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authorstainer_t <thomas.stainer@oecd-nea.org>2025-09-08 13:48:49 +0200
committerstainer_t <thomas.stainer@oecd-nea.org>2025-09-08 13:48:49 +0200
commit7dfcc480ba1e19bd3232349fc733caef94034292 (patch)
tree03ee104eb8846d5cc1a981d267687a729185d3f3 /Dragon/src/SYB005.f
Initial commit from Polytechnique Montreal
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+*DECK SYB005
+ SUBROUTINE SYB005 (NGEN,NPIJ,NPIS,NRAYRE,SIGT2,SIGW2,IMPX,NCOUR,
+ 1 IQUAD,XX,YY,LSECT,NMC,NMCR,RAYRE,MAIL,IZMAIL,RZMAIL,PIJW,PISW,
+ 2 PSJW,PSSW)
+*
+*-----------------------------------------------------------------------
+*
+*Purpose:
+* Compute the cellwise scattering-reduced collision, escape and
+* transmission probabilities in a 2-D Cartesian or hexagonal assembly
+* with DP-1 approximation.
+*
+*Copyright:
+* Copyright (C) 2002 Ecole Polytechnique de Montreal
+* This library is free software; you can redistribute it and/or
+* modify it under the terms of the GNU Lesser General Public
+* License as published by the Free Software Foundation; either
+* version 2.1 of the License, or (at your option) any later version
+*
+*Author(s): A. Hebert
+*
+*Parameters: input
+* NGEN total number of generating cells.
+* NPIJ length of cellwise scattering-reduced collision probability
+* matrices.
+* NPIS length of cellwise scattering-reduced escape probability
+* matrices (NPIS=NMC(NGEN+1)).
+* NRAYRE size of array rayre (NRAYRE=NMCR(NGEN+1)).
+* SIGT2 total macroscopic cross sections.
+* SIGW2 P0 within-group scattering macroscopic cross sections.
+* IMPX print flag (equal to 0 for no print).
+* NCOUR number of currents surrounding the cells (=12 Cartesian
+* lattice; =18 hexagonal lattice).
+* IQUAD quadrature parameters.
+* XX X-thickness of the generating cells.
+* YY Y-thickness of the generating cells.
+* LSECT type of sectorization.
+* NMC offset of the first volume in each generating cell.
+* NMCR offset of the first radius in each generating cell.
+* RAYRE radius of the tubes in each generating cell.
+* MAIL offset of the first tracking information in each generating
+* cell.
+* IZMAIL integer tracking information.
+* RZMAIL real tracking information.
+*
+*Parameters: output
+* PIJW cellwise scattering-reduced collision probability matrices.
+* PISW cellwise scattering-reduced escape probability matrices.
+* PSJW cellwise scattering-reduced collision probability matrices
+* for incoming neutrons.
+* PSSW cellwise scattering-reduced transmission probability
+* matrices.
+*
+*-----------------------------------------------------------------------
+*
+*----
+* SUBROUTINE ARGUMENTS
+*----
+ INTEGER NGEN,NPIJ,NPIS,NRAYRE,IMPX,NCOUR,IQUAD(4),LSECT(NGEN),
+ 1 NMC(NGEN+1),NMCR(NGEN+1),MAIL(2,NGEN),IZMAIL(*)
+ REAL SIGT2(NPIS),SIGW2(NPIS),XX(NGEN),YY(NGEN),RAYRE(NRAYRE),
+ 1 RZMAIL(*),PIJW(NPIJ),PISW(NCOUR*NPIS),PSJW(NCOUR*NPIS),
+ 2 PSSW(NGEN*NCOUR*NCOUR)
+*----
+* LOCAL VARIABLES
+*----
+ PARAMETER (PI=3.141592654,SMALL=5.0E-3,SQRT3=1.732050807568877)
+ LOGICAL LSKIP
+ REAL PSS(324),SURFA(6),ALPA(64),PWA(64)
+ DOUBLE PRECISION PPP(16)
+ REAL, ALLOCATABLE, DIMENSION(:) :: VOL,WORK
+ REAL, ALLOCATABLE, DIMENSION(:,:) :: PIS,PSJ,PP
+*
+ IPIJ=0
+ IPIS=0
+ IPSS=0
+ DO 240 JKG=1,NGEN
+ J1=NMC(JKG)
+ J2=NMC(JKG+1)-J1
+ J1R=NMCR(JKG)
+ J2R=NMCR(JKG+1)-J1R
+ ALLOCATE(PIS(J2,NCOUR),PSJ(NCOUR,J2),PP(J2,J2),VOL(J2))
+*----
+* COMPUTE THE REDUCED COLLISION PROBABILITY MATRIX
+*----
+ A=XX(JKG)
+ B=YY(JKG)
+ IF((NCOUR.EQ.12).AND.(LSECT(JKG).NE.0)) THEN
+* SECTORIZED CARTESIAN CELL.
