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 65
Page 243
... materials whose surface of separation is a plane parallel to the plates . The first material ( with properties σ , and e1 ) is of thickness x , while the second material ( 02 , € 2 ) has thickness d− x . There is a steady current ...
... materials whose surface of separation is a plane parallel to the plates . The first material ( with properties σ , and e1 ) is of thickness x , while the second material ( 02 , € 2 ) has thickness d− x . There is a steady current ...
Page 357
... material would " spontaneously " have its charges separated which is incompatible with our picture of magnetization as arising from a reorientation of existing current whirls . The induction produced outside the material can be found ...
... material would " spontaneously " have its charges separated which is incompatible with our picture of magnetization as arising from a reorientation of existing current whirls . The induction produced outside the material can be found ...
Page 379
... materials since they are typified by the neighboring metals iron , cobalt , and nickel . There are , however , many alloys and nonmetals that also fall into this category . Although specific properties vary from material to material ...
... materials since they are typified by the neighboring metals iron , cobalt , and nickel . There are , however , many alloys and nonmetals that also fall into this category . Although specific properties vary from material to material ...
Other editions - View all
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