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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

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