2022-04-12 19:20:18 +02:00
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/*********************************************************************************/
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/* */
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/* Animation of wave equation in a planar domain */
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/* */
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/* N. Berglund, december 2012, may 2021 */
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/* */
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/* UPDATE 24/04: distinction between damping and "elasticity" parameters */
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/* UPDATE 27/04: new billiard shapes, bug in color scheme fixed */
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/* UPDATE 28/04: code made more efficient, with help of Marco Mancini */
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/* */
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/* Feel free to reuse, but if doing so it would be nice to drop a */
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/* line to nils.berglund@univ-orleans.fr - Thanks! */
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/* */
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/* compile with */
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/* gcc -o wave_billiard wave_billiard.c */
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/* -L/usr/X11R6/lib -ltiff -lm -lGL -lGLU -lX11 -lXmu -lglut -O3 -fopenmp */
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/* */
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/* OMP acceleration may be more effective after executing */
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/* export OMP_NUM_THREADS=2 in the shell before running the program */
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/* */
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/* To make a video, set MOVIE to 1 and create subfolder tif_wave */
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/* It may be possible to increase parameter PAUSE */
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/* */
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/* create movie using */
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/* ffmpeg -i wave.%05d.tif -vcodec libx264 wave.mp4 */
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/* */
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/*********************************************************************************/
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/*********************************************************************************/
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/* */
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/* NB: The algorithm used to simulate the wave equation is highly paralellizable */
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/* One could make it much faster by using a GPU */
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/* */
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/*********************************************************************************/
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#include <math.h>
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#include <string.h>
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#include <GL/glut.h>
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#include <GL/glu.h>
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#include <unistd.h>
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#include <sys/types.h>
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#include <tiffio.h> /* Sam Leffler's libtiff library. */
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#include <omp.h>
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2022-05-14 20:58:08 +02:00
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#include <time.h>
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2022-04-12 19:20:18 +02:00
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2023-01-22 16:49:04 +01:00
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#define MOVIE 1 /* set to 1 to generate movie */
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2022-10-18 23:28:20 +02:00
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#define DOUBLE_MOVIE 1 /* set to 1 to produce movies for wave height and energy simultaneously */
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2023-01-22 16:49:04 +01:00
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#define SAVE_MEMORY 1 /* set to 1 to save memory when writing tiff images */
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#define NO_EXTRA_BUFFER_SWAP 1 /* some OS require one less buffer swap when recording images */
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2022-04-12 19:20:18 +02:00
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/* General geometrical parameters */
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2023-01-22 16:49:04 +01:00
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// #define WINWIDTH 1920 /* window width */
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// #define WINHEIGHT 1150 /* window height */
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// // // // #define NX 2500 /* number of grid points on x axis */
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// // // // #define NY 1250 /* number of grid points on y axis */
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// #define NX 1800 /* number of grid points on x axis */
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// #define NY 1800 /* number of grid points on y axis */
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// // #define NX 2700 /* number of grid points on x axis */
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// // #define NY 1350 /* number of grid points on y axis */
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// // #define YMIN -1.041666667
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// // #define YMAX 1.041666667 /* y interval for 9/16 aspect ratio */
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//
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// #define XMIN -2.0
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// #define XMAX 2.0 /* x interval */
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2022-04-12 19:20:18 +02:00
