## 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 5

The product of a scalar s and a vector, which we

merely the sum of s vectors A, or is a vector with a magnitude equal to |s| times

the magnitude of A, and is in the same direction as A if 5 is positive, and in the ...

The product of a scalar s and a vector, which we

**write**as either s\ or As, is thenmerely the sum of s vectors A, or is a vector with a magnitude equal to |s| times

the magnitude of A, and is in the same direction as A if 5 is positive, and in the ...

Page 286

inductance L with a current /, we can

middle term of (18-8) involves both currents and arises from the fact that a

changing flux in one circuit produces an induced emf in the other; this term can

be taken to ...

inductance L with a current /, we can

**write**its energy as Um = \LP (18-9) Themiddle term of (18-8) involves both currents and arises from the fact that a

changing flux in one circuit produces an induced emf in the other; this term can

be taken to ...

Page 455

We note that we can

coefficients, the real and imaginary parts of any solution will separately be

solutions of the differential equation. Hence, as in Section 24-2, it will be

convenient to ...

We note that we can

**write**S= Re[<f0e"*"] and, since (27-11) is linear and has realcoefficients, the real and imaginary parts of any solution will separately be

solutions of the differential equation. Hence, as in Section 24-2, it will be

convenient to ...

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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