A dynamical theory of the electromagnetic field (1865)
Maxwell, James Clerk, 1831-1879, Burndy Library, donor. DSI, Royal Society (Great Britain) · [London : The Royal Society] · leaf 23
cuit S is removed, the value of x will be E w= j sm(pt-x), where Aa=Ka+Ly, and _Lp tan a= R The effect of the presence of the circuit S in the neighbourhood is to alter the value of A and a, to that which they would be if R become MS ~&+P\ Ss+j92N2 and L became MN L— jy S2+^N2 Hence the effect of… … potentials at the four points be A, C, D, E. Then the conditions of steady currents may be found from the equations Po?=A-D Q(x-z)=D-C, R^=A-E S(y+z)=E-C, (21) Gz=D-E B(#+^)=-A+C+F. Solving these equations for z, we find 4p+Q+E+H+B(f+h)(q+I)+g(p+4)(s+I)+pSs(P+Q+E+S)}=F(^-5r)- (22) mdccclxv. 3 t
Electromagnetic fields
Internet Archive · Smithsonian Libraries · Public domain (published before 1931). Free to use for anything.
