Dear friends,
Recently I write a Fortran code to implement the single component multiphase Shan-Chen model based on Mike Sukop’s book and code.However, I find it is not right.Could you help me to find the mistake?Thanks in advance and best regards.Thes code is as follow:
C A short and simple gravity-driven LBM solver based on the code snippets
C in Sukop and Thorne’s ‘Lattice Boltzmann Modeling’
C Note indexing differences between book’s C code and FORTRAN:
C C uses 0 for the first index value, while FORTRAN starts at one.
C Numerous changes are needed. In some places, we have just
C explicitly added one to the C index.
[code="fortran"]
parameter(ly=201,lx=201)
CHARACTER(len=10)::filename,form
integer is_solid_node(ly,lx)
real rho(ly,lx),f(ly,lx,9),ftemp(ly,lx,9),ex(9),ey(9),
+ u_x(ly,lx),u_y(ly,lx),x(ly,lx),y(ly,lx),feq(ly,lx,9),
+ psi(ly,lx)
tau = 1.
wm=1./9.
wd=1./36.
C Set solid nodes at walls on top and bottom
is_solid_node=0 !periodic boundary at all sides
C Set initial density
do j=1,ly
do i=1,lx
CALL random_number(t) ! random number between 0 and 1
rho(j,i)=200.0*t ! initial density at each node
f(j,i,1) = (4./9. )*rho(j,i)
f(j,i,2) = (1./9. )*rho(j,i)
f(j,i,3) = (1./9. )*rho(j,i)
f(j,i,4) = (1./9. )*rho(j,i)
f(j,i,5) = (1./9. )*rho(j,i)
f(j,i,6) = (1./36.)*rho(j,i)
f(j,i,7) = (1./36.)*rho(j,i)
f(j,i,8) = (1./36.)*rho(j,i)
f(j,i,9) = (1./36.)*rho(j,i)
enddo
enddo
C Define lattice velocity vectors
ex(0+1)= 0
ey(0+1)= 0
ex(1+1)= 1
ey(1+1)= 0
ex(2+1)= 0
ey(2+1)= 1
ex(3+1)=-1
ey(3+1)= 0
ex(4+1)= 0
ey(4+1)=-1
ex(5+1)= 1
ey(5+1)= 1
ex(6+1)=-1
ey(6+1)= 1
ex(7+1)=-1
ey(7+1)=-1
ex(8+1)= 1
ey(8+1)=-1
C Time loop
do is=0,300
C Computing macroscopic density, rho, and velocity, u=(ux,uy).
do j=1,ly
do i=1,lx
u_x(j,i) = 0.0
u_y(j,i) = 0.0
rho(j,i) = 0.0
if(is_solid_node(j,i).eq.0) then
do k=1,9
rho(j,i) = rho(j,i) + f(j,i,k)
u_x(j,i) = u_x(j,i) + ex(k)*f(j,i,k)
u_y(j,i) = u_y(j,i) + ey(k)*f(j,i,k)
enddo
u_x(j,i) = u_x(j,i)/rho(j,i)
u_y(j,i) = u_y(j,i)/rho(j,i)
psi(j,i)=4.0*exp(-200.0/rho(j,i)) ! interaction potential
endif
C Add space matricies for plotting
x(j,i)=i
y(j,i)=j
enddo
enddo
C Compute the equilibrium distribution function, feq.
f1=3.
f2=9./2.
f3=3./2.