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// #define YMIN -1.041666667
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// #define YMAX 1.041666667 /* y interval for 9/16 aspect ratio */
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2023-01-22 16:49:04 +01:00
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#define HIGHRES 0 /* set to 1 if resolution of grid is double that of displayed image */
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2022-11-20 23:17:39 +01:00
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2023-01-22 16:49:04 +01:00
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#define WINWIDTH 1280 /* window width */
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#define WINHEIGHT 720 /* window height */
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2023-01-22 16:49:04 +01:00
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// #define NX 1280 /* number of grid points on x axis */
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#define NX 720 /* number of grid points on x axis */
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#define NY 720 /* number of grid points on y axis */
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// #define NX 2560 /* number of grid points on x axis */
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// #define NX 1440 /* number of grid points on x axis */
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// #define NY 1440 /* number of grid points on y axis */
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// #define NX 360 /* number of grid points on x axis */
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// #define NY 360 /* number of grid points on y axis */
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2022-11-20 23:17:39 +01:00
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// #define XMIN -2.0
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// #define XMAX 2.0 /* x interval */
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// #define YMIN -1.125
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// #define YMAX 1.125 /* y interval for 9/16 aspect ratio */
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#define XMIN -1.1
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#define XMAX 1.1 /* x interval */
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#define YMIN -1.1
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#define YMAX 1.1 /* y interval */
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2022-11-20 23:17:39 +01:00
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2022-04-12 19:20:18 +02:00
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#define JULIA_SCALE 0.8 /* scaling for Julia sets */
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/* Choice of the billiard table */
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2023-01-22 16:49:04 +01:00
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#define B_DOMAIN 32 /* choice of domain shape, see list in global_pdes.c */
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// #define B_DOMAIN 999 /* choice of domain shape, see list in global_pdes.c */
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2022-08-20 16:02:07 +02:00
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2022-10-18 23:28:20 +02:00
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#define CIRCLE_PATTERN 2 /* pattern of circles or polygons, see list in global_pdes.c */
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2022-08-20 16:02:07 +02:00
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#define COMPARISON 0 /* set to 1 to compare two different patterns */
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#define B_DOMAIN_B 20 /* second domain shape, for comparisons */
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#define CIRCLE_PATTERN_B 0 /* second pattern of circles or polygons */
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2022-05-14 20:58:08 +02:00
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2023-01-22 16:49:04 +01:00
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#define VARIABLE_IOR 1 /* set to 1 for a variable index of refraction */
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#define IOR 3 /* choice of index of refraction, see list in global_pdes.c */
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2022-06-25 15:49:37 +02:00
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#define MANDEL_IOR_SCALE -0.05 /* parameter controlling dependence of IoR on Mandelbrot escape speed */
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#define P_PERCOL 0.25 /* probability of having a circle in C_RAND_PERCOL arrangement */
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#define NPOISSON 300 /* number of points for Poisson C_RAND_POISSON arrangement */
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#define RANDOM_POLY_ANGLE 1 /* set to 1 to randomize angle of polygons */
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2022-04-12 19:20:18 +02:00
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2023-01-22 16:49:04 +01:00
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#define LAMBDA 0.75 /* parameter controlling the dimensions of domain */
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#define MU 0.25 /* parameter controlling the dimensions of domain */
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#define NPOLY 6 /* number of sides of polygon */
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#define APOLY 0.0 /* angle by which to turn polygon, in units of Pi/2 */
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#define MDEPTH 7 /* depth of computation of Menger gasket */
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#define MRATIO 3 /* ratio defining Menger gasket */
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#define MANDELLEVEL 1000 /* iteration level for Mandelbrot set */
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#define MANDELLIMIT 10.0 /* limit value for approximation of Mandelbrot set */
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#define FOCI 1 /* set to 1 to draw focal points of ellipse */
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2022-10-18 23:28:20 +02:00
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#define NGRIDX 12 /* number of grid point for grid of disks */
