## Encyclopedia of Physical Science and Technology, Volume 10 |

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Page 541

is a nonnegative distortion measure , and x and y are

XN - 1 ) and y = ( yi , y2 , . . . , yn ) , respectively . Upon defining Pi Pr ( xk - 1 < U S

xk ) , k = 1 , 2 , . . . , N ( 40 ) the entropy at the quantizer output is

is a nonnegative distortion measure , and x and y are

**given**by x = ( x1 , x2 , . . . ,XN - 1 ) and y = ( yi , y2 , . . . , yn ) , respectively . Upon defining Pi Pr ( xk - 1 < U S

xk ) , k = 1 , 2 , . . . , N ( 40 ) the entropy at the quantizer output is

**given**by N H ...Page 715

ensemble average or equivalently the average value of any classical dynamical

variable O ( pN , qN ) associated with a classical system by using the relation "

N O ( pN ...

**Given**the density distribution function p ( pN , q ^ ) , we can compute theensemble average or equivalently the average value of any classical dynamical

variable O ( pN , qN ) associated with a classical system by using the relation "

N O ( pN ...

Page 742

Now the spectral density of the force fluctuations is

- iwt % f ( t ) · F ( O ) eq From these results , we see that the frictional damping of

the particle momentum arises from spontaneous equilibrium fluctuations in the ...

Now the spectral density of the force fluctuations is

**given**by Čislim ) = $ * dt exp (- iwt % f ( t ) · F ( O ) eq From these results , we see that the frictional damping of

the particle momentum arises from spontaneous equilibrium fluctuations in the ...

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### Contents

Seismology Observational 17 Stochastic Description | 325 |

Semiconductor Alloys LongRange and Karl Friedrich | 349 |

Sequency and Series 73 Solar Energy Engineering | 361 |

Copyright | |

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