Electromagnetic FieldsThis revised edition provides patient guidance in its clear and organized presentation of problems. It is rich in variety, large in number and provides very careful treatment of relativity. One outstanding feature is the inclusion of simple, standard examples demonstrated in different methods that will allow students to enhance and understand their calculating abilities. There are over 145 worked examples; virtually all of the standard problems are included. |
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Page 44
... rectangular parallelepiped of sides a , b , c with origin at one corner and edges along the positive directions of the rectangular axes as shown in Figure 1-41 . Evaluate SV.Adr over the volume of this same parallelepiped and compare ...
... rectangular parallelepiped of sides a , b , c with origin at one corner and edges along the positive directions of the rectangular axes as shown in Figure 1-41 . Evaluate SV.Adr over the volume of this same parallelepiped and compare ...
Page 492
... Rectangular Guide This guide has a rectangular cross section of sides a and b , which we take to be located in the xy plane as shown in Figure 26-2 . We see from ( 26-29 ) and ( 26-30 ) that for either type of mode we have to solve an ...
... Rectangular Guide This guide has a rectangular cross section of sides a and b , which we take to be located in the xy plane as shown in Figure 26-2 . We see from ( 26-29 ) and ( 26-30 ) that for either type of mode we have to solve an ...
Page 505
... rectangular wave guide with vacuum inside has a = 8 centimeters and b = 6 centime- ters . If a wave of frequency v = 4 × 109 hertz is to be propagated down the guide , what modes are possible ? 26-5 Consider a wave guide of square cross ...
... rectangular wave guide with vacuum inside has a = 8 centimeters and b = 6 centime- ters . If a wave of frequency v = 4 × 109 hertz is to be propagated down the guide , what modes are possible ? 26-5 Consider a wave guide of square cross ...
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Common terms and phrases
Ampère's law angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point flux force free charge free currents frequency function given induction infinitely long integral integrand k₂ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quadrupole quantities radiation radius rectangular region result satisfy scalar scalar potential shown in Figure solenoid sphere spherical tangential components unit vacuum vector potential velocity volume write written xy plane zero Απερ дх Мо