## Classical Electrodynamics |

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Page 63

If the point x is on the z

hand side becomes: |-- 1 --— |x – x' T (r” + r.” – 2rr' cos y)” |r — r" (3.43)

Expanding (3.43), we find 1 1 < (#) - - - 3.44 |x — x"| r X. (3.44) For points off the

If the point x is on the z

**axis**, the right-hand side reduces to (3.38), while the left-hand side becomes: |-- 1 --— |x – x' T (r” + r.” – 2rr' cos y)” |r — r" (3.43)

Expanding (3.43), we find 1 1 < (#) - - - 3.44 |x — x"| r X. (3.44) For points off the

**axis**it is ...Page 166

c C W on A cylindrical conductor of radius a has a hole of radius b bored parallel

to, and centered a distance d from, the cylinder

density is uniform throughout the remaining metal of the cylinder and is parallel to

the ...

c C W on A cylindrical conductor of radius a has a hole of radius b bored parallel

to, and centered a distance d from, the cylinder

**axis**(d + b : a). The currentdensity is uniform throughout the remaining metal of the cylinder and is parallel to

the ...

Page

The speed of the particle is constant so that at any position along the z

” = to (12.126) where to” - vu" + to is the square of the speed at z = 0. If we

assume that the flux linked is a constant of the motion, then (12.125) allows us to

write ...

The speed of the particle is constant so that at any position along the z

**axis**to + c,” = to (12.126) where to” - vu" + to is the square of the speed at z = 0. If we

assume that the flux linked is a constant of the motion, then (12.125) allows us to

write ...

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### Contents

Introduction to Electrostatics | 1 |

Nº 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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