PHOTON USE p;;;;; up 1 0 0;vi 0.5 1 0.75 gr ou x 1;gr ou y 1;gr ou z 1 gr ou x m;gr ou y m;gr ou z m gr ou x 1 y 1 2 z 2 2 col 2 gr ou x 6 y 1 2 z 7 7 col 2 gr ou z 4 x 1 4 y 1 3 col 6 gr ou z 6 x 2 5 y 1 3 col 6 ve y 2 sh msg 3D SHELL-AND-TUBE HEAT EXCHANGER msg -------------------------------- msg Velocity 1 phase: msg Press Enter to continue pause;vi 0 1 0 msg 3D SHELL-AND-TUBE HEAT EXCHANGER msg -------------------------------- msg Temperature distribution 1 phase: con 1sth y 2 sh;in 50 msg Press Enter to continue pause con off;red msg 3D SHELL-AND-TUBE HEAT EXCHANGER msg -------------------------------- msg Temperature distribution 2 phase: con 2ndh y 2 sh;in 50 msg Press e to END ENDUSE GROUP 1. Run title TEXT(3D SHELL-AND-TUBE HEAT EXCHANGER:110 DISPLAY The heat exchanger considered has two baffles within the shell and the tubes arranged in five passes. The overall heat transfer coefficient depends on the local velocity and is introduced by PLANT. ===================== ENDDIS REAL(T1IN,T2IN,FLO1,FLO2,COEF1,COEF2,COEF12) Here 1 refers to the shell-side fluid and 2 to the tube-side fluid The units are arbitrary T1IN=1.0; T2IN=0.0 ! temperatures FLO1=0.1; FLO2=0.1 ! flow rates COEF1=0.1; COEF2=0.4 ! heat-transfer coefficients COEF12=1.0/(1.0/COEF1+1.0/COEF2) RG(1)=COEF12 ! overall coefficient, transmitted via RG(1) REAL(RESCO);RESCO=1.E2 ! tube-bank flow-resistance coefficient GROUP 3. X-direction grid specification The heat exchanger is a rectangular box, 1m high, 1m wide and 4m long. A uniform 5*3*8 grid is used, as was done by Patankar and Spalding in the first-ever heat-exchanger simulation [ Afghan & Schluender (Eds), 'Heat Exchangers', Scripta Book Company, 1974]. The example is chosen only because of its historical interest; for the 5-pass flow pattern does not make it a good heat exchanger. Only one half of the exchanger is included in the calculation domain, because of symmetry. The shell-side flow pattern, and the temperature fields of both fluids, are 3D because the shell-fluid inlet and outlet do not cover the whole dise area. GRDPWR(X,5,1.0,1.0) GROUP 4. Y-direction grid specification GRDPWR(Y,3,0.5,1.0) ! half-width is 0.5 m GROUP 5. Z-direction grid specification GRDPWR(Z,8,4.0,1.0) GROUP 7. Variables stored, solved & named The shell-side fluid is a single-phase one, for which the folowing five variables must be solved; only the enthalpy needs to be computed for the tube-side fluid, because its flow pattern is prescribed. SOLVE(P1,U1,V1,W1,H1,H2) NAME(H1)=1STH;NAME(H2)=2NDH ! names signify first- and second- ! fluid enthalpy STORE(EPOR,NPOR,HPOR) GROUP 8. Terms (in differential equations) & devices The "diffusion" terms are cut out for all vaiables, and the built-in sources for the enthalpies. TERMS(U1,Y,Y,N,Y,Y,Y);TERMS(V1,Y,Y,N,Y,Y,Y) TERMS(W1,Y,Y,N,Y,Y,Y);TERMS(1STH,N,Y,N,Y,Y,Y) TERMS(2NDH,N,N,N,Y,N,N) GROUP 11. Initialization of variable or porosity fields FIINIT(W1)=FLO1;FIINIT(U1)=0.0;FIINIT(V1)=0.0 FIINIT(1STH)=T1IN;FIINIT(2NDH)=T2IN FIINIT(EPOR)=0.5;FIINIT(NPOR)=0.5;FIINIT(HPOR)=0.5 GROUP 13. Boundary conditions and special sources West boundary; shell fluid inlet ; 2 cells in west wall PATCH(SHELLIN,CELL,1,1,2,3,2,2,1,1000) ! small patch in west wall COVAL(SHELLIN,P1,FIXFLU,FLO1/2.0); COVAL(SHELLIN,1STH,ONLYMS,T1IN) East boundary; shell fluid outlet; 2 cells in east wall PATCH(SHELLOUT,EAST,NX,NX,2,3,NZ-1,NZ-1,1,1000) ! patch in east wall COVAL(SHELLOUT,P1,FIXP,0.0) High boundary, tube fluid inlet; 5 cells in high wall PATCH(TUBEIN,CELL,1,1,1,NY,NZ,NZ,1,1000) ! IX=1; all IY; IZ=NZ COVAL(TUBEIN,2NDH,FLO2/3.0,T2IN) Note how the giving of special names to patches, beginning NE (for neighbour), coupled with LOCNE (GRND8) in the "value" location, produces sources which simulate along- the-tube convection fluid-to-metal heat transfer etc, by activating special calls to the built-in coding: gxnepat.for The flow pattern is: ---<-------------------------------------------- ^ --------------------------------------------! ^ !-------------------------------------------- ^ --------------------------------------------! ^ !--------------------------------------------<--- In the following COVALs, the /3.0 appears because there are 3 cells in the y-direction (NY=3) Flow of tube fluid in first pass <--- PATCH(NEH1,CELL,1,1,1,NY,1,NZ-1,1,1000) ! IX=1; all IY; IZ=1,NZ COVAL(NEH1,2NDH,FLO2/3.0,LOCNE) ! from higher-z neighbour Flow of tube fluid in first bend ^ PATCH(NEW1,CELL,2,2,1,NY,1,1,1,1000) ! IX=2; all IY; IZ=1 COVAL(NEW1,2NDH,FLO2/3.0,LOCNE) ! from lower-x neighbour Flow of tube fluid in second pass ---> PATCH(NEL1,CELL,2,2,1,NY,2,NZ,1,1000) ! IX=2; all IY; IZ=2,NZ COVAL(NEL1,2NDH,FLO2/3.0,LOCNE) ! from lower-z neighbour Flow of tube fluid in second bend ^ PATCH(NEW2,CELL,3,3,1,NY,NZ,NZ,1,1000) ! IX=3; all IY; IZ=NZ COVAL(NEW2,2NDH,FLO2/3.0,LOCNE) ! from lower-x neighbour Flow of tube fluid in third pass <--- PATCH(NEH2,CELL,3,3,1,NY,1,NZ-1,1,1000) ! IX=3; all IY; IZ=1,NZ-1 COVAL(NEH2,2NDH,FLO2/3.0,LOCNE) ! from higher-z