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 186
... satisfy ( 11-61 ) , and each combination will give a solution , so that there are many possibilities . At the same time , the constants of integration a , a , b1 , ... may themselves depend on the particular values of a , ẞ , y , so ...
... satisfy ( 11-61 ) , and each combination will give a solution , so that there are many possibilities . At the same time , the constants of integration a , a , b1 , ... may themselves depend on the particular values of a , ẞ , y , so ...
Page 254
... satisfy this same condition , so that , in addition to asking that A give the correct B , we require that A also satisfy ( 16-17 ) : ▽ · A = 0 ( 16-26 ) This will clearly lead to some restriction on our choice of x . We can see what ...
... satisfy this same condition , so that , in addition to asking that A give the correct B , we require that A also satisfy ( 16-17 ) : ▽ · A = 0 ( 16-26 ) This will clearly lead to some restriction on our choice of x . We can see what ...
Page 501
... satisfy the conditions that x = Vt x ' Vt ' = - = when x ' when x = 0 0 ( 29-19 ) satisfy ( 29-19 ) , that is , the linear equations We will try the simplest relations that will x ' = y ( x − Vt ) x = y ' ( x ' + Vt ' ) ( 29-20 ) where ...
... satisfy the conditions that x = Vt x ' Vt ' = - = when x ' when x = 0 0 ( 29-19 ) satisfy ( 29-19 ) , that is , the linear equations We will try the simplest relations that will x ' = y ( x − Vt ) x = y ' ( x ' + Vt ' ) ( 29-20 ) where ...
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 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