- #1
Berko
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On page 60 of his 3rd edition of Classical Electrodynamics, he discusses the method of images applied to a grounded conducting sphere with a single charge q outside it.
Near the end of the problem, he calculates the force on a small patch of area da as (sigma^2/2epsilon_nought)da.
Now, it seems to me that the force should be the E field at that point times the charge of the patch...i.e.
dF = (sigma/epsilon_nought)*(sigma da).
Where does the factor of 2 come from?
Thank you.
Near the end of the problem, he calculates the force on a small patch of area da as (sigma^2/2epsilon_nought)da.
Now, it seems to me that the force should be the E field at that point times the charge of the patch...i.e.
dF = (sigma/epsilon_nought)*(sigma da).
Where does the factor of 2 come from?
Thank you.