Barry Koren, Jasper Kreeft, Jeroen Wackers A New Model and Numerical Method for Compressible...
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Transcript of Barry Koren, Jasper Kreeft, Jeroen Wackers A New Model and Numerical Method for Compressible...
Barry Koren, Jasper Kreeft, Jeroen Wackers
A New Model and Numerical Method for Compressible Two-Fluid Euler Flow
HYP2012, PadovaJune 28, 2012
Contents
• Introduction
• Flow model
• Flow solver
• Flow problems
• Conclusions
Introduction Flow Model Flow Solver Flow Problems Conclusions
Introduction
Two-fluid interface
Introduction Flow Model Flow Solver Flow Problems Conclusions
Separates two fluids
Divide domain in small volumes
Interface Capturing
Introduction Flow Model Flow Solver Flow Problems Conclusions
• Not applicable: single-fluid flow models only
• Not directly imposable: boundary conditions at interface
Flow Model
Euler equations
Mass
Momentum
Energy
Rate of changeof mass
Mass transport across boundary
Introduction Flow Model Flow Solver Flow Problems Conclusions
Interface-capturing model
Assumptions
• Equal velocities
• Equal pressures
Introduction Flow Model Flow Solver Flow Problems Conclusions
Interface-capturing model
Assumptions• Equal velocities• Equal
pressures
Introduction Flow Model Flow Solver Flow Problems Conclusions
Interface-capturing model
Volume fraction:
Bulk mass
Bulk momentum
Bulk energy
Mass fluid 1
Energy fluid 1
Introduction Flow Model Flow Solver Flow Problems Conclusions
2 equations of state
Energy-exchange terms
Quasi-1D channel flow 1D two-fluid flow
Introduction Flow Model Flow Solver Flow Problems Conclusions
Pressure force due to change in volume fraction
Energy-exchange terms
Friction force to keep velocities equal
Introduction Flow Model Flow Solver Flow Problems Conclusions
Energy-exchange terms
Compression or expansion
Isentropic compressibility
Energy exchange to keep pressures equal
Introduction Flow Model Flow Solver Flow Problems Conclusions
Flow Solver
Finite-volume discretization
• Integral form:
?
• Time stepping:three-stage explicit Runge-Kutta
• Monotone second-order accurate spatial discretization: limiter BK
• Flux vector evaluation: Approximate Riemann solver
Introduction Flow Model Flow Solver Flow Problems Conclusions
Energy-exchange-term evaluation
Introduction Flow Model Flow Solver Flow Problems Conclusions
In solution space:
Flow Problems
Shock-tube problems
• Exact solutions known
• Perfect gases
Introduction Flow Model Flow Solver Flow Problems Conclusions
Translating-interface problem
Pressure Volume fractionDensity
Introduction Flow Model Flow Solver Flow Problems Conclusions
Pressure-oscillation-free without special precaution
No-reflection problemIntroduction Flow Model Flow Solver Flow Problems Conclusions
• Shock hitting interface• Density distributions• Influence of energy-exchange term
Without exchange term With exchange term
Water-air mixture problem
Introduction Flow Model Flow Solver Flow Problems Conclusions
Shock-bubble interaction problem
R22 – Higher density and lower ratio of specific heats than air lower speed of sound
Helium – Lower density and higher ratio of specific heats than air higher speed of sound
Introduction Flow Model Flow Solver Flow Problems Conclusions
R22 – density
Introduction Flow Model Flow Solver Flow Problems Conclusions
Comparison with experiment
Introduction Flow Model Flow Solver Flow Problems Conclusions
Introduction Flow Model Flow Solver Flow Problems Conclusions
Helium bubble – density
Comparison with experiment
Introduction Flow Model Flow Solver Flow Problems Conclusions
Conclusions
• New five-equation model (improvement to Kapila’s model); with energy-exchange laws
• Approximate Riemann solver used for both flux and energy-exchange evaluation • Mixture flows can also be computed
• Physically correct solutions without tuning or post-processing
• J.J. Kreeft and BK, J. Comput. Phys., 229, 6220-6242
• Room for further extensions and applications
Introduction Flow Model Flow Solver Flow Problems Conclusions
Thank you for your interest