numerical modeling of compressible two-phase flows hervé guillard inria sophia-antipolis, pumas...
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NUMERICAL MODELING OF COMPRESSIBLE TWO-PHASE FLOWS
Hervé Guillard
INRIA Sophia-antipolis, Pumas Team, B.P. 93, 06902 Sophia-Antipolis Cedex, France,[email protected]
Thanks to Fabien Duval, Mathieu Labois, Angelo Murrone, Roxanna Panescu, Vincent Perrier
Example of Interface problems : Shock-bubble interaction
Non structured tet mesh : 18M nodes 128 processors 3h30 h
model suitable for two fluid studies :
no general agreement
large # of different models : homogeneous,
mixture models, two-fluid models, drift-flux
models
number of variables,
definition of the unknowns
number of equations
large # of different approximations
conservative, non-conservative, incompressible vs incompressible techniques,
TWO-PHASE MODELS
-Construction of a general 2-phase model
- Non-equilibrium thermodynamics of two phase non-miscible mixtures
- Equilibria in two phase mixture
-Reduced “hyperbolic” models for equilibrium situations
- Technical tool : Chapman-Enskog expansion
- A hierarchy of models
- Some examples
- Reduced “parabolic” models
- First-order Chapman-Enskog expansion
- Iso-pressure, iso-velocity model
- Traveling waves and the structure of two-phase shock
OVERVIEW OF THIS TALK
HOMOGENIZED MODELS
Reference textbooks : Ishii (1984), Drew-Passman (1998)
Let us consider 2 unmiscible fluids described by the Euler eq
Introduce averaging operators
Let X_k be the characteristic function of the fluid region k
where σ is the speed of the interface
Let f be any regular enough function
Define averaged quantities :
etc
Multiply the eq by X_k and apply Gauss and Leibnitz rules
Assume :
Then first line :
One important remark (Coquel, Gallouet,Herard, Seguin, CRAS 2002) :
The two-fluid system + volume fraction equation is (always) hyperbolic
but
the field associated with the eigenvalue
is linearly degenerate if and only if
Summary
- Two fluid system + volume fraction eq = hyperbolic system
the entropy production terms are positive
- This system evolves to a state characterized by
- pressure equality - velocity equality
- temperature equality
- chemical potential equality
Deduce from this system, several reduced systems
characterized by instantaneous equilibrium between
- pressure
- pressure + velocity
- pressure + velocity + temperature
- .............
One example : Bubble column : AMOVI MOCK UP (CEA Saclay)
Pressure relaxation time
Velocity relaxation time
Temperature relaxation time
Bubble transit time
Construction of reduced models :
Technical tool : The Chapmann-Enskog expansion
What is a Chapman-Enskog asymptotic expansion ?
- technique introduced by Chapmann and Enskog
to compute the transport coefficients of the Navier-Stokes
equations from the Boltzmann equations-technique used in the Chen-Levermore paper on hyperbolic
relaxation problems
Some examples : Assume pressure equilibrium :
“classical” two-fluid model (Neptune)
eos : solve p1 = p2 for the volume fraction
Non-hyperbolic !
Some examples : Assume : - pressure equilibrium
- velocity equilibrium one-pressure, one velocity model (Stewart-Wendroff 1984, Murrone-Guillard, 2005)
one-pressure, one velocity model (Stewart-Wendroff 1984, Murrone-Guillard, 2005)
Hyperbolic system
u-c, u+c gnl, u,u ldEntropy
Some examples : Assume - pressure equilibrium - velocity equilibrium
- temperature equilibrium
Multi-component Euler equations :
eos : solve : p1 = p2, T1=T2
A Small summary :
Model # eqs complexity hyperbolic conservative contact respect
total nonequilibrium 7 +++ yes no yes
pressure equilibrium 6 +++ no no ?
pressure andvelocityequilibrium 5 ++ yes no yes
pressure andvelocity andtemperature 4 + yes yes noequilibrium
Why the 4 equation conservative model cannot compute a contact
1
u
p
Ti
0
u
p
Ti+1
1
u
p
Ti
Y
u
p
T
1
u
p
Ti
1
u
p
Ti
0
u
p
Ti+1
Not possible at constant pressure
keeping constant the conservative
variables
R. Abgrall, How to prevent pressure oscillations in multi-component flow calculation: a quasi-conservative approach, JCP, 1996
Mathematical properties of the model :
First-order part : hyperbolic Second-order part : dissipative
Comparison of non-equilibrium model (7 eqs) Vs Equilibrium model (5 eqs) with dissipative Terms (air-water shock tube pb)
Sedimentation test-case (Stiffened gas state law)
Note : velocities of air and water are of opposite sign
Sedimentation test-case (Perfect gas state law)
Note : velocities of air and water are of opposite sign
5 eqs dissipative model Non-equilibrium model
Two-phase flows models have non-conservative form
Non-conservative models : Definition of shock solution
Traveling waves
Weak point of the model : Non conservative form
Shock solutions are not defined
One answer : LeFloch, Raviart-Sainsaulieu
change
into
Define the shock solutions as limits of travelling waves solution of the regularized dissipative system for
Drawback of the approach : the limit solution depends on the
viscosity tensor
How to be sure that the viscosity tensor
encode the right physical informations ?
The dissipative tensor retains physical informations comingfrom the non-equilibrium modell
ISOTHERMAL MODEL with DARCY-LIKE DRIFT LAWISOTHERMAL MODEL with DARCY-LIKE DRIFT LAW
Rankine-Hugoniot Relations :
TRAVELLING WAVES II
If TW exists, they are characterized by a differential system of Degree 2
Isothermal case : This ODE has two equilibrium point
Stable one
unstable one
CONCLUSIONS
- Hierarchy of two-fluid models characterized by stronger
and stronger assumptions on the equilibriums realized in
the two fluid system
- on-going work to define shock solutions for two-phase model
as limit of TW of a dissipative system characterized by a
viscosity tensor that retain physical informations on
disequilibrium