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 157
... Sect . 3.4.4 . The answer is that the differentiation leading to Eq . 3.103 is perfectly valid except at r = O , but we should have known ( from our experience in Sect . 1.5.1 ) that the point r = 0 is problematic . See C. P. Frahm , Am ...
... Sect . 3.4.4 . The answer is that the differentiation leading to Eq . 3.103 is perfectly valid except at r = O , but we should have known ( from our experience in Sect . 1.5.1 ) that the point r = 0 is problematic . See C. P. Frahm , Am ...
Page 268
... Sect . 6.2.1 are applied to points inside magnetized material , as you can prove for yourself in the following problem . Problem 6.11 In Sect , 6.2.1 , we began with the potential of a perfect dipole ( Eq . 6.10 ) , whereas in fact we ...
... Sect . 6.2.1 are applied to points inside magnetized material , as you can prove for yourself in the following problem . Problem 6.11 In Sect , 6.2.1 , we began with the potential of a perfect dipole ( Eq . 6.10 ) , whereas in fact we ...
Page 363
... Sect . 8.1.2 , starting with Eq . 8.6 , but using Jf in place of J. Show that the Poynting vector becomes S = Ex H , and the rate of change of the energy density in the fields is диет at ƏD = E. + H Ət For linear media , show that . ав ...
... Sect . 8.1.2 , starting with Eq . 8.6 , but using Jf in place of J. Show that the Poynting vector becomes S = Ex H , and the rate of change of the energy density in the fields is диет at ƏD = E. + H Ət For linear media , show that . ав ...
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