PHOTON USE
p
gr x 1
msg Grid
vec x 1 sh
MSG Velocity vectors
msg Press return to redraw
pause
gr cl; gr ou x 1; red
msg Press return to plot pressure contours
pause
cont p1 x 1 fil;.01
msg Type e to End
ENDUSE
GROUP 1. Run title
TEXT(External flow over a rocket: B529
TITLE
DISPLAY
This case represents supersonic flow along an axisymmetric
body of rotation whose axis is parallel to the free stream.
The grid is generated using transfinite interpolation.
Density is calculated from temperature assuming constant
stagnation enthalpy and is thus valid for adiabatic
non-isentropic flow.
ENDDIS
REAL(Z1,DZ1,DZ2,DZ3,RR1,RR2,RR3,RR4,PWRY,PZ1,PZ2,PZ3,PZ4,ZZ,HJ,DJ)
REAL(PZ5,STH,CTH,Z5)
INTEGER(K1,K2,K3,K4,KJ)
STH=0.2;CTH=(1.0-STH*STH)**0.5
REAL(GA,RGAS,AM,WMOL,DENS,RTEMP,CP,WVEL,COEF)
GROUP 6. Body-fitted coordinates or grid distortion
BFC=T;NONORT=T
GSET(D,1,14,39,1.0,2.0,4.0)
PWRY=1.7
PZ1=1.8;PZ2=1.5;PZ3=1.0;PZ4=1.0;PZ5=1.5
Z1 Z-coordinate of nose from start of domain
DZ1 Z-distance from nose to large end of first cone
DZ2 Length of second cone
DZ3 Length of third cone
RR1 Nose radius
RR2 Base radius of first cone
RR3 base radius of second cone
RR4 base radius of third cone and cylinder
Z1=0.5;DZ1=.2874;DZ2=0.9;DZ3=0.4;RR1=0.03;RR2=0.1;RR3=0.2;RR4=0.35
Z5=0.2271
** Coordinates of join between nose and first cone; from front
DJ=0.03
K1=8;K2=15;K3=23;K4=29;KJ=10
GSET(P,P0,0.0,0.0,0.0)
GSET(P,P5,0.0,0.0,Z5)
** Set nose position
GSET(P,P1,0.0,0.0,Z1)
** set join between nose and first cone
GSET(P,PJ,0.0,RR1,Z1+DJ)
ZZ=Z1+DZ1;GSET(P,P2,0.0,RR2,ZZ)
ZZ=ZZ+DZ2;GSET(P,P3,0.0,RR3,ZZ)
ZZ=ZZ+DZ3;GSET(P,P4,0.0,RR4,ZZ)
GSET(P,PN,0.0,RR4,ZWLAST)
** Set all points along south boundary
GSET(L,L05,P5,P0,2,:PZ1:)
GSET(L,L51,P1,P5,K1-3,:PZ1:)
GSET(P,P7,0.0,0.03*0.707,0.53-0.03*0.707)
GSET(L,L1J,P1,PJ,KJ-K1,1.0,ARC,P7)
GSET(L,LJ2,PJ,P2,K2-KJ,:PZ2:)
GSET(L,L23,P2,P3,K3-K2,:PZ3:)
GSET(L,L34,P3,P4,K4-K3,:PZ4:)
GSET(L,L4N,P4,PN,NZ+1-K4,:PZ5:)
** Set points along low and high boundaries
GSET(P,PA,0.0,YVLAST,0.0);GSET(P,PB,0.0,YVLAST,ZWLAST)
GSET(P,P6,0.0,YVLAST,Z5)
GSET(L,L0A,P0,PA,NY,:PWRY:);GSET(L,LNB,PN,PB,NY,:PWRY:)
GSET(L,LA6,P6,PA,2,:PZ1:);GSET(L,L6B,P6,PB,NZ-2,1.0)
GSET(L,L56,P5,P6,NY,:PWRY:)
GSET(F,F1,P0,-,PA,-,P6,-,P5,-)
GSET(M,F1,+J+K,1,1,1,TRANS)
GSET(F,F2,P5,-,P6,-,PB,-,PN,P4.P3.P2.PJ.P1)
GSET(M,F2,+J+K,1,1,3,LAP10.FFFTFT)
** Adjust near axis points at entry
GSET(T,J3,F,J1,1,1,1,2,1.0)
** Transform to 2D polar domain
GSET(C,I2,F,I1,1,NY,1,NZ,RZ,-0.2,0.0,0.0)
GROUP 7. Variables stored, solved & named
SOLVE(P1,V1,W1);SOLUTN(P1,Y,Y,Y,N,N,N);STORE(DEN1)
NCRT=2;STORE(VCRT,WCRT)
GROUP 9. Properties of the medium (or media)
** Ratio of specific heats
GA=1.4
** Gas constant
RGAS=8305.6
** Molecular weight
WMOL=29.
