Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Temperature evolutions for the boson systems (solid line) and that for the fermion systems (dashed line). The concentration is high,
because eγ∼10.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Particle number evolutions for the boson systems (solid line) and that for the fermion systems (dashed line). The concentration is
high, because eγ∼10.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Temperature evolutions for the boson systems (solid line) and that for the fermion systems (dashed line). The solid line and the
dashed line converge. The concentration is low, because eγ≫1.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Particle number evolutions for the boson systems (solid line) and that for fermion systems (dashed line). The solid line and the
dashed line converge. The concentration is low, because eγ≫1.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Temperature evolutions for the boson systems for the four cases. γ a and γb increase and, thus, concentration decreases from the
bottom curve to the top one for system a and from the top curve to the bottom one for system b. γa−γb is kept constant. The curves
for the two low concentration cases converge.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Normalized particle number evolutions for the boson systems for the four cases. γ a and γb increase and, thus, concentration
decreases from the bottom curve to the top one for system a and from the top curve to the bottom one for system b. γa−γb is kept
constant. The curves for the two low concentration cases converge.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Temperature evolutions for the boson systems for different volumes and the same (γa,γb). The curves of the three cases converge.
Date of download: 7/31/2017
Copyright © ASME. All rights reserved.
From: Study of Nonequilibrium Size and Concentration Effects on the Heat and Mass Diffusion of
Indistinguishable Particles Using Steepest-Entropy-Ascent Quantum Thermodynamics
J. Heat Transfer. 2017;139(12):122003-122003-8. doi:10.1115/1.4036735
Figure Legend:
Normalized particle number evolution evolutions for boson systems for different volumes and the same (γa,γb). The curves of the
three cases converge.