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 96
... capacitor is made from two infinitely long conductors with coaxial ... parallel . ( b ) Capacitors in series . tion . Show qualitatively that this ... plate capacitor , that is , we assumed that E went abruptly to zero at the edges . Actu ...
... capacitor is made from two infinitely long conductors with coaxial ... parallel . ( b ) Capacitors in series . tion . Show qualitatively that this ... plate capacitor , that is , we assumed that E went abruptly to zero at the edges . Actu ...
Page 104
... parallel plate capacitor of capacitance C. By means of the switch S , the terminals T and T ' can be connected by conducting wires to a battery B that will provide a difference of potential Ap between the plates , thus charging the ...
... parallel plate capacitor of capacitance C. By means of the switch S , the terminals T and T ' can be connected by conducting wires to a battery B that will provide a difference of potential Ap between the plates , thus charging the ...
Page 109
... parallel plate capacitor has plates of area A. The lower plate is rigidly fastened to a table top . The upper plate is suspended from a spring of spring constant k whose upper end is rigidly fastened . The plates are originally ...
... parallel plate capacitor has plates of area A. The lower plate is rigidly fastened to a table top . The upper plate is suspended from a spring of spring constant k whose upper end is rigidly fastened . The plates are originally ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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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