## Classical Electrodynamics |

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Page 10

da (1.23) Another problem of interest is the potential due to a

distribution on a surface S. A

letting the surface S have a surface-charge density of x) on it, and another

surface S", ...

da (1.23) Another problem of interest is the potential due to a

**dipole**-layerdistribution on a surface S. A

**dipole**layer can be imagined as being formed byletting the surface S have a surface-charge density of x) on it, and another

surface S", ...

Page 132

The basic entity in magnetic studies was what we now know as a magnetic

. In the presence of magnetic materials the

direction. That direction is by definition the direction of the magnetic-flux density,

...

The basic entity in magnetic studies was what we now know as a magnetic

**dipole**. In the presence of magnetic materials the

**dipole**tends to align itself in a certaindirection. That direction is by definition the direction of the magnetic-flux density,

...

Page 274

Considering only the magnetization term, we have the vector potential, ikor A(x) =

ik(n x m) o( - #) (9.33) r ikr where m is the magnetic

se x J) doc (9.34) c The fields can be determined by noting that the vector ...

Considering only the magnetization term, we have the vector potential, ikor A(x) =

ik(n x m) o( - #) (9.33) r ikr where m is the magnetic

**dipole**moment, in E so d°r = ;se x J) doc (9.34) c The fields can be determined by noting that the vector ...

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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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