/** # The GABLS2 case using a fixed and equidistant grid approach comments will follow. Look [here](GABLS2.c). */ #include "grid/multigrid1D.h" #include "diffusion.h" #include "run.h" #define T1bottom (((((-25*cos(0.22*((t/3600)+16.) + 0.2)-10.) *(((t/3600.)+16.)<=17.4))+((((t/3600.)+16.)<=30.)*(((t/3600.)+16.)>17.4)*((-0.54*((t/3600.)+16.))+15.2))+((((t/3600.)+16.)<=41.9)*(((t/3600.)+16.)>30)*(-7-(25*cos(0.21*((t/3600.)+16.)+1.8))))+((((t/3600.)+16.)<=53.3)*(((t/3600.)+16.)>41.9)*(-0.37*((t/3600.)+16.)+18.0))+((((t/3600.)+16.)<=65.6)*(((t/3600.)+16.)>53.3)*(-4-25*cos(0.22*((t/3600.)+16.)+2.5)))+((((t/3600.)+16.)>65.6)*(4.4)))+273.15)) #define maxlevel 9 // Holtslag and Boville with Stable F(Ri) according to vdW #define fris(Ri) (sq((1-(Ri/0.20)))*(Ri<0.20)) //vdW 2017 Critical Ri //#define fris(x) (1/(1+(10*x*(1+8*x)))) #define friu(Ri) (sqrt(1-(18.*Ri))) // Holtslag en Boville 1992 #define friubm(Ri,y) ((1-((10*Ri)/(1+75*y*sqrt((x+zo/zo)*fabs(Ri)))))) // Louis 1982 #define friubh(Ri,y) ((1-((15*Ri)/(1+75*y*sqrt((x+zo/zo)*fabs(Ri)))))) // louis 1982 int nn; double Tref=283.15; double Ugeo=-8.; double Vgeo = 3.; double He= 65.6; double Rv= 461.5; double Rd = 287.; double L= 2500000.; double cpd= 1004; double exner; double Up[100]; double Cm,Ch,Cq,qtsat,TK1; double zo=0.01; scalar u[],v[],T1[],qt[]; scalar * tracers = {u,v,T1,qt}; mgstats mgb; int m = 0; double eu=0.; double eb=0.; int main(){ init_grid(1<<(maxlevel)); L0=4096; X0=0; run(); } u[left]=dirichlet(0.); v[left]=dirichlet(0.); T1[left]=dirichlet(T1bottom); T1[right]=neumann((20./3000.)); event init(i=0){ exner = pow(972./1000.,Rd/cpd); TOLERANCE=10E-8; DT=1; foreach(){ u[]=Ugeo; v[]=Vgeo; T1[]=(((x<=200))*(288-(2*x/200)))+ ((x>200)*(x<=850)*286)+ ((x>850)*(x<=900)*(286+2*(x-850)/50))+ ((x>900)*(x<=1000)*(288+4*(x-900)/100))+ ((x>1000)*(292+20*((x-1000)/3000))); qt[]=0.0025; } } event Diffusion(i++){ boundary({u,v,T1,qt}); nn=0; scalar rx[],ry[],rT1[],T1f[],rqt[],b[],w[]; face vector kh[],sqd[],Ri[],fRi[]; double CN,U,bbottom,es,qsl; foreach() b[]=((T1[]-Tref)*(9.81/Tref))*(1+(0.608*qt[])); foreach(){ w[]=-0.005*(((x/1000)*(x<=1000))+(x>1000))*(((t/3600)+16-24)>=24); rx[]=0.000139*(v[]-Vgeo); rx[]-=w[]*((u[1]-u[-1])/(2*Delta)); rT1[]=-w[]*((T1[1]-T1[-1])/(2*Delta)); ry[]=0.000139*(Ugeo-u[]); ry[]-=w[]*((v[1]-v[-1])/(2*Delta)); rqt[]=-w[]*((qt[1]-qt[-1])/(2*Delta)); if (xbbottom){ Cm=CN*fris(((x-zo)*(b[]-(bbottom))/(sq(u[])+sq(v[])))); Ch=Cm; Cq=Cm*0.025; } else{ CN = sq(0.4/log((x)/zo)); Cm = CN*friubm((x-zo)*(b[]-(bbottom))/(sq(u[])+sq(v[])),CN); Ch = CN*friubh((x-zo)*(b[]-(bbottom))/(sq(u[])+sq(v[])),CN); Cq = Ch*0.025; } U=sqrt(sq(u[])+sq(v[])); rx[]-=(u[]*Cm*U)/Delta; ry[]-=(v[]*Cm*U)/Delta; rT1[]-=((T1[]-T1bottom)*Cm*U)/Delta; rqt[]-=((qt[]-qtsat)*Cq*U)/Delta; } } boundary(all); foreach_face()//Compute turbulent diffusivities { sqd.x[]=(sq((u[]-u[-1])/(Delta))+sq((v[]-v[-1])/(Delta))); Ri.x[]= ((b[]-b[-1])/(Delta))/(sqd.x[]+0.00001); if (Ri.x[]<0) fRi.x[]=friu(Ri.x[]); else fRi.x[]=fris(Ri.x[]); kh.x[]=sq(min(0.4*x,70))*(sqrt(sqd.x[]))*fRi.x[]; } boundary({kh.x}); dt=dtnext(DT); // Log total number of Multigrid Cycles mgb=diffusion(u,dt,kh,rx); nn+=mgb.i; mgb=diffusion(v,dt,kh,ry); nn+=mgb.i; mgb=diffusion(T1,dt,kh,rT1); nn+=mgb.i; mgb=diffusion(qt,dt,kh,rqt); nn+=mgb.i; } event output(t+=360){ scalar U[]; int ng=0; foreach(){ U[]=sqrt(sq(u[])+sq(v[])); ng++; } boundary({U}); static FILE * fp4 = fopen("datogablsfg.dat","w"); fprintf(fp4,"%g\t%g\t%d\t%g\t%d\t%g\t%g\n",t,dt,i,interpolate(U,10),ng,qtsat,TK1); fflush(fp4); fprintf(stdout,"%g\t%g\t%d\t%g\t%d\t%g\t%g\n",t,dt,i,interpolate(U,10),ng,qtsat,TK1); static FILE * fp = fopen("prfilesGABLS2fg.dat","w"); double yp=0; while (yp14) DT=max(DT/(1+((double)nn/10.)),2.); if (nn<8) DT=min(DT*(1+((double)nn/100.)),15.); }