383 lines
18 KiB
Fortran
383 lines
18 KiB
Fortran
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!
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!=======================================================================
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!
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MODULE CLASSICAL_FLUID
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!
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USE ACCURACY_REAL
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!
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!
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CONTAINS
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!
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!
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!=======================================================================
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!
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SUBROUTINE CFLUID_3D(R,N0,T,EPS,CF_TYPE,D,LAMBDA,ETA,ZETA)
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!
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! This subroutine computes the self-diffusion, thermal conductivity,
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! shear viscosity and bulk viscosity of a classical 3D fluid
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! composed of identical spheres.
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!
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! References: (1) O. Kravchenko and M. Thachuk, J. Chem. Phys. 136, 044520 (2012)
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! (2) K. M. Dyer, B. M. Pettitt and G. Stell, J. Chem. Phys. 126,
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! 034502 (2007)
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! (3) J.-M. Bomont and J.-L. Bretonnet, Chem. Phys. 439, 85-94 (2014)
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!
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!
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! Input parameters:
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!
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! * R : sphere's radius (SI)
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! * N0 : number density of spheres (SI)
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! * T : temperature (SI)
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! * EPS : depth of Lennard-Jones potential (SI)
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! * CF_TYPE : type of classical fluid calculation
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! CF_TYPE = 'SHS' smooth hard spheres
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! CF_TYPE = 'RH1' rough hard spheres (Pidduck)
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! CF_TYPE = 'RH2' rough hard spheres (Condiff-Lu-Dahler)
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! CF_TYPE = 'RH3' rough hard spheres (McCoy-Sandler-Dahler)
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! CF_TYPE = 'DCE' dilute Chapman-Enskog
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! CF_TYPE = 'HCE' heavy (i.e. dense) Chapman-Enskog
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! CF_TYPE = 'LJF' Lennard-Jones fluid
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!
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!
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! Note: The Lennard-Jones potential is written as
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!
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! _ _
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! | ( 2R )^12 ( 2R )^6 |
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! V(r) = 4*EPS * | ( ---- ) - ( ---- ) |
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! |_ ( r ) ( r ) _|
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!
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!
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! Output parameters:
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!
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! * D : (self-)diffusion coefficient
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! * LAMBDA : thermal conductivity
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! * ETA : shear viscosity
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! * ZETA : bulk viscosity
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!
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! Author : D. Sébilleau
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!
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! Last modified : 10 Jun 2020
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!
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!
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USE REAL_NUMBERS, ONLY : ZERO,ONE,TWO,THREE,FOUR,FIVE, &
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SIX,SEVEN,EIGHT,NINE,TEN, &
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HALF,THIRD
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USE CONSTANTS_P1, ONLY : M_E,K_B
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USE PI_ETC, ONLY : PI,PI_INV
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USE PACKING_FRACTION, ONLY : PACK_FRAC_3D
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!
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IMPLICIT NONE
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!
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CHARACTER (LEN = 3) :: CF_TYPE
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!
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REAL (WP) :: R,N0,T,EPS
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REAL (WP) :: D,LAMBDA,ETA,ZETA
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REAL (WP) :: SG,S2,S3,AL,AL2,AL3,AL4
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REAL (WP) :: DZ,L0,E0,Z0
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REAL (WP) :: K1,K2,NUM,DEN,C0,C1,C2
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REAL (WP) :: B,G,BRG,PF
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REAL (WP) :: TS,NS,Y,Z
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!
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SG=R+R ! particle diameter
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S2=SG*SG !
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S3=S2*SG !
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B=TWO*PI*SG*S2*THIRD ! 2nd virial coefficient
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AL=0.40E0_WP ! reduced moment of inertia
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! ! of sphere with uniform mass density
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AL2=AL*AL !
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AL3=AL2*AL !
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AL4=AL3*AL !
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!
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K1=DSQRT(K_B*T*PI_INV/M_E) !
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K2=DSQRT(K_B*T*PI_INV*M_E) !
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!
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! Computing the packing fraction
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!
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PF=PACK_FRAC_3D(N0,SG,'HSM') !
