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 6
... axes respectively , as shown in Figure 1-6 . In other words , each is in the direction of increasing value of the corresponding rectangu- lar coordinate . We also see that any one of this set is perpendicular to each of the other two ...
... axes respectively , as shown in Figure 1-6 . In other words , each is in the direction of increasing value of the corresponding rectangu- lar coordinate . We also see that any one of this set is perpendicular to each of the other two ...
Page 149
... axes . ( For example , p is not parallel to any of the axes . ) Express its potential at a point r in rectangular coordinates , and find the rectangular components of E. Show that E can be written in the form E ( r ) = 1 Απερτο [ 3 ...
... axes . ( For example , p is not parallel to any of the axes . ) Express its potential at a point r in rectangular coordinates , and find the rectangular components of E. Show that E can be written in the form E ( r ) = 1 Απερτο [ 3 ...
Page 208
... axes are parallel . For simplicity , we assume that they have the same radius A ; their axes are separated by a distance D as shown in Figure 11-10 . If we identify these cylinders with the appropriate equipotentials of Figure 5-8 ...
... axes are parallel . For simplicity , we assume that they have the same radius A ; their axes are separated by a distance D as shown in Figure 11-10 . If we identify these cylinders with the appropriate equipotentials of Figure 5-8 ...
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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