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authorEugeniy Mikhailov <evgmik@gmail.com>2013-09-03 18:17:11 -0400
committerEugeniy Mikhailov <evgmik@gmail.com>2013-09-03 18:17:11 -0400
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typos fixed in emratio chapter
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diff --git a/manual_source/chapters/emratio.tex b/manual_source/chapters/emratio.tex
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--- a/manual_source/chapters/emratio.tex
+++ b/manual_source/chapters/emratio.tex
@@ -44,8 +44,8 @@
\section*{Theory}
- The apparatus shown in Figure \ref{emfig1}.
-consists of a glass tube that
+ The apparatus shown in Figure \ref{emfig1}
+ consists of a glass tube that
houses a small electron gun. This gun has a cathode filament
from which electrons can be thermionically released (boiled
off), and a nearby anode which can be set to a potential which
@@ -142,7 +142,7 @@ electron beam.
The Helmholtz coils of the $e/m$ apparatus have a radius and separation of
$a=15$~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
+$7.80\cdot10^{-4}$~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 automatically when the heater of the electron
gun is powered. By lining the electron beam up with its image in the mirrored