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!
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! Carnahan-Starling value of contact value of radial distribution
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!
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G=(ONE-HALF*PF) / (ONE-PF)**3 ! ref. 1 eq. (32)
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!
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BRG=B*N0*G
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!
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IF(CF_TYPE == 'SHS') THEN !
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!
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NUM=ONE+AL !
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DEN=ONE+AL+AL !
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D=THREE*K1/(EIGHT*N0*S2) ! ref. 1 eq. (17)
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!
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NUM=12.0E0_WP * (ONE+AL)**2 * ( & !
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37.0E0_WP + 151.0E0_WP*AL +& !
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50.0E0_WP*AL2 & !
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) !
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DEN=25.0E0_WP*( 12.0E0_WP + 75.0E0_WP*AL + & !
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101.0E0_WP*AL2 + 102.0E0_WP*AL3 & !
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) !
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LAMBDA=75.0E0_WP*K_B*K1/(64.0E0_WP*S2) ! ref. 1 eq. (18)
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!
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NUM=SIX*(ONE+AL)*(ONE+AL) !
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DEN=SIX+13.0E0_WP*AL !
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ETA=FIVE*K2/(16.0E0_WP*S2) ! ref. 1 eq. (19)
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!
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ZETA=ZERO !
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!
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ELSE IF(CF_TYPE == 'RH1') THEN !
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!
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NUM=ONE+AL !
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DEN=ONE+AL+AL !
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DZ=THREE*K1/(EIGHT*N0*S2) !
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D=DZ*NUM/DEN ! ref. 1 eq. (17)
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!
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NUM=12.0E0_WP * (ONE+AL)**2 * ( 37.0E0_WP + & !
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151.0E0_WP*AL + & !
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50.0E0_WP*AL2 & !
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) !
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DEN=25.0E0_WP*( 12.0E0_WP + 75.0E0_WP*AL + & !
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101.0E0_WP*AL2 + 102.0E0_WP*AL3 & !
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) !
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L0=75.0E0_WP*K_B*K1/(64.0E0_WP*S2) !
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LAMBDA=L0*NUM/DEN ! ref. 1 eq. (18)
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!
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NUM=SIX*(ONE+AL)*(ONE+AL) !
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DEN=SIX+13.0E0_WP*AL !
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E0=FIVE*K2/(16.0E0_WP*S2) !
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ETA=E0*NUM/DEN ! ref. 1 eq. (19)
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!
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NUM=(ONE+AL)*(ONE+AL) !
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DEN=AL !
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Z0=K2/(32.0E0_WP*S2) !
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ZETA=Z0*NUM/DEN ! ref. 1 eq. (20)
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!
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ELSE IF(CF_TYPE == 'RH2') THEN !
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!
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NUM=ONE+AL !
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DEN=ONE+AL+AL !
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DZ=THREE*K1/(EIGHT*N0*S2) !
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D=DZ*NUM/DEN !
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NUM=PI*AL*(ONE+AL) !
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DEN=TWO*(ONE+AL+AL)*(FIVE+NINE*AL+EIGHT*AL2) !
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D=D/(ONE + NUM/DEN) ! ref. 1 eq. (21)
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!
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NUM=FOUR*(ONE+AL)*( 1121.0E0_WP + 733.0E0_WP*AL + & !
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13449.0E0_WP*AL2 + 9490.0E0_WP*AL3 + & !
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2000.0E0_WP*AL4 & !
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) !
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DEN=25.0E0_WP*( 116.0E0_WP + 853.0E0_WP*AL + & !
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1707.0E0_WP*AL2 + 2266.0E0_WP*AL3 + & !
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1360.0E0_WP*AL4 & !
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) !
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L0=75.0E0_WP*K_B*K1/(64.0E0_WP*S2) !
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LAMBDA=L0*NUM/DEN ! ref. 1 eq. (22)
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!
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NUM=TWO*(ONE+AL)*(ONE+AL)*(THREE+TEN*AL) !
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DEN=SIX+33.0E0_WP*AL+35.0E0_WP*AL2 !