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#define NGRIDY 16 /* number of grid point for grid of disks */
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2022-04-12 19:20:18 +02:00
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#define X_SHOOTER -0.2
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#define Y_SHOOTER -0.6
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#define X_TARGET 0.4
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#define Y_TARGET 0.7 /* shooter and target positions in laser fight */
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#define ISO_XSHIFT_LEFT -2.9
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#define ISO_XSHIFT_RIGHT 1.4
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#define ISO_YSHIFT_LEFT -0.15
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#define ISO_YSHIFT_RIGHT -0.15
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#define ISO_SCALE 0.5 /* coordinates for isospectral billiards */
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/* You can add more billiard tables by adapting the functions */
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/* xy_in_billiard and draw_billiard below */
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/* Physical parameters of wave equation */
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2023-01-22 16:49:04 +01:00
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#define TWOSPEEDS 0 /* set to 1 to replace hardcore boundary by medium with different speed */
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2022-10-18 23:28:20 +02:00
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#define OSCILLATE_LEFT 0 /* set to 1 to add oscilating boundary condition on the left */
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#define OSCILLATE_TOPBOT 0 /* set to 1 to enforce a planar wave on top and bottom boundary */
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#define OSCILLATION_SCHEDULE 3 /* oscillation schedule, see list in global_pdes.c */
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#define OMEGA 0.001 /* frequency of periodic excitation */
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// #define OMEGA 0.0005 /* frequency of periodic excitation */
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#define AMPLITUDE 0.8 /* amplitude of periodic excitation */
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#define ACHIRP 0.2 /* acceleration coefficient in chirp */
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#define DAMPING 0.0 /* damping of periodic excitation */
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#define COURANT 0.1 /* Courant number */
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// #define COURANTB 0.0 /* Courant number in medium B */
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#define COURANTB 0.04658753 /* Courant number in medium B */
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#define GAMMA 0.0 /* damping factor in wave equation */
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#define GAMMAB 0.0 /* damping factor in wave equation */
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#define GAMMA_SIDES 1.0e-4 /* damping factor on boundary */
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#define GAMMA_TOPBOT 1.0e-7 /* damping factor on boundary */
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#define KAPPA 0.0 /* "elasticity" term enforcing oscillations */
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#define KAPPA_SIDES 5.0e-4 /* "elasticity" term on absorbing boundary */
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#define KAPPA_TOPBOT 0.0 /* "elasticity" term on absorbing boundary */
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/* The Courant number is given by c*DT/DX, where DT is the time step and DX the lattice spacing */
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/* The physical damping coefficient is given by GAMMA/(DT)^2 */
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/* Increasing COURANT speeds up the simulation, but decreases accuracy */
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/* For similar wave forms, COURANT^2*GAMMA should be kept constant */
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2022-11-20 23:17:39 +01:00
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#define ADD_OSCILLATING_SOURCE 1 /* set to 1 to add an oscillating wave source */
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#define OSCILLATING_SOURCE_PERIOD 100 /* period of oscillating source */
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#define ALTERNATE_OSCILLATING_SOURCE 0 /* set to 1 to alternate sign of oscillating source */
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/* Boundary conditions, see list in global_pdes.c */
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2022-10-18 23:28:20 +02:00
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// #define B_COND 1
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#define B_COND 2
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#define PRECOMPUTE_BC 0 /* set to 1 to compute neighbours for Laplacian in advance */
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/* Parameters for length and speed of simulation */
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2023-01-22 16:49:04 +01:00
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#define NSTEPS 2800 /* number of frames of movie */
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// #define NSTEPS 200 /* number of frames of movie */
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#define NVID 6 /* number of iterations between images displayed on screen */
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#define NSEG 1000 /* number of segments of boundary */
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#define INITIAL_TIME 0 /* time after which to start saving frames */
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#define BOUNDARY_WIDTH 2 /* width of billiard boundary */
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#define PRINT_SPEED 0 /* set to 1 to print speed of moving source */
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2022-05-14 20:58:08 +02:00
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#define PAUSE 100 /* number of frames after which to pause */
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#define PSLEEP 3 /* sleep time during pause */
