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. |
From inside the book
Results 1-3 of 86
Page 44
... given by u = xy . Find Vu . Given the vector A = 3x + 2ŷ + 42 , find the component of A in the direction of Vu at the point on the curve for which u = 3 and for which x = 2 . 1-9 The equation giving a family of ellipsoids is u = ++ 를 ...
... given by u = xy . Find Vu . Given the vector A = 3x + 2ŷ + 42 , find the component of A in the direction of Vu at the point on the curve for which u = 3 and for which x = 2 . 1-9 The equation giving a family of ellipsoids is u = ++ 를 ...
Page 79
... given the values and locations of the source point charge distributions . For example , if everything is given in rectangular coordinates , we can use ( 1-14 ) to write ( 5-2 ) as N qi p ( r ) = 4 ( x , y , z ) = Σ i = 1 4π € o [ ( x ...
... given the values and locations of the source point charge distributions . For example , if everything is given in rectangular coordinates , we can use ( 1-14 ) to write ( 5-2 ) as N qi p ( r ) = 4 ( x , y , z ) = Σ i = 1 4π € o [ ( x ...
Page 22
... given temperature , we must invoke a result from statistical mechanics which says that the probability of finding a system in a given quantum state of energy Wm is given by e -BWm Pm ( Wm ) = Σe - BWm m ( B - 22 ) where ẞ = 1 / kT and k ...
... given temperature , we must invoke a result from statistical mechanics which says that the probability of finding a system in a given quantum state of energy Wm is given by e -BWm Pm ( Wm ) = Σe - BWm m ( B - 22 ) where ẞ = 1 / kT and k ...
Other editions - View all
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