Classical electrodynamicsThis edition refines and improves the first edition. It treats the present experimental limits on the mass of photon and the status of linear superposition, and introduces many other innovations. 
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Page 41
theorem, there results Green's first identity: f (4>V2«HV<f>V^)d3x = <f <i>^da (
1.34) Jv h on If we write down (1.34) again with <\> and \fi interchanged, and then
subtract it from (1.34), the V<f> • Vi/» terms cancel, and we obtain Green's second
...
theorem, there results Green's first identity: f (4>V2«HV<f>V^)d3x = <f <i>^da (
1.34) Jv h on If we write down (1.34) again with <\> and \fi interchanged, and then
subtract it from (1.34), the V<f> • Vi/» terms cancel, and we obtain Green's second
...
Page 394
The key result is the exact expansion (16.22) for the Green function appearing in
(9.3). For points outside the source (9.3) then becomes A(x)=— X h!1,(kr)Ylm(e, <
*>) fj(x')/.(kr')Yt(0', $>) dV (9.11) C l.m J If the source dimensions are small ...
The key result is the exact expansion (16.22) for the Green function appearing in
(9.3). For points outside the source (9.3) then becomes A(x)=— X h!1,(kr)Ylm(e, <
*>) fj(x')/.(kr')Yt(0', $>) dV (9.11) C l.m J If the source dimensions are small ...
Page 627
where the argument of the logarithm is <W>Omin Ze (to) ' The average frequency
(<u) appearing in Bc is a geometric mean defined by Z In (o>)=£/, In to, (13.38)
The result (13.36)(13.38) is that obtained by Bohr in his classic paper on energy
...
where the argument of the logarithm is <W>Omin Ze (to) ' The average frequency
(<u) appearing in Bc is a geometric mean defined by Z In (o>)=£/, In to, (13.38)
The result (13.36)(13.38) is that obtained by Bohr in his classic paper on energy
...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
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