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 225
... length parallel to the line charge , and the force per unit length on the line charge . 11-12 Show that the attractive force on a length L of one of the cylinders of Figure 11-10 is given by 11-13 Fe = περα ( Αφ ) 2 [ cosh = ' ( D / 2A ) ...
... length parallel to the line charge , and the force per unit length on the line charge . 11-12 Show that the attractive force on a length L of one of the cylinders of Figure 11-10 is given by 11-13 Fe = περα ( Αφ ) 2 [ cosh = ' ( D / 2A ) ...
Page 275
... length / and each the same distance D from the sheet ; these are connected by two vertical sides of length 2D . On the horizontal sides , B is parallel to ds , so that B.ds = B ( D ) ds and B ( D ) is constant . On the vertical sides ...
... length / and each the same distance D from the sheet ; these are connected by two vertical sides of length 2D . On the horizontal sides , B is parallel to ds , so that B.ds = B ( D ) ds and B ( D ) is constant . On the vertical sides ...
Page 545
... length of interest . Although such a detailed specification appears to be trivial when the measuring rod and the length are relatively at rest , it is essential when they are moving with respect to each other . Let L = x2 - x1 be the ...
... length of interest . Although such a detailed specification appears to be trivial when the measuring rod and the length are relatively at rest , it is essential when they are moving with respect to each other . Let L = x2 - x1 be the ...
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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