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 44
... calculation . 1-11 Do the example of Section 1-11 by integrating over y rather than x and thus show that the same ... calculate the surface integral of VXA over the enclosed area and show that ( 1-67 ) is satisfied . 1-15 Given the ...
... calculation . 1-11 Do the example of Section 1-11 by integrating over y rather than x and thus show that the same ... calculate the surface integral of VXA over the enclosed area and show that ( 1-67 ) is satisfied . 1-15 Given the ...
Page 62
... calculate E first and then insert q as a last step by means of ( 3-1 ) . We can thus regard the calculation of E as merely providing us with a sort of contingency statement distributed throughout space in the sense that E ( r ) ...
... calculate E first and then insert q as a last step by means of ( 3-1 ) . We can thus regard the calculation of E as merely providing us with a sort of contingency statement distributed throughout space in the sense that E ( r ) ...
Page 497
... calculation to be & 2 = E。sin ( MπX a sin ппу b ( 26-61 ) which can now be used to calculate the rest of the field amplitudes by means of ( 26-25 ) through ( 26-28 ) . We note that m = n = 0 makes & ,, and then all of the other field ...
... calculation to be & 2 = E。sin ( MπX a sin ппу b ( 26-61 ) which can now be used to calculate the rest of the field amplitudes by means of ( 26-25 ) through ( 26-28 ) . We note that m = n = 0 makes & ,, and then all of the other field ...
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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