Classical ElectrodynamicsProblems after each chapter |
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Page 13
Equations ( 1.13 ) and ( 1.16 ) can be combined into one partial differential equation for the single function ( x ) : V20 = –4πρ ( 1.28 ) This equation is called Poisson's equation . In regions of space where there is no charge density ...
Equations ( 1.13 ) and ( 1.16 ) can be combined into one partial differential equation for the single function ( x ) : V20 = –4πρ ( 1.28 ) This equation is called Poisson's equation . In regions of space where there is no charge density ...
Page 337
+ ( Ane * no ) n m an independent equation , but may be derived by combining the last two equations in ( 10.91 ) . Since the force equation in ( 10.91 ) is independent of magnetic field , we suspect that there exist solutions of a ...
+ ( Ane * no ) n m an independent equation , but may be derived by combining the last two equations in ( 10.91 ) . Since the force equation in ( 10.91 ) is independent of magnetic field , we suspect that there exist solutions of a ...
Page 582
The equation can be criticized on the grounds that it is second order in time , rather than first , and therefore runs counter to the well - known requirements for a dynamical equation of motion . This difficulty manifests itself ...
The equation can be criticized on the grounds that it is second order in time , rather than first , and therefore runs counter to the well - known requirements for a dynamical equation of motion . This difficulty manifests itself ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
TimeVarying Fields Maxwells Equations Con | 169 |
Copyright | |
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