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 23
... surface composed of those portions of S2 and S1 to the left of the plane plus the plane surfaces of intersection shown by AB and CD ; the outward normal to the new part of the bounding surface is shown as 2. Similar remarks apply to V1 ...
... surface composed of those portions of S2 and S1 to the left of the plane plus the plane surfaces of intersection shown by AB and CD ; the outward normal to the new part of the bounding surface is shown as 2. Similar remarks apply to V1 ...
Page 86
... surface will be given by ( 6-4 ) as E = Q / 47ea2 . Furthermore , since the field E at the surface is in the normal ... bounding surface of the conductor now has two parts : an outer surface S. , and an inner surface S. Again let us ...
... surface will be given by ( 6-4 ) as E = Q / 47ea2 . Furthermore , since the field E at the surface is in the normal ... bounding surface of the conductor now has two parts : an outer surface S. , and an inner surface S. Again let us ...
Page 442
... bounding surface , call this field ổ , and then find from ( 26-67 ) , we can use the results in ( 26-14 ) and ( 26-15 ) to give a possible TEM mode for the system . The two - dimensional field pattern obtained in this way will then ...
... bounding surface , call this field ổ , and then find from ( 26-67 ) , we can use the results in ( 26-14 ) and ( 26-15 ) to give a possible TEM mode for the system . The two - dimensional field pattern obtained in this way will then ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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Common terms and phrases
Ampère's law angle assume axes axis bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equipotential evaluate example expression field point free charge function given induction infinitely long integral integrand Laplace's equation line charge line integral located magnetic magnitude Maxwell's equations obtained origin P₁ perpendicular point charge polarized position vector potential difference quadrupole R₁ region result scalar potential Section shown in Figure sphere of radius spherical surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ μο дх