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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Results 1-3 of 81
Page 144
... write this in terms of the external electric field E by noting that ( ado / aj ) oEoj because of ( 5-3 ) so that = - Veog = - 1 6 a Eoi Ək j = x , y , z k = x , y , z ΣΣΩ ( 8-69 ) which , when written out , becomes Еох aEox + VeoQ ...
... write this in terms of the external electric field E by noting that ( ado / aj ) oEoj because of ( 5-3 ) so that = - Veog = - 1 6 a Eoi Ək j = x , y , z k = x , y , z ΣΣΩ ( 8-69 ) which , when written out , becomes Еох aEox + VeoQ ...
Page 323
... write K1 = nlê . Similarly , we found in ( 16-46 ) and after ( 16-50 ) that the vector potential on the surface ( where K , ‡ 0 ) is A = 1⁄2μonlap where we write the radius as ā . If we insert these into ( 18-13 ) in order to obtain the ...
... write K1 = nlê . Similarly , we found in ( 16-46 ) and after ( 16-50 ) that the vector potential on the surface ( where K , ‡ 0 ) is A = 1⁄2μonlap where we write the radius as ā . If we insert these into ( 18-13 ) in order to obtain the ...
Page 4
... write the rate of change of the vector v1 in the form dv dt = wcXVL Equating ( A - 15 ) with ( A - 11 ) , we find the vector angular velocity to be ( A - 15 ) ως -- ( 2 ) B то ( A - 16 ) and whose sign agrees with Figure A - 1 since we ...
... write the rate of change of the vector v1 in the form dv dt = wcXVL Equating ( A - 15 ) with ( A - 11 ) , we find the vector angular velocity to be ( A - 15 ) ως -- ( 2 ) B то ( A - 16 ) and whose sign agrees with Figure A - 1 since we ...
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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