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Page 63
If the point x is on the z axis , the right - hand side reduces to ( 3.38 ) , while the left - hand side becomes : 1 = 1 ( p2 + p ' ? – 2rr ' cos y ) " 1 ir – r ' ( 3.43 ) | x – X ' ! Expanding ( 3.43 ) , we find 1 | x – X ' !
If the point x is on the z axis , the right - hand side reduces to ( 3.38 ) , while the left - hand side becomes : 1 = 1 ( p2 + p ' ? – 2rr ' cos y ) " 1 ir – r ' ( 3.43 ) | x – X ' ! Expanding ( 3.43 ) , we find 1 | x – X ' !
Page 166
( c ) Show that at the end of a long solenoid the magnetic induction near the axis has components 20NI πΝΙ B2B. – с a 5.3 A cylindrical conductor of radius a has a hole of radius b bored parallel to , and centered a distance d from ...
( c ) Show that at the end of a long solenoid the magnetic induction near the axis has components 20NI πΝΙ B2B. – с a 5.3 A cylindrical conductor of radius a has a hole of radius b bored parallel to , and centered a distance d from ...
Page 422
2 orbit of small radius with a transverse velocity Vzo and a component of velocity v ... parallel to B at z = 0 , where the axial field strength is B. The speed of the particle is constant so that at any position along the z axis 0,2 +0 ...
2 orbit of small radius with a transverse velocity Vzo and a component of velocity v ... parallel to B at z = 0 , where the axial field strength is B. The speed of the particle is constant so that at any position along the z axis 0,2 +0 ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
TimeVarying Fields Maxwells Equations Con | 169 |
Copyright | |
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