## 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

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Page 95

If p is the perpendicular distance from the axis of the cylinder, show that the

potential outside the cylinder can be written ♢(p)-T^-ln(-) (P>«) (6-42) ... 6-6 A

capacitor C, is charged resulting in a

If p is the perpendicular distance from the axis of the cylinder, show that the

potential outside the cylinder can be written ♢(p)-T^-ln(-) (P>«) (6-42) ... 6-6 A

capacitor C, is charged resulting in a

**potential difference**A<f/> between its plates.Page 105

IP* (7-39) [In this process, the

change in order that Q = CA<j> remain constant. Since this leads to dQ = 0 = ( dC

)(^<t>) + Cd(A<t>), we find rf(A</>) dC A<//> C (7-40) which says that the

fractional ...

IP* (7-39) [In this process, the

**potential difference**between the plates mustchange in order that Q = CA<j> remain constant. Since this leads to dQ = 0 = ( dC

)(^<t>) + Cd(A<t>), we find rf(A</>) dC A<//> C (7-40) which says that the

fractional ...

Page 109

What additional mass must be placed in the other arm of the balance so that the

suspended plate will retain its original position? 7-16 A battery is used to charge

a parallel plate capacitor to a

What additional mass must be placed in the other arm of the balance so that the

suspended plate will retain its original position? 7-16 A battery is used to charge

a parallel plate capacitor to a

**potential difference**A<//> and is then disconnected.### What people are saying - Write a review

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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