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 3
... magnitude ( its length ) and a direction ( from P , to P2 ) . If we now further displace our point along E from P2 to still another point P3 , we see from Figure 1-2 that the new net effect is the same as if the point had been given the ...
... magnitude ( its length ) and a direction ( from P , to P2 ) . If we now further displace our point along E from P2 to still another point P3 , we see from Figure 1-2 that the new net effect is the same as if the point had been given the ...
Page 9
... magnitude of A = ( A cos ) B = component of A along B times the magnitude of B. It is clear from ( 1-15 ) that the order of terms does not change the scalar product , that is , A.B = B.A ( 1-16 ) · and that if two vectors are ...
... magnitude of A = ( A cos ) B = component of A along B times the magnitude of B. It is clear from ( 1-15 ) that the order of terms does not change the scalar product , that is , A.B = B.A ( 1-16 ) · and that if two vectors are ...
Page 3
... magnitude v . Consequently , the magnitude of dv / dt will be constant and equal to ( q / m 。) v B. This situation is illustrated in Figure A - 1 , which is drawn for positive q and B out of the paper . We recall that an acceleration ...
... magnitude v . Consequently , the magnitude of dv / dt will be constant and equal to ( q / m 。) v B. This situation is illustrated in Figure A - 1 , which is drawn for positive q and B out of the paper . We recall that an acceleration ...
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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