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
Results 1-3 of 88
Page 239
... angle has the same value that it had initially , so that A = 0 and ( 15-4 ) becomes $ B. ds = 0 C ( 15-5 ) 2. The ... angle between da ' and  is YA 90 ° - 8 where 8 is very small and positive . Then the solid angle subtended by da ' at ...
... angle has the same value that it had initially , so that A = 0 and ( 15-4 ) becomes $ B. ds = 0 C ( 15-5 ) 2. The ... angle between da ' and  is YA 90 ° - 8 where 8 is very small and positive . Then the solid angle subtended by da ' at ...
Page 408
... angle of reflection equals the angle of incidence . Thus , this ancient and well - known law of optics is seen to be a direct consequence of Maxwell's equations . For the transmitted wave , we find from ( 25-10 ) , ( 25-11 ) , ( 25-12 ) ...
... angle of reflection equals the angle of incidence . Thus , this ancient and well - known law of optics is seen to be a direct consequence of Maxwell's equations . For the transmitted wave , we find from ( 25-10 ) , ( 25-11 ) , ( 25-12 ) ...
Page 410
... angle of incidence is less than the critical angle . Figure 25-7 . The three propagation vectors when the angle of incidence equals the critical angle . Thus in this case it is not fruitful to continue with 0 ,; we can , however , go ...
... angle of incidence is less than the critical angle . Figure 25-7 . The three propagation vectors when the angle of incidence equals the critical angle . Thus in this case it is not fruitful to continue with 0 ,; we can , however , go ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
12 other sections not shown
Other editions - View all
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