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 xi
... Induction 255 14-1 Definition of the Magnetic Induction 255 14-2 14-3 Straight Current of Finite Length Axial Induction of a Circular Current 258 260 14-4 14-5 Infinite Plane Uniform Current Sheet Moving Point Charges 262 263 15 The ...
... Induction 255 14-1 Definition of the Magnetic Induction 255 14-2 14-3 Straight Current of Finite Length Axial Induction of a Circular Current 258 260 14-4 14-5 Infinite Plane Uniform Current Sheet Moving Point Charges 262 263 15 The ...
Page 255
... induction " ; the term " magnetic field " is generally used for a different vector field that we define later when we include the effects of matter . 14-1 ... INDUCTION 255 The Magnetic Induction 14-1 Definition of the Magnetic Induction.
... induction " ; the term " magnetic field " is generally used for a different vector field that we define later when we include the effects of matter . 14-1 ... INDUCTION 255 The Magnetic Induction 14-1 Definition of the Magnetic Induction.
Page 265
... induction at any point on the z axis when a current I ' circulates around the square . Show that your result gives the value 2√2 μÏ ' / πa for the induction at the center . 14-5 An ideal solenoid of length L and N turns is wound with a ...
... induction at any point on the z axis when a current I ' circulates around the square . Show that your result gives the value 2√2 μÏ ' / πa for the induction at the center . 14-5 An ideal solenoid of length L and N turns is wound with a ...
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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