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#define SLEEP1 1 /* initial sleeping time */
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#define SLEEP2 1 /* final sleeping time */
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#define MID_FRAMES 100 /* number of still frames between parts of two-part movie */
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#define END_FRAMES 100 /* number of still frames at end of movie */
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#define FADE 1 /* set to 1 to fade at end of movie */
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2022-08-20 16:02:07 +02:00
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#define ROTATE_VIEW_WHILE_FADE 1 /* set to 1 to keep rotating viewpoint during fade */
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2022-04-12 19:20:18 +02:00
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/* Parameters of initial condition */
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2023-01-22 16:49:04 +01:00
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// #define INITIAL_AMP 0.25 /* amplitude of initial condition */
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// #define INITIAL_VARIANCE 0.001 /* variance of initial condition */
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// #define INITIAL_WAVELENGTH 0.1 /* wavelength of initial condition */
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#define INITIAL_AMP 0.3 /* amplitude of initial condition */
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#define INITIAL_VARIANCE 0.0004 /* variance of initial condition */
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#define INITIAL_WAVELENGTH 0.02 /* wavelength of initial condition */
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2023-01-22 16:49:04 +01:00
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// #define INITIAL_AMP 0.35 /* amplitude of initial condition */
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// #define INITIAL_VARIANCE 0.0002 /* variance of initial condition */
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// #define INITIAL_WAVELENGTH 0.01 /* wavelength of initial condition */
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2022-10-18 23:28:20 +02:00
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2022-04-12 19:20:18 +02:00
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/* Plot type, see list in global_pdes.c */
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2023-01-22 16:49:04 +01:00
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// #define ZPLOT 103 /* wave height */
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// #define CPLOT 103 /* color scheme */
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#define ZPLOT 104 /* wave height */
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#define CPLOT 104 /* color scheme */
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#define ZPLOT_B 108
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#define CPLOT_B 108 /* plot type for second movie */
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2023-01-22 16:49:04 +01:00
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#define CHANGE_LUMINOSITY 1 /* set to 1 to let luminosity depend on energy flux intensity */
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#define FLUX_WINDOW 30 /* size of averaging window of flux intensity */
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#define AMPLITUDE_HIGH_RES 1 /* set to 1 to increase resolution of plot */
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#define SHADE_3D 1 /* set to 1 to change luminosity according to normal vector */
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#define NON_DIRICHLET_BC 0 /* set to 1 to draw only facets in domain, if field is not zero on boundary */
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#define FLOOR_ZCOORD 1 /* set to 1 to draw only facets with z not too negative */
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#define DRAW_BILLIARD 0 /* set to 1 to draw boundary */
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#define DRAW_BILLIARD_FRONT 0 /* set to 1 to draw front of boundary after drawing wave */
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#define DRAW_CONSTRUCTION_LINES 0 /* set to 1 to draw construction lines of certain domains */
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#define FADE_IN_OBSTACLE 1 /* set to 1 to fade color inside obstacles */
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#define DRAW_OUTSIDE_GRAY 0 /* experimental, draw outside of billiard in gray */
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2022-10-18 23:28:20 +02:00
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#define PLOT_SCALE_ENERGY 0.01 /* vertical scaling in energy plot */
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2023-01-22 16:49:04 +01:00
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#define PLOT_SCALE_LOG_ENERGY 0.2 /* vertical scaling in log energy plot */
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/* 3D representation */
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#define REPRESENTATION_3D 1 /* choice of 3D representation */
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#define REP_AXO_3D 0 /* linear projection (axonometry) */
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#define REP_PROJ_3D 1 /* projection on plane orthogonal to observer line of sight */
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2022-11-20 23:17:39 +01:00
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#define ROTATE_VIEW 1 /* set to 1 to rotate position of observer */
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2023-01-22 16:49:04 +01:00
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#define ROTATE_ANGLE 540.0 /* total angle of rotation during simulation */
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// #define ROTATE_ANGLE 45.0 /* total angle of rotation during simulation */
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2022-06-25 15:49:37 +02:00
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2022-04-12 19:20:18 +02:00
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/* Color schemes */
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2023-01-22 16:49:04 +01:00
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#define COLOR_PALETTE 11 /* Color palette, see list in global_pdes.c */
