Spatial distribution of thermal energy in equilibrium.
@article{BarSinai2015SpatialDO, title={Spatial distribution of thermal energy in equilibrium.}, author={Yohai Bar-Sinai and Eran Bouchbinder}, journal={Physical review. E, Statistical, nonlinear, and soft matter physics}, year={2015}, volume={91 6}, pages={ 060103 } }
The equipartition theorem states that in equilibrium, thermal energy is equally distributed among uncoupled degrees of freedom that appear quadratically in the system's Hamiltonian. However, for spatially coupled degrees of freedom, such as interacting particles, one may speculate that the spatial distribution of thermal energy may differ from the value predicted by equipartition, possibly quite substantially in strongly inhomogeneous or disordered systems. Here we show that for systems…
3 Citations
Effects of geometrical structure on spatial distribution of thermal energy in two-dimensional triangular lattices
- Physics, MathematicsPhysica A: Statistical Mechanics and its Applications
- 2018
Local thermal energy as a structural indicator in glasses
- Materials ScienceProceedings of the National Academy of Sciences
- 2017
This work proposes that fluctuational thermal energy reveals highly localized and soft structures in glasses, and shows that the degree of softness of these “soft spots” follows a universal fat-tailed statistical distribution and relate it to the density of noncrystalline vibrational states.
Thermal fracture kinetics of heterogeneous semiflexible polymers.
- BiologySoft matter
- 2020
The results presented here point to a potential mechanism for disassembly of polymeric materials in general and cytoskeletal actin networks in particular by the introduction of locally softened chain regions, as occurs with cofilin binding.
8 References
Matrix Analysis and Applied Linear Algebra
- Mathematics
- 2000
The author presents Perron-Frobenius theory of nonnegative matrices Index, a theory of matrices that combines linear equations, vector spaces, and matrix algebra with insights into eigenvalues and Eigenvectors.
To keep the springs constants positive, we used kα = max(κi, κm), where κi are normally distributed
and E
- M. De La Cruz, J. Mol. Biol. 381, 550
- 2008
Whenever H is non-invertible, i.e. in the presence of Goldstone modes, the notation H −1 should be interpreted as the Moore-Penrose pseudoinverse
Biophys
- J. 80, 505
- 2001