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 280
... cross section of radius b . If the radius of the central axis is a , that is , this is the distance from the center 0 to the center of the cross section , find the ratio b / a necessary in order that the total deviation in B , across ...
... cross section of radius b . If the radius of the central axis is a , that is , this is the distance from the center 0 to the center of the cross section , find the ratio b / a necessary in order that the total deviation in B , across ...
Page 390
... Section 20-5 , except that region 2 between the conductors is filled with a nonhomogeneous material such that Km K ... cross section of radius a . When a field Ho is applied to one arm of the U - tube , the liquid level is found to rise ...
... Section 20-5 , except that region 2 between the conductors is filled with a nonhomogeneous material such that Km K ... cross section of radius a . When a field Ho is applied to one arm of the U - tube , the liquid level is found to rise ...
Page 492
... Section 11-4 . ) It will be left as exercises to show that the results of this section can be written in an even more compact and elegant form before it is necessary to specify the shape of the cross section of the guide . For our ...
... Section 11-4 . ) It will be left as exercises to show that the results of this section can be written in an even more compact and elegant form before it is necessary to specify the shape of the cross section of the guide . For our ...
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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