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A LATTICE BOLTZMANN MODEL FOR COMPRESSIBLE PERFECT GAS 被引量:4
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作者 胡守信 阎广武 施卫平 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 1997年第3期218-226,共9页
A new lattice Boltzmann model for compressible perfect gas is proposed. The numerical example shows that it can be used to simulate shock wave and contact discontinuity. The results are comparable with those obtained ... A new lattice Boltzmann model for compressible perfect gas is proposed. The numerical example shows that it can be used to simulate shock wave and contact discontinuity. The results are comparable with those obtained by traditional methods. The ratio of specific heats gamma may be chosen according to the requirement of problems. 展开更多
关键词 lattice Boltzmann method COMPRESSIBLE perfect gas general case of the ratio of specific heats two-speed three-energy-level model
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LATTICE-BOLTZMANN MODEL FOR COMPRESSIBLE PERFECT GASES 被引量:1
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作者 孙成海 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2000年第4期289-300,共12页
We present an adaptive lattice Boltzmann model to simulate super- sonic flows.The particle velocities are determined by the mean velocity and internal energy.The adaptive nature of particle velocities permits the mean... We present an adaptive lattice Boltzmann model to simulate super- sonic flows.The particle velocities are determined by the mean velocity and internal energy.The adaptive nature of particle velocities permits the mean flow to have high Mach number.A particle potential energy is introduced so that the model is suitable for the perfect gas with arbitrary specific heat ratio.The Navier-Stokes equations are derived by the Chapman-Enskog method from the BGK Boltzmann equation. As preliminary tests,two kinds of simulations have been performed on hexagonal lattices.One is the one-dimensional simulation for sinusoidal velocity distributions. The velocity distributions are compared with the analytical solution and the mea- sured viscosity is compared with the theoretical values.The agreements are basically good.However,the discretion error may cause some non-isotropic effects.The other simulation is the 29 degree shock reflection. 展开更多
关键词 lattice Boltzmann Euler equation N-S equation adaptive velocities perfect gas
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Stagnation temperature effect on the conical shock with application for air 被引量:1
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作者 Toufik ELAICHI Toufik ZEBBICHE 《Chinese Journal of Aeronautics》 SCIE EI CAS CSCD 2018年第4期672-697,共26页
The aim of this work is to realize a new numerical program based on the development of a mathematical model allowing determining the parameters of the supersonic flow through a conical shock under hypothesis at high t... The aim of this work is to realize a new numerical program based on the development of a mathematical model allowing determining the parameters of the supersonic flow through a conical shock under hypothesis at high temperature, in the context of correcting the perfect gas model. In this case, the specific heat at constant pressure does not remain constant and varies with the increase of temperature. The stagnation temperature becomes an important parameter in the calculation.The mathematical model is presented by the numerical resolution of a system of first-order nonlinear differential equations with three coupled unknowns for initial conditions. The numerical resolution is made by adapting the higher order Runge Kutta method. The parameters through the conical shock can be determined by considering a new model of an oblique shock at high temperature. All isentropic parameters of after the shock flow depend on the deviation of the flow from the transverse direction. The comparison of the results is done with the perfect gas model for low stagnation temperatures, upstream Mach number and cone deviation angle. A calculation of the error is made between our high temperature model and the perfect gas model. The application is made for air. 展开更多
关键词 Calorically imperfect gas Conical shock High temperature Numerical integration Oblique shock perfect gas model Runge Kutta method Supersonic flow
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Adaptive Lattice Boltzmann Model for Compressible Flows
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作者 孙成海 王保国 沈孟育 《Tsinghua Science and Technology》 EI CAS 2000年第1期43-46,共4页
A new lattice Boltzmann model for compressible flows is presented. The main difference from the standard lattice Boltzmann model is that the particle velocities are no longer constant, but vary with the mean velocity ... A new lattice Boltzmann model for compressible flows is presented. The main difference from the standard lattice Boltzmann model is that the particle velocities are no longer constant, but vary with the mean velocity and internal energy. The adaptive nature of the particle velocities permits the mean flow to have a high Mach number. The introduction of a particle potential energy makes the model suitable for a perfect gas with arbitrary specific heat ratio. The Navier Stokes (N\|S) equations are derived by the Chapman Enskog method from the BGK Boltzmann equation. Two kinds of simulations have been carried out on the hexagonal lattice to test the proposed model. One is the Sod shock tube simulation. The other is a strong shock of Mach number 5 09 diffracting around a corner. 展开更多
关键词 lattice Boltzmann Euler equation N S equation adaptive velocity perfect gas
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