SUBROUTINE STATE(ID,TE,ANE,Q) C C modified LTE Saha equations - possibly using C radiation temperatures after C Schaerer and Schmutz AA 288, 321, 1994 C INCLUDE 'PARAMS.FOR' INCLUDE 'WINCOM.FOR' common/moltst/pfmol(600,mdepth),anmol(600,mdepth), * pfato(100,mdepth),anato(100,mdepth), * pfion(100,mdepth),anion(100,mdepth) common/ioniz2/anion2(30,mdepth) dimension FFI(MION0) C Q=0. DO 50 I=1,NATOMS IF(LGR(I)) GO TO 50 ION=IONIZ(I) RQ=0. RS=1. T=TRAD(INPOT(I,1),ID) if(t.le.0.) t=te X=SQRT(T/ANE) XMX=2.145E4*SQRT(X) CALL PARTF(I,1,T,ANE,XMX,UM) PFSTD(1,I)=UM JMAX=1 DO J=2,ION J1=J-1 T=TRAD(INPOT(I,J),ID) if(t.le.0.) t=te TLN=LOG(T)*1.5 TK=BOLK*T THL=11605./T X=SQRT(T/ANE) XMX=2.145E4*SQRT(X) DCH=EH/XMX/XMX/TK DCHT=DCH*J1 FI=36.113+TLN-THL*ENEV(I,J1)+DCHT X=J XMAX=XMX*SQRT(X) CALL PARTF(I,J,T,ANE,XMAX,U) PFSTD(J,I)=U FI=EXP(FI)*U/UM/ANE FFI(J)=FI IF(FFI(J).GT.1.) JMAX=J UM=U END DO IF(JMAX.LT.ION) THEN R=1. RQ=JMAX-1 DO J=JMAX+1,ION R=R*FFI(J) RR(I,J)=R/PFSTD(J,I) RS=RS+R RQ=RQ+(J-1)*R END DO END IF IF(JMAX.GT.1) THEN R=1. DO JJ=1,JMAX-1 J=JMAX-JJ R=R/FFI(J+1) RR(I,J)=R/PFSTD(J,I) RS=RS+R RQ=RQ+(J-1)*R END DO END IF ABND(I)=ABNDD(I,ID) RR(I,JMAX)=ABND(I)/RS DO J=1,ION IF(J.NE.JMAX) RR(I,J)=RR(I,J)*RR(I,JMAX) if(rr(i,j).lt.1.e-35) rr(i,j)=0. END DO RR(I,JMAX)=RR(I,JMAX)/PFSTD(JMAX,I) X=RQ/RS c IF(LRM(I)) GO TO 50 if(i.gt.1) Q=X*ABND(I)+Q anato(i,id)=rr(i,1)*pfstd(1,i) pfato(i,id)=pfstd(1,i) anion(i,id)=rr(i,2)*pfstd(2,i) pfion(i,id)=pfstd(2,i) 50 CONTINUE c do i=2,30 anion2(i,id)=rr(i,3)*pfstd(3,i) end do c do imol=1,500 anmol(imol,id)=0. pfmol(imol,id)=0. end do c RETURN END