** Specific heat
CP=1000.
** Free-stream Mach number
AM=1.2
** F.s. static temperature
RTEMP=288.
** Datum pressure (free-stream)
PRESS0=1.E5
** Density from perfect gas law in GREX3
RHO1=IDEALGAS
** Local static temperature from GREX3
TMP1=CONSTAGH
** DRH1DP for compressible adiabatic flow.
DRH1DP=IDEALGAS; RHO1C=1./GA
** F.s. density
DENS=PRESS0*WMOL/(RGAS*RTEMP)
** Stagnation enthalpy
TMP1A=RTEMP*CP*(1.+(GA-1.)*AM*AM*.5)
CP1=CP
** Constant in ideal gas law
RHO1B=WMOL/RGAS; RHO1C=1./GA
** Free stream velocity
WVEL=AM*(GA*RGAS*RTEMP/WMOL)**.5
** Kinematic viscosity
ENUL=1.34E-5;ENUT=2.E-4
GROUP 11. Initialization of variable or porosity fields
FIINIT(W1)=WVEL;FIINIT(DEN1)=DENS
GROUP 13. Boundary conditions and special sources
** Small-wave theory b.c for supersonic flow
COEF=(AM*AM-1.)**.5/WVEL
PATCH(NB,NORTH,#1,#NREGX,#NREGY,#NREGY,#1,#NREGZ,1,1)
COVAL(NB,P1,COEF,0.0)
COVAL(NB,W1,ONLYMS,WVEL);COVAL(NB,V1,ONLYMS,SAME)
WALL (SB,SOUTH,#1,#NREGX,#1,#1,#3,#NREGZ,1,1)
INLET(BFCIN,LOW,#1,#NREGX,#1,#NREGY,#1,#1,1,1)
VALUE(BFCIN,P1,GRND1);VALUE(BFCIN,W1,GRND1)
VALUE(BFCIN,WCRT,WVEL)
* Transfer density for GXBFC subroutine
BFCA=DENS
PATCH(OUTLET,HIGH,#1,#NREGX,#1,#NREGY,#NREGZ,#NREGZ,1,1)
`Weak` exit boundary condition for supersonic flows.
This allows an oblique shock to cross the exit plane by permitting
a pressure gradient normal to the flow. This is done by making the
outflow from each cell at the exit boundary equal to that from its
low-z neighbour.
COVAL(OUTLET,P1,FIXFLU,GRND1)
COVAL(OUTLET,V1,ONLYMS,0.)
COVAL(OUTLET,W1,ONLYMS,WVEL)
GROUP 15. Termination of sweeps
LSWEEP=100
** At least 150 sweeps will be required for a converged solution.
GROUP 16. Termination of iterations
LITER(P1)=10;LITER(U1)=1;LITER(V1)=1;LITER(W1)=1
GROUP 17. Under-relaxation devices
RELAX(P1,LINRLX,.35)
RELAX(V1,FALSDT,.002)
RELAX(W1,FALSDT,.0005)
RELAX(DEN1,LINRLX,1.)
GROUP 19. Data communicated by satellite to GROUND
USEGRD=F
GROUP 21. Print-out of variables
OUTPUT(P1,Y,Y,Y,Y,Y,Y)
OUTPUT(DEN1,Y,N,N,N,N,N)
GROUP 22. Spot-value print-out
IXMON=1;IYMON=3;IZMON=28;TSTSWP=-1
SELREF=T; RESFAC=0.01
GROUP 23. Field print-out and plot control
NPRINT=LSWEEP;NYPRIN=1;NZPRIN=2
PATCH(YZ,CONTUR,1,1,1,NY,1,NZ,1,1)
PLOT(YZ,P1,0.0,20.0)