def fun_pEqn(mesh, runTime, pimple, thermo, rho, p, h, psi, U, phi, turbulence,
gh, ghf, p_rgh, UEqn, DpDt, cumulativeContErr, corr):
rho << thermo.rho()
# Thermodynamic density needs to be updated by psi*d(p) after the
# pressure solution - done in 2 parts. Part 1:
thermo.rho() << thermo.rho() - psi() * p_rgh() # mixed calculations
rAU = 1.0 / UEqn.A()
rhorAUf = ref.surfaceScalarField(ref.word("(rho*(1|A(U)))"),
ref.fvc.interpolate(rho * rAU))
U << rAU * UEqn.H()
phi << ref.fvc.interpolate(rho) * ((ref.fvc.interpolate(U) & mesh.Sf()) +
ref.fvc.ddtPhiCorr(rAU, rho, U, phi))
buoyancyPhi = -rhorAUf * ghf * ref.fvc.snGrad(rho) * mesh.magSf()
phi += buoyancyPhi
p_rghDDtEqn = ref.fvc.ddt(rho) + psi * ref.correction(
ref.fvm.ddt(p_rgh)) + ref.fvc.div(phi)
for nonOrth in range(pimple.nNonOrthCorr() + 1):
p_rghEqn = p_rghDDtEqn - ref.fvm.laplacian(rhorAUf, p_rgh)
p_rghEqn.solve(
mesh.solver(p_rgh.select(pimple.finalInnerIter(corr, nonOrth))))
if nonOrth == pimple.nNonOrthCorr():
# Calculate the conservative fluxes
phi += p_rghEqn.flux()
# Explicitly relax pressure for momentum corrector
p_rgh.relax()
# Correct the momentum source with the pressure gradient flux
# calculated from the relaxed pressure
U += rAU * ref.fvc.reconstruct(
(buoyancyPhi + p_rghEqn.flux()) / rhorAUf)
U.correctBoundaryConditions()
pass
pass
p << p_rgh + rho * gh
# Second part of thermodynamic density update
thermo.rho() << thermo.rho() + psi() * p_rgh # mixed calculations
DpDt << ref.fvc.DDt(
ref.surfaceScalarField(ref.word("phiU"),
phi() / ref.fvc.interpolate(rho)),
p) # mixed calculations
ref.rhoEqn(rho, phi)
cumulativeContErr = ref.compressibleContinuityErrs(
rho(), thermo, cumulativeContErr) #mixed calculations
return cumulativeContErr
def fun_pEqn(
mesh, runTime, pimple, thermo, rho, p, h, psi, U, phi, turbulence, gh, ghf, p_rgh, UEqn, dpdt, K, cumulativeContErr
):
rho << thermo.rho()
# Thermodynamic density needs to be updated by psi*d(p) after the
# pressure solution - done in 2 parts. Part 1:
thermo.rho() << thermo.rho() - psi() * p_rgh() # mixed calculations
rAU = 1.0 / UEqn.A()
rhorAUf = ref.surfaceScalarField(ref.word("(rho*(1|A(U)))"), ref.fvc.interpolate(rho * rAU))
U << rAU * UEqn.H()
phi << ref.fvc.interpolate(rho) * ((ref.fvc.interpolate(U) & mesh.Sf()) + ref.fvc.ddtPhiCorr(rAU, rho, U, phi))
buoyancyPhi = -rhorAUf * ghf * ref.fvc.snGrad(rho) * mesh.magSf()
phi += buoyancyPhi
p_rghDDtEqn = ref.fvc.ddt(rho) + psi * ref.correction(ref.fvm.ddt(p_rgh)) + ref.fvc.div(phi)
while pimple.correctNonOrthogonal():
p_rghEqn = p_rghDDtEqn - ref.fvm.laplacian(rhorAUf, p_rgh)
p_rghEqn.solve(mesh.solver(p_rgh.select(pimple.finalInnerIter())))
if pimple.finalNonOrthogonalIter():
# Calculate the conservative fluxes
phi += p_rghEqn.flux()
# Explicitly relax pressure for momentum corrector
p_rgh.relax()
# Correct the momentum source with the pressure gradient flux
# calculated from the relaxed pressure
U += rAU * ref.fvc.reconstruct((buoyancyPhi + p_rghEqn.flux()) / rhorAUf)
U.correctBoundaryConditions()
K << 0.5 * U.magSqr()
pass
pass
p << p_rgh + rho * gh
# Second part of thermodynamic density update
thermo.rho() << thermo.rho() + psi() * p_rgh # mixed calculations
dpdt << ref.fvc.ddt(p) # mixed calculations
ref.rhoEqn(rho, phi)
cumulativeContErr = ref.compressibleContinuityErrs(rho(), thermo, cumulativeContErr) # mixed calculations
return cumulativeContErr
def fun_pEqn( i, mesh, p, rho, turb, thermo, thermoFluid, K, UEqn, U, phi, psi, DpDt, initialMass, p_rgh, gh, ghf, \
nNonOrthCorr, oCorr, nOuterCorr, corr, nCorr, cumulativeContErr ) :
closedVolume = p_rgh.needReference()
compressibility = ref.fvc.domainIntegrate( psi )
compressible = ( compressibility.value() > ref.SMALL )
rho << thermo.rho()
rUA = 1.0 / UEqn.A()
rhorUAf = ref.surfaceScalarField( ref.word( "(rho*(1|A(U)))" ) , ref.fvc.interpolate( rho * rUA ) )
