J. C. Maxwell’s, ‘Dynamical theory of the electromagnetic field’

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                                Hence if we know the magnetic intensities I and I' due to unit 
current in each circuit we may obtain M by integrating 
<s>[mu]<s>1/4[pi] [capital sigma] [mu]II' cos[theta] dV 
over all space where [theta] is the angle between the directions of I & I' 

                            
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Manuscript details

Author
James Clerk Maxwell
Reference
PT/72/7
Series
PT
Date
1864
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Cite as

J. C. Maxwell’s, ‘Dynamical theory of the electromagnetic field’, 1864. From The Royal Society, PT/72/7

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