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 87
Page 100
... conductor C. within a cavity inside a conductor , the electric field will be always zero within the cavity , and the cavity will be an equipotential volume . In fact , the potential within the cavity will be the same as that of the ...
... conductor C. within a cavity inside a conductor , the electric field will be always zero within the cavity , and the cavity will be an equipotential volume . In fact , the potential within the cavity will be the same as that of the ...
Page 103
... conductor j brings conductor i to a potential o , then the same charge Q placed on i would bring j to the same potential p . Sometimes , if the problem is simple enough to be readily solved , the be more easily found from ( 6-11 ) than ...
... conductor j brings conductor i to a potential o , then the same charge Q placed on i would bring j to the same potential p . Sometimes , if the problem is simple enough to be readily solved , the be more easily found from ( 6-11 ) than ...
Page 487
... conductor and 8 is the skin depth . The subscript 7 indicates that E , is parallel to the surface of the conductor since it is transverse to the direction of propagation ân of Figure 25-3 . Thus , at the surface , E , will be a ...
... conductor and 8 is the skin depth . The subscript 7 indicates that E , is parallel to the surface of the conductor since it is transverse to the direction of propagation ân of Figure 25-3 . Thus , at the surface , E , will be a ...
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