Radial thermal rectification in the concentric silicon ring from ballistic to diffusive regime
arXiv:1910.04412
Abstract
The radial thermal rectification in the concentric silicon ring from ballistic to diffusive regime is investigated based on the phonon Boltzmann transport equation. In the ballistic and diffusive limits, the analytical solutions prove that there is no thermal rectification. In the ballistic-diffusive regime, the heat flux prefers to flow from the inner boundary to the outer boundary. Furthermore, as the characteristic length (the distance between two circular boundaries) increases from tens of nanometers to tens of microns, the thermal rectification ratio enhances first and then fades away gradually. It attributes to that as the direction of the temperature gradient changes, the average phonon mean free path changes. The difference of the average phonon mean free path finally leads to the change of the heat flux or thermal conductivity. As the temperature decreases, the maximum thermal rectification ratio decreases. In addition, as the radius ratio between the inner and outer boundary increases, the thermal rectification ratio decreases for a given characteristic length.
arXiv comment17 pages, 10 figures, 53 references
References in corpus (14)
- Phononics: Manipulating heat flow with electronic analogs and beyond
- Thermal diode: Rectification of heat flux
- Thermal Conductivity and Thermal Rectification in Graphene Nanoribbons: a Molecular Dynamics Study
- Thermal Logic Gates: Computation with phonons
- Controlling the energy flow in nonlinear lattices: a model for a thermal rectifier
- An oxide thermal rectifier
- Thermal transport in nanostructures
- The design of a thermal rectifier
- Thermal rectification in bulk materials with asymmetric shape
- Negative differential thermal resistance induced by ballistic transport
- Nanoscale Graphene Disk: A Natural Functionally Graded Material --The Thermal Conductivity of Nanoscale Graphene Disk by Molecular Dynamics Simulation
- Modeling semi-conductor thermal properties. The dispersion role
- Heat conduction in deformable Frenkel-Kontorova lattices: thermal conductivity and negative differential thermal resistance
- Double negative differential thermal resistance induced by the nonlinear on-site potentials