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#define COLOR_PALETTE_B 13 /* Color palette, see list in global_pdes.c */
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#define BLACK 1 /* background */
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#define COLOR_SCHEME 3 /* choice of color scheme, see list in global_pdes.c */
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#define SCALE 0 /* set to 1 to adjust color scheme to variance of field */
|
2023-01-22 16:49:04 +01:00
|
|
|
#define SLOPE 0.5 /* sensitivity of color on wave amplitude */
|
2022-08-20 16:02:07 +02:00
|
|
|
#define VSCALE_AMPLITUDE 1.0 /* additional scaling factor for color scheme P_3D_AMPLITUDE */
|
2023-01-22 16:49:04 +01:00
|
|
|
#define VSCALE_ENERGY 30.0 /* additional scaling factor for color scheme P_3D_ENERGY */
|
|
|
|
#define PHASE_FACTOR 20.0 /* factor in computation of phase in color scheme P_3D_PHASE */
|
2022-04-12 19:20:18 +02:00
|
|
|
#define PHASE_SHIFT 0.0 /* shift of phase in color scheme P_3D_PHASE */
|
2022-06-25 15:49:37 +02:00
|
|
|
#define ATTENUATION 0.0 /* exponential attenuation coefficient of contrast with time */
|
2023-01-22 16:49:04 +01:00
|
|
|
#define E_SCALE 100.0 /* scaling factor for energy representation */
|
2022-11-20 23:17:39 +01:00
|
|
|
#define LOG_SCALE 0.75 /* scaling factor for energy log representation */
|
2022-10-18 23:28:20 +02:00
|
|
|
#define LOG_SHIFT 0.5 /* shift of colors on log scale */
|
|
|
|
#define LOG_ENERGY_FLOOR -10.0 /* floor value for log of (total) energy */
|
2022-08-20 16:02:07 +02:00
|
|
|
#define LOG_MEAN_ENERGY_SHIFT 1.0 /* additional shift for log of mean energy */
|
2023-01-22 16:49:04 +01:00
|
|
|
#define FLUX_SCALE 20.0 /* scaling factor for energy flux representation */
|
|
|
|
#define FLUX_CSCALE 500.0 /* scaling factor for color in energy flux representation */
|
2022-04-12 19:20:18 +02:00
|
|
|
#define RESCALE_COLOR_IN_CENTER 0 /* set to 1 to decrease color intentiy in the center (for wave escaping ring) */
|
|
|
|
|
|
|
|
#define COLORHUE 260 /* initial hue of water color for scheme C_LUM */
|
|
|
|
#define COLORDRIFT 0.0 /* how much the color hue drifts during the whole simulation */
|
|
|
|
#define LUMMEAN 0.5 /* amplitude of luminosity variation for scheme C_LUM */
|
|
|
|
#define LUMAMP 0.3 /* amplitude of luminosity variation for scheme C_LUM */
|
|
|
|
#define HUEMEAN 240.0 /* mean value of hue for color scheme C_HUE */
|
2022-06-25 15:49:37 +02:00
|
|
|
#define HUEAMP -200.0 /* amplitude of variation of hue for color scheme C_HUE */
|
2022-04-12 19:20:18 +02:00
|
|
|
|
2023-01-22 16:49:04 +01:00
|
|
|
#define NXMAZE 8 /* width of maze */
|
|
|
|
#define NYMAZE 32 /* height of maze */
|
|
|
|
#define MAZE_MAX_NGBH 5 /* max number of neighbours of maze cell */
|
|
|
|
#define RAND_SHIFT 5 /* seed of random number generator */
|
2022-10-18 23:28:20 +02:00
|
|
|
#define MAZE_XSHIFT 0.0 /* horizontal shift of maze */
|
|
|
|
|
2022-06-25 15:49:37 +02:00
|
|
|
#define DRAW_COLOR_SCHEME 1 /* set to 1 to plot the color scheme */
|
2023-01-22 16:49:04 +01:00
|
|
|
#define COLORBAR_RANGE 6.0 /* scale of color scheme bar */
|
|
|
|
#define COLORBAR_RANGE_B 6.0 /* scale of color scheme bar for 2nd part */
|
2022-06-25 15:49:37 +02:00
|
|
|
#define ROTATE_COLOR_SCHEME 0 /* set to 1 to draw color scheme horizontally */
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
#define SAVE_TIME_SERIES 0 /* set to 1 to save wave time series at a point */
|
|
|
|
|
2022-10-18 23:28:20 +02:00
|
|
|
/* for compatibility with sub_wave and sub_maze */
|
|
|
|
#define ADD_POTENTIAL 0
|
|
|
|
// #define POT_MAZE 7
|
|
|
|
#define POTENTIAL 0
|
|
|
|
/* end of constants only used by sub_wave and sub_maze */
|
|
|
|
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
/* For debugging purposes only */
|
2022-08-20 16:02:07 +02:00
|
|
|
#define FLOOR 1 /* set to 1 to limit wave amplitude to VMAX */
|
2022-04-12 19:20:18 +02:00
|
|
|
#define VMAX 10.0 /* max value of wave amplitude */
|
|
|
|
|
|
|
|
/* Parameters controlling 3D projection */
|
|
|
|
|
|
|
|
double u_3d[2] = {0.75, -0.45}; /* projections of basis vectors for REP_AXO_3D representation */
|
|
|
|
double v_3d[2] = {-0.75, -0.45};
|
|
|
|
double w_3d[2] = {0.0, 0.015};
|
|
|
|
double light[3] = {0.816496581, -0.40824829, 0.40824829}; /* vector of "light" direction for P_3D_ANGLE color scheme */
|
2023-01-22 16:49:04 +01:00
|
|
|
double observer[3] = {8.0, 8.0, 12.0}; /* location of observer for REP_PROJ_3D representation */
|
2022-06-25 15:49:37 +02:00
|
|
|
int reset_view = 0; /* switch to reset 3D view parameters (for option ROTATE_VIEW) */
|
2022-04-12 19:20:18 +02:00
|
|
|
|
2023-01-22 16:49:04 +01:00
|
|
|
#define Z_SCALING_FACTOR 0.25 /* overall scaling factor of z axis for REP_PROJ_3D representation */
|
|
|
|
#define XY_SCALING_FACTOR 2.0 /* overall scaling factor for on-screen (x,y) coordinates after projection */
|
2022-06-25 15:49:37 +02:00
|
|
|
#define ZMAX_FACTOR 1.0 /* max value of z coordinate for REP_PROJ_3D representation */
|
|
|
|
#define XSHIFT_3D -0.1 /* overall x shift for REP_PROJ_3D representation */
|
2022-08-20 16:02:07 +02:00
|
|
|
#define YSHIFT_3D 0.1 /* overall y shift for REP_PROJ_3D representation */
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
|
|
|
|
#include "global_pdes.c" /* constants and global variables */
|
2022-10-18 23:28:20 +02:00
|
|
|
#include "global_3d.c" /* constants and global variables */
|
|
|
|
#include "sub_maze.c" /* support for generating mazes */
|
2022-04-12 19:20:18 +02:00
|
|
|
#include "sub_wave.c" /* common functions for wave_billiard, heat and schrodinger */
|
|
|
|
#include "wave_common.c" /* common functions for wave_billiard, wave_comparison, etc */
|
|
|
|
|
|
|
|
#include "sub_wave_3d.c" /* graphical functions specific to wave_3d */
|
|
|
|
|
|
|
|
FILE *time_series_left, *time_series_right;
|
|
|
|
|
|
|
|
double courant2, courantb2; /* Courant parameters squared */
|
|
|
|
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
void evolve_wave_half_new(double phi_in[NX*NY], double psi_in[NX*NY], double phi_out[NX*NY],
|
|
|
|
short int xy_in[NX*NY], double tc[NX*NY], double tcc[NX*NY], double tgamma[NX*NY],
|
|
|
|
t_laplacian laplace[NX*NY])
|
2022-04-12 19:20:18 +02:00
|
|
|
/* time step of field evolution */
|
|
|
|
/* phi is value of field at time t, psi at time t-1 */
|
|
|
|
/* this version of the function has been rewritten in order to minimize the number of if-branches */
