## Classical Electrodynamics |

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Page 247

If a > b , the lowest cutoff frequency , that of the dominant TE

= 1 , n = 0 : TTC 010 =( 8 . 45 ) * « μεα ... 0

of both TE and TM

If a > b , the lowest cutoff frequency , that of the dominant TE

**mode**, occurs for m= 1 , n = 0 : TTC 010 =( 8 . 45 ) * « μεα ... 0

**mode**has the lowest cutoff frequencyof both TE and TM

**modes**, * and so is the one used in most practical situations .Page 263

The frequency is assumed to be high enough that two

circles at the intersections of the two curves , exist . The vertical asymptotes are

given by the roots of J . ( x ) = 0 . If the maximum value of ya is smaller than the

first ...

The frequency is assumed to be high enough that two

**modes**, marked by thecircles at the intersections of the two curves , exist . The vertical asymptotes are

given by the roots of J . ( x ) = 0 . If the maximum value of ya is smaller than the

first ...

Page 576

( 6 ) Calculate numerical values for the wavelength hin in units of the radius a for

the four lowest

and magnetic fields inside the cavity for the lowest TE and lowest TM

( 6 ) Calculate numerical values for the wavelength hin in units of the radius a for

the four lowest

**modes**for TE and TM waves . ( c ) Calculate explicitly the electricand magnetic fields inside the cavity for the lowest TE and lowest TM

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

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