+ IB1=MAIL(1,JKG)
+ IB2=MAIL(2,JKG)
+ IF(LSECT(JKG).EQ.-999) THEN
+ NSECT=4
+ ELSE IF((LSECT(JKG).EQ.-1).OR.(LSECT(JKG).EQ.-101)) THEN
+ NSECT=8
+ ELSE
+ NSECT=4*MOD(ABS(LSECT(JKG)),100)
+ ENDIF
+ MNA4=4*IQUAD(1)
+ CALL SYB4QG(IMPX,3,MNA4,J2R,NSECT,LSECT(JKG),J2,RZMAIL(IB2),
+ 1 IZMAIL(IB1),A,B,RAYRE(J1R+2),SIGT2(J1+1),SMALL,VOL,PP,PIS,PSS)
+ ELSE IF(LSECT(JKG).NE.0) THEN
+* SECTORIZED HEXAGONAL CELL.
+ IB1=MAIL(1,JKG)
+ IB2=MAIL(2,JKG)
+ NSECT=6
+ MNA4=12*IQUAD(1)
+ CALL SYB7QG(IMPX,3,MNA4,J2R,NSECT,LSECT(JKG),J2,RZMAIL(IB2),
+ 1 IZMAIL(IB1),A,RAYRE(J1R+2),SIGT2(J1+1),SMALL,VOL,PP,PIS,PSS)
+ ELSE IF((NCOUR.EQ.12).AND.(J2.EQ.1)) THEN
+ CALL ALGPT(IQUAD(3),-1.0,1.0,ALPA,PWA)
+ CALL RECT2(IQUAD(3),A,B,SIGT2(J1+1),SMALL,PP,PIS,PSS,ALPA,PWA)
+ VOL(1)=A*B
+ ELSE IF(J2.EQ.1) THEN
+ CALL ALGPT(IQUAD(3),-1.0,1.0,ALPA,PWA)
+ CALL XHX2D1(IQUAD(3),ALPA,PWA,A,SIGT2(J1+1),SMALL,PP,PIS,PSS,
+ 1 PPP)
+ VOL(1)=1.5*SQRT3*A*A
+ ELSE
+* NON-SECTORIZED CARTESIAN OR HEXAGONAL CELL.
+ IB1=MAIL(1,JKG)
+ IB2=MAIL(2,JKG)
+ CALL SYBUP1(RZMAIL(IB2),IZMAIL(IB1),NCOUR/3,J2,SIGT2(J1+1),
+ 1 SMALL,A,B,IMPX,VOL,PP,PIS,PSS)
+ ENDIF
+*----
+* COMPUTE THE REDUCED COLLISION PROBABILITY MATRIX FOR INCOMING
+* NEUTRONS
+*----
+ DO 65 I=1,J2
+ IF(NCOUR.EQ.12) THEN
+ SURFA(1)=0.25*B
+ SURFA(2)=0.25*B
+ SURFA(3)=0.25*A
+ SURFA(4)=0.25*A
+ ELSE
+ DO 50 JC=1,6
+ SURFA(JC)=0.25*A
+ 50 CONTINUE
+ ENDIF
+ DO 60 JC=1,NCOUR
+ PSJ(JC,I)=PIS(I,JC)*VOL(I)/SURFA(1+(JC-1)/3)
+ 60 CONTINUE
+ 65 CONTINUE
+ DEALLOCATE(VOL)
+ IF(IMPX.GE.8) THEN
+ CALL SYBPRX(1,NCOUR,J2,JKG,SIGT2(J1+1),SIGW2(J1+1),PP(1,1),
+ 1 PIS(1,1),PSJ(1,1),PSS(1))
+ ENDIF
+*----
+* CHECK IF SCATTERING REDUCTION IS REQUIRED
+*----
+ LSKIP=.TRUE.
+ DO 70 I=1,J2
+ LSKIP=LSKIP.AND.(SIGW2(J1+I).EQ.0.0)
+ 70 CONTINUE
+*----
+* SCATTERING REDUCTION IF LSKIP=.FALSE.
