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Specific heat in a nonequilibrium system composed of Einstein oscillators
Toshiaki Tao1, Akira Yoshimori, Takashi Odagaki
1Department of Physics, Faculty of Science, Kyushu University, Fukuoka 812-8581, Japan.
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|November 22, 2002
Summary
This study models specific heat near the glass transition temperature by combining energy landscapes and particle jumps. Longer observation times shift the annealed-to-quenched transition to lower temperatures, making it sharper.
Area of Science:
- Condensed Matter Physics
- Statistical Mechanics
- Physical Chemistry
Background:
- Understanding thermodynamic properties near the glass transition temperature (Tg) is crucial.
- Nonequilibrium systems exhibit complex behaviors influenced by dynamics and observation time.
- The energy landscape theory provides a framework for analyzing complex systems.
Purpose of the Study:
- To calculate the specific heat of a nonequilibrium system near Tg.
- To investigate the influence of finite observation time on specific heat.
- To connect particle jump dynamics and energy landscapes to thermodynamic behavior.
Main Methods:
- Integration of the energy landscape picture with particle jump motion.
- Calculation of specific heat for a nonequilibrium system.
- Modeling system dynamics using Einstein oscillators within a 20-basin phase space structure.
- Analysis of the dependence of specific heat on observation time.
Main Results:
- A transition from annealed to quenched system behavior was identified.
- This transition occurs when the particle jump timescale exceeds the observation time.
- The transition temperature shifts to lower values with increasing observation time.
- Longer observation times result in a sharper transition.
Conclusions:
- Finite observation time significantly impacts the thermodynamic behavior of systems near Tg.
- The interplay between energy landscape, particle dynamics, and observation time governs the observed specific heat.
- The study provides a framework for understanding glassy dynamics in terms of observable thermodynamic quantities.