U << rUA * UEqn.H()
phiU = ( ref.fvc.interpolate( rho ) *
( ( ref.fvc.interpolate( U ) & mesh.Sf() ) +
ref.fvc.ddtPhiCorr( rUA, rho, U, phi ) ) )
phi << phiU - rhorUAf * ghf * ref.fvc.snGrad( rho ) * mesh.magSf()
p_rghDDtEqn = ref.fvc.ddt( rho ) + psi * ref.correction( ref.fvm.ddt( p_rgh ) ) + ref.fvc.div( phi )
# Thermodynamic density needs to be updated by psi*d(p) after the
# pressure solution - done in 2 parts. Part 1:
thermo.rho() << thermo.rho() - psi * p_rgh
for nonOrth in range ( nNonOrthCorr + 1 ):
p_rghEqn = p_rghDDtEqn - ref.fvm.laplacian( rhorUAf, p_rgh )
p_rghEqn.solve( mesh.solver( p_rgh.select( ( oCorr == nOuterCorr-1 and corr == nCorr-1 and nonOrth == nNonOrthCorr ) ) ) )
if nonOrth == nNonOrthCorr :
phi += p_rghEqn.flux()
pass
pass
# Second part of thermodynamic density update
thermo.rho() << thermo.rho() + psi * p_rgh
# Correct velocity field
U += rUA * ref.fvc.reconstruct( ( phi() - phiU ) / rhorUAf ) # mixed calculations
U.correctBoundaryConditions()
p << p_rgh + rho * gh
#Update pressure substantive derivative
DpDt << ref.fvc.DDt( ref.surfaceScalarField( ref.word( "phiU" ), phi() / ref.fvc.interpolate( rho ) ), p ) # mixed calculations
# Solve continuity
ref.rhoEqn( rho, phi )
# Update continuity errors
cumulativeContErr = compressibleContinuityErrors( i, mesh, rho, thermo, cumulativeContErr )
# For closed-volume cases adjust the pressure and density levels
# to obey overall mass continuity
if closedVolume and compressible:
p += ( initialMass - ref.fvc.domainIntegrate( thermo.rho() ) ) / compressibility
rho << thermo.rho()
p_rgh << p - rho * gh()
pass
#Update thermal conductivity
K << thermoFluid[ i ].Cp() * turb.alphaEff()
return cumulativeContErr
def fun_pEqn( i, mesh, p, rho, turb, thermo, thermoFluid, K, UEqn, U, phi, psi, DpDt, initialMass, p_rgh, gh, ghf, \
nNonOrthCorr, oCorr, nOuterCorr, corr, nCorr, cumulativeContErr ) :
closedVolume = p_rgh.needReference()
compressibility = ref.fvc.domainIntegrate(psi)
compressible = (compressibility.value() > ref.SMALL)
rho << thermo.rho()
rUA = 1.0 / UEqn.A()
rhorUAf = ref.surfaceScalarField(ref.word("(rho*(1|A(U)))"),
ref.fvc.interpolate(rho * rUA))
U << rUA * UEqn.H()
phiU = (ref.fvc.interpolate(rho) * ((ref.fvc.interpolate(U) & mesh.Sf()) +
ref.fvc.ddtPhiCorr(rUA, rho, U, phi)))
phi << phiU - rhorUAf * ghf * ref.fvc.snGrad(rho) * mesh.magSf()
p_rghDDtEqn = ref.fvc.ddt(rho) + psi * ref.correction(
ref.fvm.ddt(p_rgh)) + ref.fvc.div(phi)
# Thermodynamic density needs to be updated by psi*d(p) after the
# pressure solution - done in 2 parts. Part 1:
thermo.rho() << thermo.rho() - psi * p_rgh
for nonOrth in range(nNonOrthCorr + 1):
p_rghEqn = p_rghDDtEqn - ref.fvm.laplacian(rhorUAf, p_rgh)
p_rghEqn.solve(
mesh.solver(
p_rgh.select((oCorr == nOuterCorr - 1 and corr == nCorr - 1
and nonOrth == nNonOrthCorr))))
if nonOrth == nNonOrthCorr:
phi += p_rghEqn.flux()
pass
pass
# Second part of thermodynamic density update
thermo.rho() << thermo.rho() + psi * p_rgh
# Correct velocity field
U += rUA * ref.fvc.reconstruct(
(phi() - phiU) / rhorUAf) # mixed calculations
U.correctBoundaryConditions()
p << p_rgh + rho * gh
#Update pressure substantive derivative
DpDt << ref.fvc.DDt(
ref.surfaceScalarField(ref.word("phiU"),
phi() / ref.fvc.interpolate(rho)),
p) # mixed calculations
# Solve continuity
ref.rhoEqn(rho, phi)
# Update continuity errors
cumulativeContErr = compressibleContinuityErrors(i, mesh, rho, thermo,
cumulativeContErr)
# For closed-volume cases adjust the pressure and density levels
# to obey overall mass continuity
if closedVolume and compressible:
p += (initialMass -
ref.fvc.domainIntegrate(thermo.rho())) / compressibility
rho << thermo.rho()
p_rgh << p - rho * gh()
pass
#Update thermal conductivity
K << thermoFluid[i].Cp() * turb.alphaEff()
return cumulativeContErr