+*----
+ IF(LSKIP) THEN
+* DO NOT PERFORM SCATTERING REDUCTION.
+ DO 85 I=1,J2
+ DO 80 J=1,J2
+ PIJW(IPIJ+(J-1)*J2+I)=PP(I,J)
+ 80 CONTINUE
+ 85 CONTINUE
+ DO 95 I=1,J2
+ DO 90 JC=1,NCOUR
+ PISW(IPIS+(JC-1)*J2+I)=PIS(I,JC)
+ PSJW(IPIS+(I-1)*NCOUR+JC)=PSJ(JC,I)
+ 90 CONTINUE
+ 95 CONTINUE
+ DO 105 IC=1,NCOUR
+ DO 100 JC=1,NCOUR
+ PSSW(IPSS+(JC-1)*NCOUR+IC)=PSS((JC-1)*NCOUR+IC)
+ 100 CONTINUE
+ 105 CONTINUE
+ ELSE
+* COMPUTE THE SCATTERING-REDUCED COLLISION AND ESCAPE MATRICES.
+ DO 120 I=1,J2
+ DO 110 J=1,J2
+ PIJW(IPIJ+(J-1)*J2+I)=-PP(I,J)*SIGW2(J1+J)
+ 110 CONTINUE
+ PIJW(IPIJ+(I-1)*J2+I)=1.0+PIJW(IPIJ+(I-1)*J2+I)
+ 120 CONTINUE
+ CALL ALINV(J2,PIJW(IPIJ+1),J2,IER)
+ IF(IER.NE.0) CALL XABORT('SYB005: SINGULAR MATRIX.')
+ ALLOCATE(WORK(J2))
+ DO 175 I=1,J2
+ DO 130 K=1,J2
+ WORK(K)=PIJW(IPIJ+(K-1)*J2+I)
+ 130 CONTINUE
+ DO 150 J=1,J2
+ WGAR=0.0
+ DO 140 K=1,J2
+ WGAR=WGAR+WORK(K)*PP(K,J)
+ 140 CONTINUE
+ PIJW(IPIJ+(J-1)*J2+I)=WGAR
+ 150 CONTINUE
+ DO 170 JC=1,NCOUR
+ WGAR=0.0
+ DO 160 K=1,J2
+ WGAR=WGAR+WORK(K)*PIS(K,JC)
+ 160 CONTINUE
+ PISW(IPIS+(JC-1)*J2+I)=WGAR
+ 170 CONTINUE
+ 175 CONTINUE
+ DEALLOCATE(WORK)
+*
+* COMPUTE THE SCATTERING-REDUCED COLLISION PROBABILITY MATRIX
+* FOR INCOMING NEUTRONS.
+ DO 200 IC=1,NCOUR
+ DO 190 J=1,J2
+ WGAR=PSJ(IC,J)
+ DO 180 K=1,J2
+ WGAR=WGAR+PSJ(IC,K)*SIGW2(J1+K)*PIJW(IPIJ+(J-1)*J2+K)
+ 180 CONTINUE
+ PSJW(IPIS+(J-1)*NCOUR+IC)=WGAR
+ 190 CONTINUE
+ 200 CONTINUE
+*
+* COMPUTE THE SCATTERING-REDUCED TRANSMISSION PROBABILITY MATRIX.
+ DO 230 IC=1,NCOUR
+ DO 220 JC=1,NCOUR
+ WGAR=PSS((JC-1)*NCOUR+IC)
+ DO 210 K=1,J2
+ WGAR=WGAR+PSJ(IC,K)*SIGW2(J1+K)*PISW(IPIS+(JC-1)*J2+K)
+ 210 CONTINUE
+ PSSW(IPSS+(JC-1)*NCOUR+IC)=WGAR
+ 220 CONTINUE
+ 230 CONTINUE
+ ENDIF
+ DEALLOCATE(PP,PSJ,PIS)
+ IF(IMPX.GE.10) THEN
+ CALL SYBPRX(2,NCOUR,J2,JKG,SIGT2(J1+1),SIGW2(J1+1),PIJW(IPIJ+1),
+ 1 PISW(IPIS+1),PSJW(IPIS+1),PSSW(IPSS+1))
+ ENDIF
+ IPIJ=IPIJ+J2*J2
+ IPIS=IPIS+J2*NCOUR
+ IPSS=IPSS+NCOUR*NCOUR
+ 240 CONTINUE
+ RETURN
+ END