|
|
|
|
{
|
|
|
|
int i, j, iplus, iminus, jplus, jminus;
|
2022-08-20 16:02:07 +02:00
|
|
|
double x, y, c, cc, gamma, tb_shift;
|
|
|
|
static long time = 0;
|
|
|
|
double *delta;
|
|
|
|
|
|
|
|
delta = (double *)malloc(NX*NY*sizeof(double));
|
|
|
|
|
|
|
|
/* compute the Laplacian */
|
|
|
|
compute_laplacian(phi_in, laplace, delta, xy_in);
|
|
|
|
|
|
|
|
time++;
|
|
|
|
|
|
|
|
if (OSCILLATE_TOPBOT) tb_shift = (int)((XMAX - XMIN)*(double)NX/(XMAX - XMIN));
|
|
|
|
|
|
|
|
/* evolution in the bulk */
|
|
|
|
#pragma omp parallel for private(i,j,iplus,iminus,jplus,jminus,x,y)
|
|
|
|
for (i=1; i<NX-1; i++){
|
|
|
|
for (j=1; j<NY-1; j++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[i*NY+j] != 0)){
|
|
|
|
x = phi_in[i*NY+j];
|
|
|
|
y = psi_in[i*NY+j];
|
|
|
|
|
|
|
|
/* evolve phi */
|
|
|
|
phi_out[i*NY+j] = -y + 2*x + tcc[i*NY+j]*delta[i*NY+j] - KAPPA*x - tgamma[i*NY+j]*(x-y);
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* left boundary */
|
|
|
|
// if (OSCILLATE_LEFT) for (j=1; j<NY-1; j++) phi_out[j] = AMPLITUDE*cos((double)time*OMEGA);
|
|
|
|
if (OSCILLATE_LEFT)
|
|
|
|
{
|
|
|
|
for (j=1; j<NY-1; j++) phi_out[j] = oscillating_bc(time);
|
|
|
|
printf("Boundary condition %.3lg\n", oscillating_bc(time));
|
|
|
|
}
|
|
|
|
else for (j=1; j<NY-1; j++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[j] != 0)){
|
|
|
|
x = phi_in[j];
|
|
|
|
y = psi_in[j];
|
|
|
|
|
|
|
|
switch (B_COND) {
|
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
phi_out[j] = -y + 2*x + tcc[j]*delta[j] - KAPPA*x - tgamma[j]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
phi_out[j] = -y + 2*x + tcc[j]*delta[j] - KAPPA*x - tgamma[j]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
phi_out[j] = x - tc[j]*(x - phi_in[NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
phi_out[j] = x - tc[j]*(x - phi_in[NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* right boundary */
|
|
|
|
for (j=1; j<NY-1; j++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[(NX-1)*NY+j] != 0)){
|
|
|
|
x = phi_in[(NX-1)*NY+j];
|
|
|
|
y = psi_in[(NX-1)*NY+j];
|
|
|
|
|
|
|
|
switch (B_COND) {
|
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
phi_out[(NX-1)*NY+j] = -y + 2*x + tcc[(NX-1)*NY+j]*delta[(NX-1)*NY+j] - KAPPA*x - tgamma[(NX-1)*NY+j]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
phi_out[(NX-1)*NY+j] = -y + 2*x + tcc[(NX-1)*NY+j]*delta[(NX-1)*NY+j] - KAPPA*x - tgamma[(NX-1)*NY+j]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
phi_out[(NX-1)*NY+j] = x - tc[(NX-1)*NY+j]*(x - phi_in[(NX-2)*NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
phi_out[(NX-1)*NY+j] = x - tc[(NX-1)*NY+j]*(x - phi_in[(NX-2)*NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* top boundary */
|
|
|
|
for (i=0; i<NX; i++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[i*NY+NY-1] != 0)){
|
|
|
|
x = phi_in[i*NY+NY-1];
|
|
|
|
y = psi_in[i*NY+NY-1];
|
|
|
|
|
|
|
|
if ((OSCILLATE_TOPBOT)&&(i < tb_shift)&&(i<NX-1)&&(i>0))
|
|
|
|
{
|
|
|
|
iplus = i+1;
|
|
|
|
iminus = i-1; if (iminus < 0) iminus = 0;
|
|
|
|
/* TO ADAPT */
|
|
|
|
phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta[i*NY+NY-1] - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
|
|
|
|
}
|
|
|
|
|
|
|
|
else switch (B_COND) {
|
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta[i*NY+NY-1] - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta[i*NY+NY-1] - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
phi_out[i*NY+NY-1] = x - tc[i*NY+NY-1]*(x - phi_in[i*NY+NY-2]) - KAPPA_TOPBOT*x - GAMMA_TOPBOT*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
if (i==0) phi_out[NY-1] = x - tc[NY-1]*(x - phi_in[1*NY+NY-1]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
else phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta[i*NY+NY-1] - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* bottom boundary */
|
|
|
|
for (i=0; i<NX; i++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[i*NY] != 0)){
|
|
|
|
x = phi_in[i*NY];
|
|
|
|
y = psi_in[i*NY];
|
|
|
|
|
|
|
|
if ((OSCILLATE_TOPBOT)&&(i < tb_shift)&&(i<NX-1)&&(i>0))
|
|
|
|
{
|
|
|
|
/* TO ADAPT */
|
|
|
|
phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta[i*NY] - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
}
|
|
|
|
|
|
|
|
else switch (B_COND) {
|
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta[i*NY] - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta[i*NY] - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
phi_out[i*NY] = x - tc[i*NY]*(x - phi_in[i*NY+1]) - KAPPA_TOPBOT*x - GAMMA_TOPBOT*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
if (i==0) phi_out[0] = x - tc[0]*(x - phi_in[NY]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
else phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta[i*NY] - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* add oscillating boundary condition on the left corners */
|
|
|
|
if (OSCILLATE_LEFT)
|
|
|
|
{
|
|
|
|
phi_out[0] = AMPLITUDE*cos((double)time*OMEGA);
|
|
|
|
phi_out[NY-1] = AMPLITUDE*cos((double)time*OMEGA);
|
|
|
|
}
|
|
|
|
|
|
|
|
/* for debugging purposes/if there is a risk of blow-up */
|
|
|
|
if (FLOOR)
|
|
|
|
{
|
|
|
|
#pragma omp parallel for private(i,j)
|
|
|
|
for (i=0; i<NX; i++){
|
|
|
|
for (j=0; j<NY; j++){
|
|
|
|
if (xy_in[i*NY+j] != 0)
|
|
|
|
{
|
|
|
|
if (phi_out[i*NY+j] > VMAX) phi_out[i*NY+j] = VMAX;
|
|
|
|
if (phi_out[i*NY+j] < -VMAX) phi_out[i*NY+j] = -VMAX;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
free(delta);
|
|
|
|
}
|
|
|
|
|
|
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void evolve_wave_half(double phi_in[NX*NY], double psi_in[NX*NY], double phi_out[NX*NY],
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short int xy_in[NX*NY], double tc[NX*NY], double tcc[NX*NY], double tgamma[NX*NY])
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/* time step of field evolution */
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/* phi is value of field at time t, psi at time t-1 */
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/* this version of the function has been rewritten in order to minimize the number of if-branches */
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{
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int i, j, iplus, iminus, jplus, jminus, jtop, jbot;
|
2022-04-12 19:20:18 +02:00
|
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|
double delta, x, y, c, cc, gamma;
