09-03 15:42:19 -0400
commit0e6787d82bee3219cffe1abaf1fe93de8f575a49 (patch)
tree7f5dc12e889cfb572ba6d66f72397bf554292276 /manual_source/chapters
parent29fd5ddc2329880da76387d29f4ea8031110361b (diff)
downloadmanual_for_Experimental_Atomic_Physics-0e6787d82bee3219cffe1abaf1fe93de8f575a49.tar.gz
manual_for_Experimental_Atomic_Physics-0e6787d82bee3219cffe1abaf1fe93de8f575a49.zip
a bit easier sentense in the em ratio lab
Diffstat (limited to 'manual_source/chapters')
-rw-r--r--manual_source/chapters/emratio.tex2
1 files changed, 1 insertions, 1 deletions
diff --git a/manual_source/chapters/emratio.tex b/manual_source/chapters/emratio.tex
index cddd36a..e262b7e 100644
--- a/manual_source/chapters/emratio.tex
+++ b/manual_source/chapters/emratio.tex
@@ -144,7 +144,7 @@ $a=15$~cm. Each coil has $N=130$~turns. The magnetic field ($B$) produced by
the coils is proportional to the current through the coils ($I_{hc}$) times
$7.80\cdot10^{-4}$~tesla/ampere [$B (tesla) = (7.80 \cdot 10^{-4}) I_{hc}$]. A
mirrored scale is attached to the back of the rear Helmholtz coil. It is
-illuminated by lights that light automatically when the heater of the electron
+illuminated automatically when the heater of the electron
gun is powered. By lining the electron beam up with its image in the mirrored
scale, you can measure the radius of the beam path without parallax error. The
cloth hood can be placed over the top of the $e/m$ apparatus so the experiment