Introduction to ElectrodynamicsFor junior/senior-level electricity and magnetism courses. This book is known for its clear, concise and accessible coverage of standard topics in a logical and pedagogically sound order. The Third Edition features a clear, accessible treatment of the fundamentals of electromagnetic theory, providing a sound platform for the exploration of related applications (ac circuits, antennas, transmission lines, plasmas, optics, etc.). Its lean and focused approach employs numerous examples and problems. |
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Page 74
... plane is independent of how far away you are . What about the 1 / r2 in Coulomb's law ? Well , the point is that as you move farther and farther away from the plane , more and more charge comes into your " field of view " ( a cone shape ...
... plane is independent of how far away you are . What about the 1 / r2 in Coulomb's law ? Well , the point is that as you move farther and farther away from the plane , more and more charge comes into your " field of view " ( a cone shape ...
Page 126
... plane is a grounded conductor . ) Problem 3.7 ( a ) Using the law of cosines , show that Eq . 3.17 can be written as ... plane . ( Let's say the wire runs parallel to the x - axis and directly above it , and the conducting plane is the ...
... plane is a grounded conductor . ) Problem 3.7 ( a ) Using the law of cosines , show that Eq . 3.17 can be written as ... plane . ( Let's say the wire runs parallel to the x - axis and directly above it , and the conducting plane is the ...
Page 376
... plane waves , because the fields are uniform over every plane perpendicular to the direction of propagation ( Fig . 9.9 ) . We are interested , then , in fields of the form Ĕ ( z , t ) = Ēoei ( kz - wt ) , B ( z , t ) Boei ( kz - wt ) 4 ...
... plane waves , because the fields are uniform over every plane perpendicular to the direction of propagation ( Fig . 9.9 ) . We are interested , then , in fields of the form Ĕ ( z , t ) = Ēoei ( kz - wt ) , B ( z , t ) Boei ( kz - wt ) 4 ...
Contents
Vector Analysis | 1 |
Spherical Polar Coordinates | 38 |
Electrostatics | 58 |
Copyright | |
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Ampère's law angular answer atom axis Biot-Savart law bound charge boundary conditions calculate capacitor charge density charge distribution charge q components conductor configuration constant coordinates Coulomb's law curl cylinder derivative direction distance divergence theorem electric and magnetic electric field electrodynamics electromagnetic electron electrostatics energy Example field inside Figure Find the electric Find the potential flux formula free charge frequency function Gauss's law gradient infinite Laplace's equation line integral Lorentz force law magnetic dipole magnetic field magnetic force magnetostatics Maxwell's equations momentum motion moving particle perpendicular Phys plane point charge polarization Poynting vector Prob Problem radiation region relativistic scalar Sect shown in Fig solenoid Solution speed spherical steady current Suppose surface charge total charge unit vector potential velocity volume wave wire zero Απ Απερ μο ду