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|
|
static long time = 0;
|
2022-08-20 16:02:07 +02:00
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|
static short int first = 1;
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|
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static double tb_shift;
|
2022-04-12 19:20:18 +02:00
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time++;
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|
2022-08-20 16:02:07 +02:00
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if ((OSCILLATE_TOPBOT)&&(first))
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{
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tb_shift = (int)((XMAX - XMIN)*(double)NX/(XMAX - XMIN));
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if (tb_shift >= NX-1) tb_shift = NY - 2;
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first = 0;
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}
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|
2022-04-12 19:20:18 +02:00
|
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|
#pragma omp parallel for private(i,j,iplus,iminus,jplus,jminus,delta,x,y)
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/* evolution in the bulk */
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for (i=1; i<NX-1; i++){
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for (j=1; j<NY-1; j++){
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if ((TWOSPEEDS)||(xy_in[i*NY+j] != 0)){
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|
x = phi_in[i*NY+j];
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|
|
y = psi_in[i*NY+j];
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|
|
|
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/* discretized Laplacian */
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delta = phi_in[(i+1)*NY+j] + phi_in[(i-1)*NY+j] + phi_in[i*NY+j+1] + phi_in[i*NY+j-1] - 4.0*x;
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/* evolve phi */
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phi_out[i*NY+j] = -y + 2*x + tcc[i*NY+j]*delta - KAPPA*x - tgamma[i*NY+j]*(x-y);
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}
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|
}
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|
}
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/* left boundary */
|
2022-08-20 16:02:07 +02:00
|
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// if (OSCILLATE_LEFT) for (j=1; j<NY-1; j++) phi_out[j] = AMPLITUDE*cos((double)time*OMEGA);
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if (OSCILLATE_LEFT)
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{
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for (j=1; j<NY-1; j++) phi_out[j] = oscillating_bc(time);
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// printf("Boundary condition %.3lg\n", oscillating_bc(time));
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}
|
2022-04-12 19:20:18 +02:00
|
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|
else for (j=1; j<NY-1; j++){
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if ((TWOSPEEDS)||(xy_in[j] != 0)){
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x = phi_in[j];
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y = psi_in[j];
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switch (B_COND) {
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|
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case (BC_DIRICHLET):
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|
|
{
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delta = phi_in[NY+j] + phi_in[j+1] + phi_in[j-1] - 3.0*x;
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phi_out[j] = -y + 2*x + tcc[j]*delta - KAPPA*x - tgamma[j]*(x-y);
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break;
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}
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case (BC_PERIODIC):
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|
|
|
{
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|
delta = phi_in[NY+j] + phi_in[(NX-1)*NY+j] + phi_in[j+1] + phi_in[j-1] - 4.0*x;
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phi_out[j] = -y + 2*x + tcc[j]*delta - KAPPA*x - tgamma[j]*(x-y);
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break;
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}
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case (BC_ABSORBING):
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|
|
{
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delta = phi_in[NY+j] + phi_in[j+1] + phi_in[j-1] - 3.0*x;
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phi_out[j] = x - tc[j]*(x - phi_in[NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
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break;
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}
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case (BC_VPER_HABS):
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|
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{
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delta = phi_in[NY+j] + phi_in[j+1] + phi_in[j-1] - 3.0*x;
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phi_out[j] = x - tc[j]*(x - phi_in[NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
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|
break;
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|
}
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|
|
|
}
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}
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|
|
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}
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|
/* right boundary */
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|
|
for (j=1; j<NY-1; j++){
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if ((TWOSPEEDS)||(xy_in[(NX-1)*NY+j] != 0)){
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|
|
x = phi_in[(NX-1)*NY+j];
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|
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y = psi_in[(NX-1)*NY+j];
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|
|
|
switch (B_COND) {
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|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
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|
