## 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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Results 1-3 of 84

Page 6

The components can be positive or negative; for example, if Ax were negative,

then the vector A x of Figure 1-7 would have a

decreasing values of x. From Figure 1-7, it is seen that the magnitude of a vector

can be ...

The components can be positive or negative; for example, if Ax were negative,

then the vector A x of Figure 1-7 would have a

**direction**in the sense ofdecreasing values of x. From Figure 1-7, it is seen that the magnitude of a vector

can be ...

Page 9

We see from Figure 1-13 that we can get a simple interpretation of the scalar

product: (Bcos^)A = component of B along the

of A = (A cos ty)B = component of A along B times the magnitude of B. It is clear

from ...

We see from Figure 1-13 that we can get a simple interpretation of the scalar

product: (Bcos^)A = component of B along the

**direction**of A times the magnitudeof A = (A cos ty)B = component of A along B times the magnitude of B. It is clear

from ...

Page 17

We also see that a

vector h, which is normal to the surface. Thus, we can associate a vector da with

this element of area and write it as da = da ft (1-52) by following the general form

of ...

We also see that a

**direction**can be associated with this area, that is, the unitvector h, which is normal to the surface. Thus, we can associate a vector da with

this element of area and write it as da = da ft (1-52) by following the general form

of ...

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angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conducting conductor const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux free charge function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz transformation magnetic magnitude Maxwell's equations normal component obtained origin parallel plate capacitor particle perpendicular point charge polarized position vector potential difference quadrupole quantities rectangular coordinates region result satisfy scalar potential shown in Figure situation solenoid solution sphere of radius spherical surface charge surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero