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 208
... consider our next example . Example Capacitance of two parallel cylindrical conductors . Consider two infinitely long conducting cylinders whose axes are parallel . For simplicity , we assume that they have the same radius A ; their ...
... consider our next example . Example Capacitance of two parallel cylindrical conductors . Consider two infinitely long conducting cylinders whose axes are parallel . For simplicity , we assume that they have the same radius A ; their ...
Page 267
... consider is VXB . The general definition of the curl of a vector given by ( 1-73 ) suggests that we consider the line integral of B about some closed path . 15-1 Derivation of the Integral Form We will show that B.ds = B.ds = μolenc ...
... consider is VXB . The general definition of the curl of a vector given by ( 1-73 ) suggests that we consider the line integral of B about some closed path . 15-1 Derivation of the Integral Form We will show that B.ds = B.ds = μolenc ...
Page 287
... consider them again in more detail in Chapter 22 after we have completed the development of the general theory . The requirement ( 16-26 ) , and hence ( 16-27 ) , leads to the so - called Coulomb gauge . ] The vector potential is not as ...
... consider them again in more detail in Chapter 22 after we have completed the development of the general theory . The requirement ( 16-26 ) , and hence ( 16-27 ) , leads to the so - called Coulomb gauge . ] The vector potential is not as ...
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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