Statistical PhysicsElementary college physics course for students majoring in science and engineering. |
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Page 104
... particle ; it is re- lated to the wavelength λ ( the so - called de Broglie wavelength associated with the particle ) by the relation K = 2π λ Hence ... particle now represents a standing 104 Statistical Description of Systems of Particles.
... particle ; it is re- lated to the wavelength λ ( the so - called de Broglie wavelength associated with the particle ) by the relation K = 2π λ Hence ... particle now represents a standing 104 Statistical Description of Systems of Particles.
Page 139
... particle in this state is thus -F , dL , and must be equal to the increase in energy dE , of the particle in this state . Thus one has dEr = -F , dLr . ( i ) The force F , exerted by a particle in the state r is thus related to the ...
... particle in this state is thus -F , dL , and must be equal to the increase in energy dE , of the particle in this state . Thus one has dEr = -F , dLr . ( i ) The force F , exerted by a particle in the state r is thus related to the ...
Page 229
... particle are then restricted by a condi- tion of the form 0 < x < L. The energy E of the particle of mass m is merely its kinetic energy so that v E = · mv2 = 2 1 p2 2 m = mv is the where is the velocity and p momentum of the particle ...
... particle are then restricted by a condi- tion of the form 0 < x < L. The energy E of the particle of mass m is merely its kinetic energy so that v E = · mv2 = 2 1 p2 2 m = mv is the where is the velocity and p momentum of the particle ...
Contents
Characteristic Features of Macroscopic Systems | 1 |
Basic Probability Concepts | 55 |
Thermal Interaction | 141 |
Copyright | |
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absolute temperature absorbed accessible approximation assume atoms average calculate classical collision Consider constant container cules definition denote discussion distribution electron ensemble entropy equal equilibrium situation equipartition theorem example expression external parameters fluctuations fluid function Gibbs free energy given heat capacity heat Q heat reservoir Hence ideal gas initial internal energy isolated system kinetic energy large number left half liquid macroscopic system macrostate magnetic field magnetic moment magnitude mass maximum mean energy mean number mean pressure mean value measured mole molecular momentum n₁ number of molecules occur oscillator particle particular phase phase space piston plane Poisson distribution position possible values Prob probability P(n quantity quantum numbers quasi-static random relation result simply solid specific heat statistical statistical ensemble statistically independent Suppose thermal contact thermally insulated thermometer tion total energy total number unit volume velocity