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 8
... Position Vector C2 = A2 + B2 ( 1-10 ) We now consider a simple specific example of a vector . As shown in Figure 1-11 , the location of a particular point P in space can be specified by the vector r drawn from ... VECTORS The Position Vector.
... Position Vector C2 = A2 + B2 ( 1-10 ) We now consider a simple specific example of a vector . As shown in Figure 1-11 , the location of a particular point P in space can be specified by the vector r drawn from ... VECTORS The Position Vector.
Page 16
... position vector . A vector whose value is thus given at every point in space is called a vector field . We now consider some specific ways in which it can change with position . Looking back at ( 1-37 ) , we see that Vu can be ...
... position vector . A vector whose value is thus given at every point in space is called a vector field . We now consider some specific ways in which it can change with position . Looking back at ( 1-37 ) , we see that Vu can be ...
Page 49
... positions throughout otherwise empty space . We designate each charge by q , and its position vector by r , where i = 1,2 , ... , N. This situation is illustrated in Figure 2-3 ; for clarity , the individual position vectors are not ...
... positions throughout otherwise empty space . We designate each charge by q , and its position vector by r , where i = 1,2 , ... , N. This situation is illustrated in Figure 2-3 ; for clarity , the individual position vectors are not ...
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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