Difference between revisions of "Heat transfer in a 1D harmonic crystal"
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Theory: [[А.М. Кривцов|A.M. Krivtsov]], published at [http://arxiv.org/abs/1509.02506 arXiv:1509.02506 (cond-mat.stat-mech)] | Theory: [[А.М. Кривцов|A.M. Krivtsov]], published at [http://arxiv.org/abs/1509.02506 arXiv:1509.02506 (cond-mat.stat-mech)] | ||
− | Programming: | + | Programming: D.V. Tsvetkov |
== Microscopic model == | == Microscopic model == |
Revision as of 21:41, 7 October 2015
Anton Krivtsov > Heat transfer in a 1D harmonic crystalTheory: A.M. Krivtsov, published at arXiv:1509.02506 (cond-mat.stat-mech)
Programming: D.V. Tsvetkov
Contents
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.Simulation: evolution of the spatial distribution of the kinetic temperature
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.