Compositional Multiphase Flow Solver

Introduction

This flow solver is in charge of implementing the finite-volume discretization (mainly, accumulation and flux terms, boundary conditions) of the equations governing compositional multiphase flow in porous media. The present solver can be combined with the Compositional Multiphase Well Solver which handles the discrete multi-segment well model and provides source/sink terms for the fluid flow solver.

Below, we first review the set of Governing Equations, followed by a discussion of the choice of Primary Variables used in the global variable formulation. Then we give an overview of the Discretization and, finally, we provide a list of the solver Parameters and an input Example.

Theory

Governing Equations

Mass Conservation Equations

Mass conservation for component c is expressed as:

\phi \frac{ \partial  }{\partial t} \bigg( \sum_\ell \rho_{\ell} \, y_{c \ell} \, S_{\ell} \bigg)
+ \nabla \cdot \bigg( \sum_\ell \rho_{\ell} \, y_{c \ell} \, \boldsymbol{u}_{\ell} \bigg)
- \sum_\ell \rho_{\ell} \, y_{c \ell} \, q_{\ell} = 0,

where \phi is the porosity of the medium, S_{\ell} is the saturation of phase \ell, y_{c \ell} is the mass fraction of component c in phase \ell, \rho_{\ell} is the phase density, and t is time. We note that the formulation currently implemented in GEOS is isothermal.

Darcy’s Law

Using the multiphase extension of Darcy’s law, the phase velocity \boldsymbol{u}_{\ell} is written as a function of the phase potential gradient \nabla \Phi_{\ell}:

\boldsymbol{u}_{\ell} := -\boldsymbol{k} \lambda_{\ell} \nabla \Phi_{\ell}
= - \boldsymbol{k} \lambda_{\ell} \big( \nabla (p - P_{c,\ell}) - \rho_{\ell} g \nabla z \big).

In this equation, \boldsymbol{k} is the rock permeability, \lambda_{\ell} = k_{r \ell} / \mu_{\ell} is the phase mobility, defined as the phase relative permeability divided by the phase viscosity, p is the reference pressure, P_{c,\ell} is the the capillary pressure, g is the gravitational acceleration, and z is depth. The evaluation of the relative permeabilities, capillary pressures, and viscosities is reviewed in the section about Constitutive Models.

Combining the mass conservation equations with Darcy’s law yields a set of n_c equations written as:

\phi \frac{ \partial  }{\partial t} \bigg( \sum_\ell \rho_{\ell} \, y_{c \ell} \, S_{\ell} \bigg)
- \nabla \cdot \boldsymbol{k} \bigg( \sum_\ell \rho_{\ell} \, y_{c \ell} \, \lambda_{\ell} \nabla \Phi_{\ell}   \bigg)
- \sum_\ell \rho_{\ell} \, y_{c \ell} \, q_{\ell} = 0.

Constraints and Thermodynamic Equilibrium

The volume constraint equation states that the pore space is always completely filled by the phases. The constraint can be expressed as:

\sum_{\ell} S_{\ell} = 1.

The system is closed by the following thermodynamic equilibrium constraints:

f_{c \ell} - f_{c m} = 0.

where f_{c \ell} is the fugacity of component c in phase \ell. The flash calculations performed to enforce the thermodynamical equilibrium are reviewed in the section about Constitutive Models.

To summarize, the compositional multiphase flow solver assembles a set of n_c+1 equations in each element, i.e., n_c mass conservation equations and one volume constraint equation. A separate module discussed in the Constitutive Models is responsible for the enforcement of the thermodynamic equilibrium at each nonlinear iteration.

Number of equations

Equation type

n_c

Mass conservation equations

1

Volume constraint

Primary Variables

The variable formulation implemented in GEOS is a global variable formulation based on n_c+1 primary variables, namely, one pressure, p, and n_c component densities, \rho_c. By default, we use molar component densities. A flag discussed in the section Parameters can be used to select mass component densities instead of molar component densities.

Number of primary variables

Variable type

1

Pressure

n_c

Component densities

Assembling the residual equations and calling the Constitutive Models requires computing the molar component fractions and saturations. This is done with the relationship:

z_c := \frac{\rho_c}{\rho_T},

where

\rho_T := \sum_c \rho_c.

These secondary variables are used as input to the flash calculations. After the flash calculations, the saturations are computed as:

S_{\ell} := \nu_{\ell} \frac{ \rho_T }{ \rho_{\ell}},

where \nu_{\ell} is the global mole fraction of phase \ell and \rho_{\ell} is the molar density of phase \ell. These steps also involve computing the derivatives of the component fractions and saturations with respect to the pressure and component densities.

Discretization

Spatial Discretization

The governing equations are discretized using standard cell-centered finite-volume discretization.

In the approximation of the flux term at the interface between two control volumes, the calculation of the pressure stencil is general and will ultimately support a Multi-Point Flux Approximation (MPFA) approach. The current implementation of the transmissibility calculation is reviewed in the section about Numerical Methods.

The approximation of the dynamic transport coefficients multiplying the discrete potential difference (e.g., the phase mobilities) is performed with a first-order phase-per-phase single-point upwinding based on the sign of the phase potential difference at the interface.

Temporal Discretization

The compositional multiphase solver uses a fully implicit (backward Euler) temporal discretization.

