R - Galileo and Einstein
R - Galileo and Einstein
R - Galileo and Einstein
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Field from a Uniform Line of Charge<br />
• The strategy is to find the field<br />
z from a bit dz of the wire, then<br />
do an integral over the whole<br />
wire.<br />
kdq kdz kd R<br />
tan<br />
kd<br />
dE <br />
2 2 2 2<br />
r r R sec R<br />
• For an infinite wire, the net field<br />
must be directly away from the<br />
wire, so multiply by cos <strong>and</strong><br />
integrate over all z :<br />
E <br />
k<br />
R<br />
/2<br />
<br />
<br />
/2<br />
cosd<br />
<br />
2k<br />
R<br />
dE<br />
• q<br />
dE<br />
in<br />
r<br />
Rsec<br />
<br />
P<br />
<br />
R<br />
from charge<br />
d Rtan<br />
<br />
z-axis<br />
dz<br />
z<br />
Rtan<br />
O