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 301
... loop in an alternating induction . As an example of a stationary system involving a real circuit , let us consider the rectangular loop of sides a and b shown in Figure 17-4 . We choose the z axis to lie in the plane of the loop and ...
... loop in an alternating induction . As an example of a stationary system involving a real circuit , let us consider the rectangular loop of sides a and b shown in Figure 17-4 . We choose the z axis to lie in the plane of the loop and ...
Page 309
... loop . Let us consider again the loop with the dimensions and orientation shown in Figure 17-4 . However , we now assume that B = Box is constant in time , while the loop is rotating as a rigid body about the z axis with constant ...
... loop . Let us consider again the loop with the dimensions and orientation shown in Figure 17-4 . However , we now assume that B = Box is constant in time , while the loop is rotating as a rigid body about the z axis with constant ...
Page 317
... loop of radius a lies in the xz plane with its center on the positive x axis at a distance b from the origin . Find the flux through the loop . If the loop is now moved with constant speed v parallel to the x axis and away from I , find ...
... loop of radius a lies in the xz plane with its center on the positive x axis at a distance b from the origin . Find the flux through the loop . If the loop is now moved with constant speed v parallel to the x axis and away from I , find ...
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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