Solution Strategy

The nonlinear solution strategy is based on Newton’s method. At each Newton iteration, the solver assembles a residual vector, R, collecting the n_c discrete mass conservation equations and the volume constraint for all the control volumes.

Parameters

The following attributes are supported:

XML Element: CompositionalMultiphaseFVM

Name

Type

Default

Description

allowLocalCompDensityChopping

integer

1

Flag indicating whether local (cell-wise) chopping of negative compositions is allowed

allowNegativePressure

integer

1

Flag indicating if negative pressure is allowed

cflFactor

real64

0.5

Factor to apply to the CFL condition when calculating the maximum allowable time step. Values should be in the interval (0,1]

contMultiplierDBC

real64

0.5

Factor by which continuation parameter is changed every newton when DBC is used

continuationDBC

integer

1

Flag for enabling continuation parameter

discretization

groupNameRef

required

Name of discretization object (defined in the Numerical Methods) to use for this solver. For instance, if this is a Finite Element Solver, the name of a Finite Element Discretization should be specified. If this is a Finite Volume Method, the name of a Finite Volume Discretization discretization should be specified.

initialDt

real64

1e+99

Initial time-step value required by the solver to the event manager.

isThermal

integer

0

Flag indicating whether the problem is thermal or not.

kappaminDBC

real64

1e-20

Factor that controls how much dissipation is kept in the system when continuation is used

logLevel

integer

0

Sets the level of information to write in the standard output (the console typically).
Level 0 outputs no specific information for this solver. Higher levels require more outputs.
1
- Line search information
- Solution information (scaling, maximum changes, quality check)
- Convergence information
- Time step information
- Linear solver information
- Nonlinear solver information
- Solver timers information
2
- The summary of declared fields and coupling

maxAbsolutePressureChange

real64

-1

Maximum (absolute) pressure change in a Newton iteration

maxCompFractionChange

real64

0.5

Maximum (absolute) change in a component fraction in a Newton iteration

maxRelativeCompDensChange

real64

1.79769e+208

Maximum (relative) change in a component density in a Newton iteration

maxRelativePressureChange

real64

0.5

Maximum (relative) change in pressure in a Newton iteration

maxRelativeTemperatureChange

real64

0.5

Maximum (relative) change in temperature in a Newton iteration

maxSequentialCompDensChange

real64

1

Maximum (absolute) component density change in a sequential iteration, used for outer loop convergence check

maxSequentialPressureChange

real64

100000

Maximum (absolute) pressure change in a sequential iteration, used for outer loop convergence check

maxSequentialTemperatureChange

real64

0.1

Maximum (absolute) temperature change in a sequential iteration, used for outer loop convergence check

minCompDens

real64

1e-10

Minimum allowed global component density

minScalingFactor

real64

0.01

Minimum value for solution scaling factor

miscibleDBC

integer

0

Flag for enabling DBC formulation with/without miscibility

name

groupName

required

A name is required for any non-unique nodes

omegaDBC

real64

1

Factor by which DBC flux is multiplied

scalingType

geos_CompositionalMultiphaseFVM_ScalingType

Global

Solution scaling type.Valid options:
* Global
* Local

solutionChangeScalingFactor

real64

0.5

Damping factor for solution change targets

targetFlowCFL

real64

-1

Target CFL condition CFL condition when computing the next timestep.

targetPhaseVolFractionChangeInTimeStep

real64

0.2

Target (absolute) change in phase volume fraction in a time step

targetRegions

groupNameRef_array

required

Allowable regions that the solver may be applied to. Note that this does not indicate that the solver will be applied to these regions, only that allocation will occur such that the solver may be applied to these regions. The decision about what regions this solver will beapplied to rests in the EventManager.

targetRelativeCompDensChangeInTimeStep

real64

1.79769e+308

Target (relative) change in component density in a time step

targetRelativePressureChangeInTimeStep

real64

0.2

Target (relative) change in pressure in a time step (expected value between 0 and 1)

targetRelativeTemperatureChangeInTimeStep

real64

0.2

Target (relative) change in temperature in a time step (expected value between 0 and 1)

temperature

real64

required

Temperature

useDBC

integer

0

Enable Dissipation-based continuation flux

useMass

integer

0

Use mass formulation instead of molar. Warning : Affects SourceFlux rates units.

useNewGravity

integer

0

Flag indicating whether new gravity treatment is used

useSimpleAccumulation

integer

1

Flag indicating whether simple accumulation form is used

useTotalMassEquation

integer

1

Flag indicating whether total mass equation is used

writeLinearSystem

integer

0

Write matrix, rhs, solution to screen ( = 1) or file ( = 2).

LinearSolverParameters

node

unique

XML Element: LinearSolverParameters

NonlinearSolverParameters

node

unique

XML Element: NonlinearSolverParameters

Example

  <Solvers>
    <CompositionalMultiphaseFVM
      name="compflow"
      logLevel="1"
      discretization="fluidTPFA"
      targetRelativePressureChangeInTimeStep="1"
      targetPhaseVolFractionChangeInTimeStep="1"      
      targetRegions="{ Channel }"
      temperature="300">
      <NonlinearSolverParameters
        newtonTol="1.0e-10"
        newtonMaxIter="10"/>
      <LinearSolverParameters
        directParallel="0"/>
    </CompositionalMultiphaseFVM>
  </Solvers>

We refer the reader to Multiphase Flow for a complete tutorial illustrating the use of this solver.