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. |
From inside the book
Results 1-3 of 21
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 ...
Other editions - View all
Common terms and phrases
Ampère's law angle assume axis bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge function given incident induction infinitely long integral integrand k₁ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations medium molecule n₂ normal components obtained origin parallel plate capacitor particle perpendicular plane wave point charge polarized position vector potential difference quantities radiation rectangular refraction region result satisfy scalar scalar potential shown in Figure solenoid spherical surface charge density tangential components total charge vacuum vector potential velocity volume write written xy plane Z₂ zero Απερ дх