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 110
... parallel plate capacitor , that is , we assumed that E went abruptly to zero at the edges . Show that this is ... parallel faces of cross - sectional area > A is inserted between the plates of the capacitor of Figure 6-9 . The faces of ...
... parallel plate capacitor , that is , we assumed that E went abruptly to zero at the edges . Show that this is ... parallel faces of cross - sectional area > A is inserted between the plates of the capacitor of Figure 6-9 . The faces of ...
Page 193
... parallel plate capacitor of Figure 10-18 has square plates of edge L. When the dielectric is in a distance x , show that the capacitance as a function of x is given by C ( x ) = ( εoL / d ) [ L + ( k ̧− 1 ) x ] . 10-33 The parallel ...
... parallel plate capacitor of Figure 10-18 has square plates of edge L. When the dielectric is in a distance x , show that the capacitance as a function of x is given by C ( x ) = ( εoL / d ) [ L + ( k ̧− 1 ) x ] . 10-33 The parallel ...
Page 243
... parallel faces . Two metal cylinders , each of radius A , have their axes parallel and a distance D apart . These cylinders pass through the dielectric with their axes normal to the plane surfaces . If a potential difference Ap is ...
... parallel faces . Two metal cylinders , each of radius A , have their axes parallel and a distance D apart . These cylinders pass through the dielectric with their axes normal to the plane surfaces . If a potential difference Ap is ...
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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