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E0=FIVE*K2/(16.0E0_WP*S2) !
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ETA=E0*NUM/DEN ! ref. 1 eq. (23)
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!
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NUM=(ONE+AL)*(ONE+AL) !
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DEN=AL !
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Z0=K2/(32.0E0_WP*S2) !
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ZETA=Z0*NUM/DEN ! ref. 1 eq. (20)
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!
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ELSE IF(CF_TYPE == 'RH3') THEN !
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!
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NUM=ONE+AL !
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DEN=ONE+AL+AL !
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DZ=THREE*K1/(EIGHT*N0*S2) !
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D=DZ*NUM/DEN !
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NUM=PI*AL*(ONE+AL) !
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DEN=TWO*(ONE+AL+AL)*(FIVE+NINE*AL+EIGHT*AL2) !
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D=D/(ONE + NUM/DEN) ! ref. 1 eq. (21)
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!
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NUM=FOUR*(ONE+AL)*( 1121.0E0_WP + 733.0E0_WP*AL + & !
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13449.0E0_WP*AL2 + 9490.0E0_WP*AL3 + & !
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2000.0E0_WP*AL4 & !
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) !
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DEN=25.0E0_WP*( 116.0E0_WP + 853.0E0_WP*AL + & !
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1707.0E0_WP*AL2 + 2266.0E0_WP*AL3 + & !
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1360.0E0_WP*AL4 & !
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) !
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L0=75.0E0_WP*K_B*K1/(64.0E0_WP*S2) !
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LAMBDA=L0*NUM/DEN ! ref. 1 eq. (22)
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!
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NUM=TWO*( 731.0E0_WP + 4958.0E0_WP*AL + 8005.0E0_WP*AL2 +& !
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5650.0E0_WP*AL3 + 2000.0E0_WP*AL4 & !
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) !
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DEN=1121.0E0_WP + 7336.0E0_WP*AL + 13449.0E0_WP*AL2 + & !
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9490.0E0_WP*AL3 + 2000.0E0_WP*AL4 !
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C1=NUM/DEN !
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!
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C0=501.0E0_WP + 3355.0E0_WP*AL + 4860.0E0_WP*AL2 + & !
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3850.0E0_WP*AL3 + 2000.0E0_WP*AL4 !
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NUM=16.0E0_WP*( 116.0E0_WP + 853.0E0_WP*AL + & !
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1707.0E0_WP*AL2 + 2266.0E0_WP*AL3 + & !
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1360.0E0_WP*AL4 & !
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) * PI_INV/(ONE+AL) !
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NUM=C0+NUM !
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C2=NUM/DEN !
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LAMBDA=LAMBDA/G * (ONE + C1*BRG + C2*BRG*BRG) ! ref. 1 eq. (29)
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!
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NUM=TWO*(ONE+AL)*(ONE+AL)*(THREE+TEN*AL) !
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DEN=SIX+33.0E0_WP*AL+35.0E0_WP*AL2 !
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E0=FIVE*K2/(16.0E0_WP*S2) !
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ETA=E0*NUM/DEN ! ref. 1 eq. (23)
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C1=0.40E0_WP*(TWO+FIVE*AL)/(ONE+AL) !
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NUM=SIX*( SIX + 33.0E0_WP*AL + 35.0E0_WP*AL2 & !
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) * (FOUR+SEVEN*AL) !
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DEN=PI*(THREE+TEN*AL)*(ONE+AL) !
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C2=( (TWO+FIVE*AL)**2 + NUM/DEN ) / (25.0E0_WP*(ONE+AL)**2) !
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ETA=ETA/G * (ONE + C1*BRG + C2*BRG*BRG) ! ref. 1 eq. (26)
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!
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NUM=(ONE+AL)*(ONE+AL) !
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DEN=AL !
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Z0=K2/(32.0E0_WP*S2) !
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ZETA=Z0*NUM/DEN ! ref. 1 eq. (20)
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C1=TWO !
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C2=ONE + 32.0E0_WP*AL/(PI*(ONE+AL)**2) !
