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 76
... line charge , a displacement parallel to the line leads one to a point where the charge distribution will appear essentially unaltered . 1 If we now go further and let both L2 and L1 get infinitely large in ( 5-32 ) , we again get an ...
... line charge , a displacement parallel to the line leads one to a point where the charge distribution will appear essentially unaltered . 1 If we now go further and let both L2 and L1 get infinitely large in ( 5-32 ) , we again get an ...
Page 183
... charge in the dielectric . Physically , this is just the force of attraction between q and the bound surface charges ... line charge and a semiinfinite plane grounded conductor . We consider an infinitely long line charge of constant ...
... charge in the dielectric . Physically , this is just the force of attraction between q and the bound surface charges ... line charge and a semiinfinite plane grounded conductor . We consider an infinitely long line charge of constant ...
Page 200
... charge per unit length paral- lel to the line charge , and the force per unit length on the line charge . 11-12 Show that the attractive force on a length L of one of the cylinders of Figure 11-10 is given by F περ L ( ΔΦ ) 2 [ cosh ̄1 ...
... charge per unit length paral- lel to the line charge , and the force per unit length on the line charge . 11-12 Show that the attractive force on a length L of one of the cylinders of Figure 11-10 is given by F περ L ( ΔΦ ) 2 [ cosh ̄1 ...
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 curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equation 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 surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ дх