{************************************************************************** * L O R E N T Z A T T R A C T O R * * ----------------------------------------------------------------------- * * TUTORIAL: * * * * Until recently, the only known attractors were the fixed point, the * * limit cycle and the torus. In 1963, Edwards Lorenz, meteorologist at the* * M.I.T.,discovered a practical example of a simple dynamic system presen-* * ting a complex behaviour. To adapt them to computers available at that * * time, he began with simplifying the equations of metéorology to obtain * * finally a model composed of three differential equations with three * * unknown variables x, y, z and three parameters a, b, c: * * * * dx / dt = - a x + a y * * dy / dt = b x - y - x z * * dz / dt = -c z + x y * * * * During very long simulations on a computer, Lorentz decided, to check a * * result, to restart the same calculation halfway in order to spare time. * * For that, he reinjected into the computer the intermediate date obtained* * earlier. He was very surprised to see that the new results were comple- * * tely different from the first ones. After he suspected some computer * * failure, Lorenz understood at last that the big difference between both * * solutions came from very small differences in data. These small pertur- * * bations exponentially amplified themselves, being doubled every four * * days in simulated time, so after two months the results became entirely * * different ! * * * * Lorenz then realized that it would be very difficult to make meteorolo- * * gical foresights in the long term, the slightest change in initial con- * * ditions leading to a radically different evolution of atmosphere. * * * * This is still the case today with atmospheric models much more sophis- * * ticated. * * * * None of the three attractors known at the time could predict the beha- * * viour of such a dynamic system. Lorenz had just discovered a strange or * * "chaotic" attractor to which his name was given. * * ----------------------------------------------------------------------- * * REFERENCE: * * "Graphisme dans le plan et dans l'espace avec Turbo Pascal 4.0 * * By R. Dony - MASSON, Paris 1990" [BIBLI 12]. * * * * TPW version by J-P Moreau * * (www.jpmoreau.fr) * **************************************************************************} Program Lorentz_Attractor; Uses WinCrtMy,WinTypes,WinProcs,Type_def,CrtGr2D; VAR A,B,C,x,y,z : REAL_AR; CrtPen : HPEN; Procedure Lorentz; Procedure f; Const delta = 0.01; Var dx,dy,dz: REAL_AR; begin dx:=A*(y-x); dy:=x*(B-z)-y; dz:=x*y-C*z; x:=x+delta*dx; y:=y+delta*dy; z:=z+delta*dz end; Begin f; MoveXY(CrtDc,1+x,z); Repeat f; LineXY(CrtDc,1+x,z) Until KeyPressed; gotoxy(50,26); write('LORENTZ ATTRACTOR'); End; {main program} BEGIN WinCrtInit('LORENTZ ATTRACTOR'); CrtPen:=CreatePen(ps_Solid,1,RGB(0,0,255)); SelectObject(CrtDC,CrtPen); A:=10; B:=30; C:=2.6666; x:=1; y:=1; z:=1; Fenetre(-22,25,-8,60); Cloture(15,MaxX-25,80,MaxY-15); Repeat clrscr; Bordure(CrtDc); Lorentz; SortieGraphique; Until rep='n'; DoneWinCrt END. {end of file Lorentz.pas}