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ZETA=ZETA/G * (ONE + C1*BRG + C2*BRG*BRG) ! ref. 1 eq. (27)
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!
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ELSE IF(CF_TYPE == 'DCE') THEN !
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!
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NUM=ONE+AL !
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DEN=ONE+AL+AL !
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D=1.019E0_WP*THREE*K1/(EIGHT*N0*S2) ! ref. 3 eq. (19)
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!
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NUM=12.0E0_WP * (ONE+AL)**2 * ( 37.0E0_WP + & !
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151.0E0_WP*AL + & !
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50.0E0_WP*AL2 & !
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) !
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DEN=25.0E0_WP*( 12.0E0_WP + 75.0E0_WP*AL + & !
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101.0E0_WP*AL2 + 102.0E0_WP*AL3 & !
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) !
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LAMBDA=1.025E0_WP*75.0E0_WP*K_B*K1/(64.0E0_WP*S2) ! ref. 3 eq. (21)
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!
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NUM=SIX*(ONE+AL)*(ONE+AL) !
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DEN=SIX+13.0E0_WP*AL !
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ETA=1.016E0_WP*FIVE*K2/(16.0E0_WP*S2) ! ref. 3 eq. (20)
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!
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ZETA=ZERO !
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!
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ELSE IF(CF_TYPE == 'HCE') THEN !
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!
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Z=FOUR*PF*G ! ref. 3 eq. (4)
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!
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NUM=ONE+AL !
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DEN=ONE+AL+AL !
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D=1.019E0_WP*THREE*K1/(EIGHT*N0*S2) !
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D=D*FOUR*PF/Z ! ref. 3 eq. (15)
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!
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NUM=12.0E0_WP * (ONE+AL)**2 * ( 37.0E0_WP + & !
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151.0E0_WP*AL + & !
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50.0E0_WP*AL2 & !
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) !
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DEN=25.0E0_WP*( 12.0E0_WP + 75.0E0_WP*AL + & !
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101.0E0_WP*AL2 + 102.0E0_WP*AL3 & !
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) !
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LAMBDA=1.025E0_WP*75.0E0_WP*K_B*K1/(64.0E0_WP*S2) !
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LAMBDA=LAMBDA*FOUR*PF*(ONE/Z + 1.2E0_WP + 0.755E0_WP*Z) ! ref. 3 eq. (18)
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!
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NUM=SIX*(ONE+AL)*(ONE+AL) !
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DEN=SIX+13.0E0_WP*AL !
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ETA=1.016E0_WP*FIVE*K2/(16.0E0_WP*S2) !
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ETA=ETA*FOUR*PF*(ONE/Z + 0.8E0_WP + 0.761E0_WP*Z) ! ref. 3 eq. (16)
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!
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ZETA=ETA*FOUR*PF*1.002E0_WP*Z ! ref. 3 eq. (17)
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!
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ELSE IF(CF_TYPE == 'LJF') THEN !
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!
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TS=K_B*T/EPS ! T*
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NS=N0*S3 ! rho*
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Y=TWO*PI*NS*THIRD !
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!
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DZ=0.375E0_WP*DSQRT(TS*PI_INV/M_E)/SG !
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D=DZ/(NS*G) ! ref. 2 eq. (3)
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!
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LAMBDA=ZERO ! not provided
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!
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E0=0.3125E0_WP*DSQRT(M_E*TS*PI_INV)/S2 !
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ETA=E0*(ONE/G + 0.8E0_WP*Y + 0.761E0_WP*Y*Y*G) ! ref. 2 eq. (4)
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!
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ZETA=E0*1.002E0_WP*Y*Y*G !
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||
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|
!
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||
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|
END IF !
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||
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|
!
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||
|
|
END SUBROUTINE CFLUID_3D
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||
|
|
!
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||
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|
!=======================================================================
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!
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||
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|
SUBROUTINE CFLUID_2D(R,N0,T,CF_TYPE,D,LAMBDA,ETA,ZETA)
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|
!
