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 93
... Exercises 5-1 Can the vector E = ( yz - 2x ) x + xzŷ + xyî be a possible electrostatic field ? If so , find the potential from which E can be obtained . 5-2 Could the vector A of Exercise 1-15 be interpreted as a conservative electric ...
... Exercises 5-1 Can the vector E = ( yz - 2x ) x + xzŷ + xyî be a possible electrostatic field ? If so , find the potential from which E can be obtained . 5-2 Could the vector A of Exercise 1-15 be interpreted as a conservative electric ...
Page 123
... Exercise 5-9 and verify that you get the same result as for Exercise 7-4 and that your answer reduces to the correct result when n = 0 . What fraction of the total energy is outside the sphere ? 7-13 Consider the two conductors of ...
... Exercise 5-9 and verify that you get the same result as for Exercise 7-4 and that your answer reduces to the correct result when n = 0 . What fraction of the total energy is outside the sphere ? 7-13 Consider the two conductors of ...
Page 333
... Exercise 17-26 . 18-5 A self - inductance L , a resistance R , and a battery of emf & are all connected in series . Use energy considerations to show that the current i satisfies the differential equation L ( di / dt ) + Ri = & . Now ...
... Exercise 17-26 . 18-5 A self - inductance L , a resistance R , and a battery of emf & are all connected in series . Use energy considerations to show that the current i satisfies the differential equation L ( di / dt ) + Ri = & . Now ...
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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