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 76
... cylinder of radius Po whose axis coincides with the line charge . The surface of the cylinder carries a charge of constant surface density o . Find E everywhere . What particular value of o will make E = 0 for all points outside the ...
... cylinder of radius Po whose axis coincides with the line charge . The surface of the cylinder carries a charge of constant surface density o . Find E everywhere . What particular value of o will make E = 0 for all points outside the ...
Page 208
... cylinder . There will be a surface charge on the cylinder given by ( 6-4 ) , but , as we can easily see , the total charge per unit length on the cylinder will still be A ( assuming a surface in the right half of Figure 5-8 ) . Consider ...
... cylinder . There will be a surface charge on the cylinder given by ( 6-4 ) , but , as we can easily see , the total charge per unit length on the cylinder will still be A ( assuming a surface in the right half of Figure 5-8 ) . Consider ...
Page 358
... cylinder . ( a ) Side view . ( b ) End view . by B ; the relevant one is that the normal components of B are continuous as given by ( 16-4 ) . But this is precisely the same boundary condition that we used to obtain the cavity ...
... cylinder . ( a ) Side view . ( b ) End view . by B ; the relevant one is that the normal components of B are continuous as given by ( 16-4 ) . But this is precisely the same boundary condition that we used to obtain the cavity ...
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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