Unformatted text preview: 57. We note that the contributions to the ﬁeld from the pair of −2q charges exactly cancel, and we are left
with the (opposing) contributions from the 4q (at r = 2d) and −q (at r = d) charges. Therefore, using
k = 1/4πε0
4q
q
Enet  = k
−k 2 =0 .
2
(2d)
d
The net ﬁeld at P vanishes completely. ...
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This note was uploaded on 11/12/2011 for the course PHYS 2001 taught by Professor Sprunger during the Fall '08 term at LSU.
 Fall '08
 SPRUNGER
 Physics, Charge

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