neighbour Flow of tube fluid in third bend ^ PATCH(NEW3,CELL,4,4,1,NY,1,1,1,1000) ! IX=4; all IY; IZ=1 COVAL(NEW3,2NDH,FLO2/3.0,LOCNE) ! from lower-x neighbour Flow of tube fluid in fourth pass ---> PATCH(NEL2,CELL,4,4,1,NY,2,NZ,1,1000) ! IX=4; all IY; IZ=2,NZ COVAL(NEL2,2NDH,FLO2/3.0,LOCNE) ! from lower-z neighbour Flow of tube fluid in fourth bend ^ PATCH(NEW4,CELL,NX,NX,1,NY,NZ,NZ,1,1000) ! IX=5; all IY; IZ=NZ COVAL(NEW4,2NDH,FLO2/3.0,LOCNE) ! from lower-x neighbour Flow of tube fluid in fifth pass <--- PATCH(NEH3,CELL,NX,NX,1,NY,1,NZ-1,1,1000) ! IX=5; all IY; IZ=1,NZ-1 COVAL(NEH3,2NDH,FLO2/3.0,LOCNE) ! from higher-z neighbour PLANTBEGIN Heat-exchange with tube fluid, throughout the exchanger. PATCH(HEX,VOLUME,1,NX,1,NY,1,NZ,1,1000)CO=2.*(U1**2+V1**2+W1**2)**0.25 VAL=2NDH COVAL(HEX,1STH,GRND,GRND) Heat-exchange with shell fluid, throughout the exchanger. CO=2.*(U1**2+W1**2+V1**2)**0.25 VAL=1STH COVAL(HEX,2NDH,GRND,GRND) PLANTEND Baffle 1 at NZ=3 PATCH(BAFFLE1,HIGH,1,NX-1,1,NY,3,3,1,1000) COVAL(BAFFLE1,W1,FIXVAL,0.0) Baffle 2 at NZ=5 PATCH(BAFFLE2,HIGH,2,NX,1,NY,5,5,1,1000) COVAL(BAFFLE2,W1,FIXVAL,0.0) Resistance to flow exerted by tubes, throughout the shell. PATCH(RESIST,PHASEM,1,NX,1,NY,1,NZ,1,1000) COVAL(RESIST,U1,RESCO,0.0);COVAL(RESIST,V1,RESCO,0.0) COVAL(RESIST,W1,0.5*RESCO,0.0) GROUP 15. Termination of sweeps LSWEEP=100 GROUP 16. Termination of iterations LITER(P1)=100 GROUP 17. Under-relaxation devices RELAX(U1,FALSDT,1.0);RELAX(V1,FALSDT,1.0) RELAX(W1,FALSDT,1.0) RELAX(1STH,FALSDT,100.0);RELAX(2NDH,FALSDT,100.0) GROUP 19. Data communicated by satellite to GROUND NAMSAT=MOSG GROUP 20. Preliminary print-out GROUP 21. Print-out of variables Print-out of porosities is suppressed. OUTPUT(EPOR,N,N,N,N,N,N);OUTPUT(NPOR,N,N,N,N,N,N) OUTPUT(HPOR,N,N,N,N,N,N) OUTPUT(1STH,Y,N,Y,Y,Y,Y);OUTPUT(2NDH,Y,N,Y,Y,Y,Y) GROUP 22. Spot-value print-out IXMON=6;IYMON=6;TSTSWP=5 GROUP 23. Field print-out and plot control IPLTL=LSWEEP;IPROF=1;ORSIZ=0.4;XZPR=T;NPLT=1 PATCH(PASS1,PROFIL,1,1,2,2,1,NZ,1,1000) PLOT(PASS1,1STH,T2IN,T1IN);PLOT(PASS1,2NDH,T2IN,T1IN) PATCH(PASS2,PROFIL,2,2,2,2,1,NZ,1,1000) PLOT(PASS2,1STH,T2IN,T1IN);PLOT(PASS2,2NDH,T2IN,T1IN) PATCH(PASS3,PROFIL,3,3,2,2,1,NZ,1,1000) PLOT(PASS3,1STH,T2IN,T1IN);PLOT(PASS3,2NDH,T2IN,T1IN) PATCH(PASS4,PROFIL,4,4,2,2,1,NZ,1,1000) PLOT(PASS4,1STH,T2IN,T1IN);PLOT(PASS4,2NDH,T2IN,T1IN) tstswp=-1 dmpstk=t DISTIL=T EX(P1)=1.191E+02; EX(U1)=3.000E-01 EX(V1)=2.262E-02; EX(W1)=3.339E-01 EX(1STH)=4.835E-01; EX(2NDH)=4.681E-01 LIBREF=110 STOP