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 107
... plate capacitor . This system consists of two conducting plates , each of area A , which are parallel to each other and separated by a distance d that is small compared to their linear dimensions . The plates need not be square , but ...
... plate capacitor . This system consists of two conducting plates , each of area A , which are parallel to each other and separated by a distance d that is small compared to their linear dimensions . The plates need not be square , but ...
Page 193
... plates . The value of κe is κe for a < r < ro and K2 for ro < r < b . Find the capacitance of this system by finding the total energy of the fields between the plates . 10-30 The coaxial cylindrical capacitor of Figure 6-12 has a ...
... plates . The value of κe is κe for a < r < ro and K2 for ro < r < b . Find the capacitance of this system by finding the total energy of the fields between the plates . 10-30 The coaxial cylindrical capacitor of Figure 6-12 has a ...
Page 393
... plate capacitor with circular plates of radius a . For simplicity , we assume a vacuum between the plates , and , as usual , we also assume that the separation between the plates is so small compared with the radius that the electric ...
... plate capacitor with circular plates of radius a . For simplicity , we assume a vacuum between the plates , and , as usual , we also assume that the separation between the plates is so small compared with the radius that the electric ...
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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