general-purpose simulation tools Search Results


90
ANSYS inc general purpose finite element analysis software
General Purpose Finite Element Analysis Software, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc comsol multiphysics
Comsol Multiphysics, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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86
Molecular Dynamics Inc generalpurpose molecular dynamics software package lammps
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Generalpurpose Molecular Dynamics Software Package Lammps, supplied by Molecular Dynamics Inc, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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90
COMSOL Inc multiphysics general-purpose physics simulation software
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Multiphysics General Purpose Physics Simulation Software, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc commercial general-purpose simulation software
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Commercial General Purpose Simulation Software, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc generalpurpose simulation software comsol-multiphysics
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Generalpurpose Simulation Software Comsol Multiphysics, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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ANSYS inc multi-purpose general fea simulation software ansys workbench v2024r1
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Multi Purpose General Fea Simulation Software Ansys Workbench V2024r1, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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96
MathWorks Inc general purpose state flow
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
General Purpose State Flow, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 96/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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96
MathWorks Inc simulation tools
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Simulation Tools, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 96/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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90
ANSYS inc fem analysis software ansys mechanical
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Fem Analysis Software Ansys Mechanical, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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90
SCAPS GmbH scaps 1d
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
Scaps 1d, supplied by SCAPS GmbH, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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ANSYS inc general-purpose structure analysis tool
Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package <t>LAMMPS</t> [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a
General Purpose Structure Analysis Tool, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Image Search Results


Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package LAMMPS [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a

Journal: Computer Physics Communications

Article Title: A coherent phonon pulse model for transient phonon thermal transport

doi: 10.1016/j.cpc.2015.05.008

Figure Lengend Snippet: Fig. 1: (a) Wave packet composed of Gaussian waves. (b) Fourier Transform of the wave packet in (a), inset in (b) is the PDOS of SiNW at 500K computed from MD results. In Fig. 2, we present the schematic of the computational model (~600,000 atoms, ~ 3 3 1.2 nm nm m μ × × ). The general- purpose molecular dynamics software package LAMMPS [45] is employed in all the simulations in this work without assuming periodic boundary conditions. Velocity Verlet algorithm with time step of 0.55fs is used, which is about 1% of the shortest phonon period in Si lattice. Before the heat pulse is generated, the MD model is equilibrated at 0.1K to allow only the scattering events that involve phonons generated from the heat source. Note that with a higher initial temperature, the scattering events involve the original thermal phonons can be naturally incorporated. Thereafter, the heat pulse constructed by CPP model is applied in the middle of the Grain I, and naturally allowed in the MD simulations to propagate across the GBs into the Grain II (positive z) and the Grain III (negative z) at the two ends of the NW. With the heat source region located at the center of the Grain I, unwanted phonon scatterings by free boundaries are avoided. Since the model is symmetric, only half of which is of interest, we take it as a

Article Snippet: The generalpurpose molecular dynamics software package LAMMPS [45] is employed in all the simulations in this work without assuming periodic boundary conditions.

Techniques: Software, Generated, Construct