Heat transfer in a 1D harmonic crystal — различия между версиями
Материал из Department of Theoretical and Applied Mechanics
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Programming: [[Д.В. Цветков|D.V. Tsvetkov]] | Programming: [[Д.В. Цветков|D.V. Tsvetkov]] | ||
− | == | + | == Microscopic model == |
We consider a one-dimensional crystal, described by the following equations of motion: | We consider a one-dimensional crystal, described by the following equations of motion: | ||
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</math> | </math> | ||
where <math>\varrho_i</math> are independent random values with zero expectation and unit variance; <math>\sigma</math> is variance of the initial velocities of the particles, which is a slowly varying function of the spatial coordinate <math>x=ia</math>, where <math>a</math> is the lattice constant. These initial conditions correspond to an instantaneous temperature perturbation, which can be induced in crystals, for example, by an ultrashort laser pulse. | where <math>\varrho_i</math> are independent random values with zero expectation and unit variance; <math>\sigma</math> is variance of the initial velocities of the particles, which is a slowly varying function of the spatial coordinate <math>x=ia</math>, where <math>a</math> is the lattice constant. These initial conditions correspond to an instantaneous temperature perturbation, which can be induced in crystals, for example, by an ultrashort laser pulse. | ||
+ | |||
+ | == Kinetic temperature: link between micro and macro == | ||
+ | |||
+ | The kinetic temperature <math>T</math> is defined as | ||
+ | :<math> | ||
+ | T(x) = \frac m{k_{B}}\langle\dot u_i^2\rangle, | ||
+ | </math> | ||
+ | where | ||
+ | <math>k_{B}</math> is the Boltzmann constant, | ||
+ | <math>i=x/a</math>, | ||
+ | angle brackets stand for mathematical expectation. | ||
== Macroscopic equations == | == Macroscopic equations == |
Версия 00:00, 26 сентября 2015
Виртуальная лаборатория > Heat transfer in a 1D harmonic crystal
Theory: A.M. Krivtsov, published at arXiv:1509.02506 (cond-mat.stat-mech)
Programming: D.V. Tsvetkov
Microscopic model
We consider a one-dimensional crystal, described by the following equations of motion:
where
is the displacement of the th particle, is the particle mass, is the stiffness of the interparticle bond. The crystal is infinite: the index is an arbitrary integer. The initial conditions arewhere
are independent random values with zero expectation and unit variance; is variance of the initial velocities of the particles, which is a slowly varying function of the spatial coordinate , where is the lattice constant. These initial conditions correspond to an instantaneous temperature perturbation, which can be induced in crystals, for example, by an ultrashort laser pulse.Kinetic temperature: link between micro and macro
The kinetic temperature
is defined aswhere
is the Boltzmann constant, , angle brackets stand for mathematical expectation.Macroscopic equations
— Heat (Fourier): [1]
— Heat wave (MCV):
— Wave (d’Alembert): [2]
— Reversible (Krivtsov): [3]
Notations:
is time (variable), is the relaxation time (constant), is the thermal diffusivity, is the thermal conductivity, is the sound speed, is the density, MCV stands for Maxwell-Cattaneo-Vernotte.