## Classical Electrodynamics |

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Page 218

7.9 Reflection and refraction with polarization

incidence. E and H are continuous. In terms of fields (7.49)–(7.51) these

boundary conditions at z = 0 are: [e(Eo + Eo") – e'Eo'] n = 0 [k × Eo + k" x Eo" – k'

x Eo'] n ...

7.9 Reflection and refraction with polarization

**perpendicular**to k” the plane ofincidence. E and H are continuous. In terms of fields (7.49)–(7.51) these

boundary conditions at z = 0 are: [e(Eo + Eo") – e'Eo'] n = 0 [k × Eo + k" x Eo" – k'

x Eo'] n ...

Page

parallel to and

comparable parallel and

component is negligible (of order 1/y”) compared to that from the

component.

parallel to and

**perpendicular**to the velocity. But we have just seen that forcomparable parallel and

**perpendicular**forces the radiation from the parallelcomponent is negligible (of order 1/y”) compared to that from the

**perpendicular**component.

Page

For simplicity we consider a small angle deflection so that AB is approximately

relationships. Without loss of generality n, the observation direction, is chosen in

the r-z ...

For simplicity we consider a small angle deflection so that AB is approximately

**perpendicular**to the incident direction. Figure 15.2 shows the vectorialrelationships. Without loss of generality n, the observation direction, is chosen in

the r-z ...

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### Contents

Introduction to Electrostatics | 1 |

Nº 3 | 3 |

Greens theorem | 14 |

Copyright | |

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