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||
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|
! This subroutine computes the self-diffusion, thermal conductivity,
|
||
|
|
! shear viscosity and bulk viscosity of a classical 2D fluid
|
||
|
|
! composed of identical spheres.
|
||
|
|
!
|
||
|
|
! References: (1) R. Garcia-Rojo, S. Luding and J. J. Brey,
|
||
|
|
! Phys. Rev. E 74, 061395 (2006)
|
||
|
|
!
|
||
|
|
!
|
||
|
|
! Input parameters:
|
||
|
|
!
|
||
|
|
! * R : disks radius (SI)
|
||
|
|
! * N0 : number density of spheres (SI)
|
||
|
|
! * T : temperature (SI)
|
||
|
|
! * CF_TYPE : type of classical fluid calculation
|
||
|
|
! CF_TYPE = 'DHD' dense hard disks
|
||
|
|
!
|
||
|
|
!
|
||
|
|
! Output parameters:
|
||
|
|
!
|
||
|
|
! * D : (self-)diffusion coefficient
|
||
|
|
! * LAMBDA : thermal conductivity
|
||
|
|
! * ETA : shear viscosity
|
||
|
|
! * ZETA : bulk viscosity
|
||
|
|
!
|
||
|
|
! Author : D. Sébilleau
|
||
|
|
!
|
||
|
|
! Last modified : 10 Jun 2020
|
||
|
|
!
|
||
|
|
!
|
||
|
|
USE REAL_NUMBERS, ONLY : ONE,TWO,THREE,FOUR,SEVEN, &
|
||
|
|
EIGHT,NINE,HALF
|
||
|
|
USE CONSTANTS_P1, ONLY : M_E,K_B
|
||
|
|
USE PI_ETC, ONLY : PI_INV
|
||
|
|
USE PACKING_FRACTION, ONLY : PACK_FRAC_2D
|
||
|
|
!
|
||
|
|
IMPLICIT NONE
|
||
|
|
!
|
||
|
|
CHARACTER*3 CF_TYPE
|
||
|
|
!
|
||
|
|
REAL (WP) :: R,N0,T
|
||
|
|
REAL (WP) :: K1,K2,SG,PF,G
|
||
|
|
REAL (WP) :: D,LAMBDA,ETA,ZETA
|
||
|
|
!
|
||
|
|
K1=DSQRT(K_B*T*PI_INV/M_E) !
|
||
|
|
K2=DSQRT(K_B*T*PI_INV*M_E) !
|
||
|
|
!
|
||
|
|
SG=R+R ! particle diameter
|
||
|
|
!
|
||
|
|
! Computing the packing fraction
|
||
|
|
!
|
||
|
|
PF=PACK_FRAC_2D(N0,SG,'HDM') !
|
||
|
|
!
|
||
|
|
! Henderson's value of contact value of radial distribution
|
||
|
|
!
|
||
|
|
G=(ONE -SEVEN*PF/16.0E0_WP) / (ONE-PF)**2 ! ref. 1 eq. (6)
|
||
|
|
!
|
||
|
|
IF(CF_TYPE == 'DHD') THEN !
|
||
|
|
D=HALF*K1 / (N0*SG*G) ! ref. 1 eq. (5)
|
||
|
|
LAMBDA=TWO*K_B*K1* ( &!
|
||
|
|
ONE/G + THREE*PF + &!
|
||
|
|
(NINE/FOUR + FOUR*PI_INV)*G*PF*PF &! ref. 1 eq. (24)
|
||
|
|
) / SG !
|
||
|
|
ETA=HALF*K2* ( &!
|
||
|
|
ONE/G + TWO*PF + &!
|
||
|
|
(ONE+EIGHT*PI_INV)*G*PF*PF &! ref. 1 eq. (15)
|
||
|
|
) / SG !
|
||
|
|
ZETA=EIGHT*K2*PF*PF*G*PI_INV/SG ! ref. 1 eq. (22)
|
||
|
|
END IF !
|
||
|
|
!
|
||
|
|
END SUBROUTINE CFLUID_2D
|
||
|
|
!
|
||
|
|
END MODULE CLASSICAL_FLUID
|