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 24
... volume V enclosed by a surface S. Gauss ' divergence theorem states that $ A · da = √√√ · Adr · ( 1-59 ) The integrals are taken over the total surface S and throughout the volume V whose volume element is dr . Again , for ...
... volume V enclosed by a surface S. Gauss ' divergence theorem states that $ A · da = √√√ · Adr · ( 1-59 ) The integrals are taken over the total surface S and throughout the volume V whose volume element is dr . Again , for ...
Page 26
... volume V surrounded by two surfaces S , and S2 ; two representative outward normals to the volume are shown as în and î ' . We now imagine a plane intersecting the volume and dividing it into two volumes V2 and V1 ; the trace of this ...
... volume V surrounded by two surfaces S , and S2 ; two representative outward normals to the volume are shown as în and î ' . We now imagine a plane intersecting the volume and dividing it into two volumes V2 and V1 ; the trace of this ...
Page 51
... volume , we can introduce a volume charge density p , which is defined as the charge per unit volume and hence will be measured in coulombs / ( meter ) 3 . ( We will write this charge density as Pch in the infrequent cases in which it ...
... volume , we can introduce a volume charge density p , which is defined as the charge per unit volume and hence will be measured in coulombs / ( meter ) 3 . ( We will write this charge density as Pch in the infrequent cases in which it ...
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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