## 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 26

Thus, when we perform the final integration over x in (1-70), that is, adding up the

contributions of all of the strips, the contribution from each strip will be Axdsx from

its share of the bounding

Thus, when we perform the final integration over x in (1-70), that is, adding up the

contributions of all of the strips, the contribution from each strip will be Axdsx from

its share of the bounding

**curve**; the final result will be the line integral of Ax dsx ...Page 339

If Rc is the resistance of this circuit, we find from (12-2) and (17-3) that the

magnitude of AQc is which agrees with the result of Exercise 17-6 and gives us

AB = RcAQc/S thus enabling us to evaluate A B. In this way, the

the ...

If Rc is the resistance of this circuit, we find from (12-2) and (17-3) that the

magnitude of AQc is which agrees with the result of Exercise 17-6 and gives us

AB = RcAQc/S thus enabling us to evaluate A B. In this way, the

**curve**describingthe ...

Page 340

20-21, and then start to decrease H. We find, as indicated by the directions of the

arrowheads, that the

rapidly as it originally increased. A general behavior like this is known as ...

20-21, and then start to decrease H. We find, as indicated by the directions of the

arrowheads, that the

**curve**does not retrace its path, and B does not decrease asrapidly as it originally increased. A general behavior like this is known as ...

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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