do j=1,ly
do i=1,lx
!!!! periodic boundary at all sides
if(i.gt.1) then
in = i-1
else
in =lx
endif
if(i.lt.LX) then
ip = i+1
else
ip = 1
endif
if(j.gt.1) then
jn = j-1
else
jn = ly
endif
if(j.lt.ly) then
jp = j+1
else
jp = 1
endif
fx=0.0
fy=0.0
if(is_solid_node(j,i).eq.0) then
! compute the interaction force
fx=wm*(psi(j,ip)-psi(j,in))
fx=fx+wd*(psi(jp,ip)-psi(jp,in)-psi(jn,in)+psi(jn,ip) )
fy=wm*(psi(jp,i)-psi(jn,i))
fy=fy+wd*( psi(jp,ip)+psi(jp,in)-psi(jn,in)-psi(jn,ip) )
fx=120.*psi(j,i)*fx
fy=120.*psi(j,i)*fy
rt0 = (4./9. )*rho(j,i)
rt1 = (1./9. )*rho(j,i)
rt2 = (1./36.)*rho(j,i)
ueqxij = u_x(j,i)+tau*fx/rho(j,i) ! care about this place
ueqyij = u_y(j,i)+tau*fy/rho(j,i) ! care about this place
uxsq = ueqxij * ueqxij
uysq = ueqyij * ueqyij
uxuy5 = ueqxij + ueqyij
uxuy6 = -ueqxij + ueqyij
uxuy7 = -ueqxij -ueqyij
uxuy8 = ueqxij -ueqyij
usq = uxsq + uysq
feq(j,i,0+1) = rt0*(1. - f3*usq)
feq(j,i,1+1) = rt1*(1.+ f1*ueqxij+f2*uxsq - f3*usq)
feq(j,i,2+1) = rt1*(1.+ f1*ueqyij+f2*uysq - f3*usq)
feq(j,i,3+1) = rt1*(1.- f1*ueqxij+f2*uxsq - f3*usq)
feq(j,i,4+1) = rt1*(1.- f1*ueqyij+f2*uysq - f3*usq)
feq(j,i,5+1) = rt2*(1.+ f1*uxuy5 +f2*uxuy5*uxuy5-f3*usq)
feq(j,i,6+1) = rt2*(1.+ f1*uxuy6 +f2*uxuy6*uxuy6-f3*usq)
feq(j,i,7+1) = rt2*(1.+ f1*uxuy7 +f2*uxuy7*uxuy7-f3*usq)
feq(j,i,8+1) = rt2*(1.+ f1*uxuy8 +f2*uxuy8*uxuy8-f3*usq)
endif
enddo
enddo
C Collision step.
do j=1,ly
do i=1,lx
if(is_solid_node(j,i).eq.1) then
C Standard bounceback
temp= f(j,i,1+1)
f(j,i,1+1) = f(j,i,3+1)
f(j,i,3+1) = temp
temp= f(j,i,2+1)
f(j,i,2+1) = f(j,i,4+1)
f(j,i,4+1) = temp
temp= f(j,i,5+1)
f(j,i,5+1) = f(j,i,7+1)
f(j,i,7+1) = temp
temp= f(j,i,6+1)
f(j,i,6+1) = f(j,i,8+1)
f(j,i,8+1) = temp
else
C Regular collision
do k=1,9
f(j,i,k) = f(j,i,k)-( f(j,i,k) - feq(j,i,k))/tau
enddo
endif
enddo
enddo
C Streaming step; subtle changes to periodicity here due to indexing
do j=1,ly
if (j.gt.1) then
jn = j-1
else
jn = ly
endif
if (j.lt.ly) then
jp = j+1
else
jp = 1
endif
do i=1,lx
if (i.gt.1) then
in = i-1
else
in = lx
endif
if (i.lt.LX) then
ip = i+1
else
ip = 1
endif
ftemp(j,i,0+1) = f(j,i,0+1)
ftemp(j,ip,1+1) = f(j,i,1+1)
ftemp(jp,i,2+1) = f(j,i,2+1)
ftemp(j,in,3+1) = f(j,i,3+1)
ftemp(jn,i ,4+1) = f(j,i,4+1)
ftemp(jp,ip,5+1) = f(j,i,5+1)
ftemp(jp,in,6+1) = f(j,i,6+1)
ftemp(jn,in,7+1) = f(j,i,7+1)
ftemp(jn,ip,8+1) = f(j,i,8+1)
enddo
enddo
f=ftemp
!export the results
IF(MOD(is,1).EQ.0)THEN
write(,) “is=”,is
SELECT CASE (INT(is))
CASE(0:9)
WRITE(form,'(i1)') INT(is)
CASE(10:99)
WRITE(form,'(i2)') INT(is)
CASE(100:999)
WRITE(form,'(i3)') INT(is)
CASE(1000:9999)
WRITE(form,'(i4)') INT(is)
CASE(10000:99999)
WRITE(form,'(i5)') INT(is)
CASE(100000:999999)
WRITE(form,'(i6)') INT(is)
ENDSELECT
WRITE(filename,*) trim(form), ".dat"
open(unit=20,file=filename,status='unknown')
WRITE(20,*) 'variables = x, y, u, v,density '
WRITE(20,*) 'zone i=',lx,',j=',ly,' f=point'
do j=1,ly
do i=1,lx
write(20,*) x(j,i),y(j,i),u_x(j,i),u_y(j,i),rho(j,i)
a=a+rho(j,i)
enddo
enddo
close(20)
ENDIF
C End time loop
enddo
pause
end