delta = phi_in[(NX-2)*NY+j] + phi_in[(NX-1)*NY+j+1] + phi_in[(NX-1)*NY+j-1] - 3.0*x;
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|
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phi_out[(NX-1)*NY+j] = -y + 2*x + tcc[(NX-1)*NY+j]*delta - KAPPA*x - tgamma[(NX-1)*NY+j]*(x-y);
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|
break;
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|
}
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|
case (BC_PERIODIC):
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|
|
|
{
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|
|
delta = phi_in[(NX-2)*NY+j] + phi_in[j] + phi_in[(NX-1)*NY+j+1] + phi_in[(NX-1)*NY+j-1] - 4.0*x;
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phi_out[(NX-1)*NY+j] = -y + 2*x + tcc[(NX-1)*NY+j]*delta - KAPPA*x - tgamma[(NX-1)*NY+j]*(x-y);
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|
break;
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|
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|
}
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|
|
|
case (BC_ABSORBING):
|
|
|
|
{
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|
|
|
delta = phi_in[(NX-2)*NY+j] + phi_in[(NX-1)*NY+j+1] + phi_in[(NX-1)*NY+j-1] - 3.0*x;
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|
|
phi_out[(NX-1)*NY+j] = x - tc[(NX-1)*NY+j]*(x - phi_in[(NX-2)*NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
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|
break;
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|
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|
}
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|
case (BC_VPER_HABS):
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|
|
{
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|
|
|
delta = phi_in[(NX-2)*NY+j] + phi_in[(NX-1)*NY+j+1] + phi_in[(NX-1)*NY+j-1] - 3.0*x;
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|
|
phi_out[(NX-1)*NY+j] = x - tc[(NX-1)*NY+j]*(x - phi_in[(NX-2)*NY+j]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
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|
break;
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|
|
|
}
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|
|
|
}
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|
|
|
}
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|
|
}
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|
|
/* top boundary */
|
2022-08-20 16:02:07 +02:00
|
|
|
if (COMPARISON) jbot = NY/2;
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|
else jbot = 0;
|
2022-04-12 19:20:18 +02:00
|
|
|
for (i=0; i<NX; i++){
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|
|
if ((TWOSPEEDS)||(xy_in[i*NY+NY-1] != 0)){
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|
x = phi_in[i*NY+NY-1];
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|
|
y = psi_in[i*NY+NY-1];
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|
2022-08-20 16:02:07 +02:00
|
|
|
if ((OSCILLATE_TOPBOT)&&(i < tb_shift)&&(i<NX-1)&&(i>0))
|
|
|
|
{
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|
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|
iplus = i+1;
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|
iminus = i-1; if (iminus < 0) iminus = 0;
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|
delta = phi_in[iplus*NY+NY-1] + phi_in[iminus*NY+NY-1] + - 2.0*x;
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|
phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
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|
|
}
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|
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|
else switch (B_COND) {
|
2022-04-12 19:20:18 +02:00
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
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|
iplus = i+1; if (iplus == NX) iplus = NX-1;
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|
|
iminus = i-1; if (iminus == -1) iminus = 0;
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|
|
|
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|
|
delta = phi_in[iplus*NY+NY-1] + phi_in[iminus*NY+NY-1] + phi_in[i*NY+NY-2] - 3.0*x;
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|
|
phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
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|
break;
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|
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|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
iplus = (i+1) % NX;
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|
|
iminus = (i-1) % NX;
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|
|
if (iminus < 0) iminus += NX;
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|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
delta = phi_in[iplus*NY+NY-1] + phi_in[iminus*NY+NY-1] + phi_in[i*NY+NY-2] + phi_in[i*NY+jbot] - 4.0*x;
|
2022-04-12 19:20:18 +02:00
|
|
|
phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+NY-1] + phi_in[iminus*NY+NY-1] + phi_in[i*NY+NY-2] - 3.0*x;
|
|
|
|
phi_out[i*NY+NY-1] = x - tc[i*NY+NY-1]*(x - phi_in[i*NY+NY-2]) - KAPPA_TOPBOT*x - GAMMA_TOPBOT*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
delta = phi_in[iplus*NY+NY-1] + phi_in[iminus*NY+NY-1] + phi_in[i*NY+NY-2] + phi_in[i*NY+jbot] - 4.0*x;
|
2022-04-12 19:20:18 +02:00
|
|
|
if (i==0) phi_out[NY-1] = x - tc[NY-1]*(x - phi_in[1*NY+NY-1]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
else phi_out[i*NY+NY-1] = -y + 2*x + tcc[i*NY+NY-1]*delta - KAPPA*x - tgamma[i*NY+NY-1]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* bottom boundary */
|
2022-08-20 16:02:07 +02:00
|
|
|
if (COMPARISON) jtop = NY/2-1;
|
|
|
|
else jtop = NY-1;
|
2022-04-12 19:20:18 +02:00
|
|
|
for (i=0; i<NX; i++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[i*NY] != 0)){
|
|
|
|
x = phi_in[i*NY];
|
|
|
|
y = psi_in[i*NY];
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
if ((OSCILLATE_TOPBOT)&&(i < tb_shift)&&(i<NX-1)&&(i>0))
|
|
|
|
{
|
|
|
|
iplus = i+1;
|
|
|
|
iminus = i-1; if (iminus < 0) iminus = 0;
|
|
|
|
delta = phi_in[iplus*NY] + phi_in[iminus*NY] + - 2.0*x;
|
|
|
|
phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
}
|
|
|
|
|
|
|
|
else switch (B_COND) {
|
2022-04-12 19:20:18 +02:00
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
iplus = i+1; if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = i-1; if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY] + phi_in[iminus*NY] + phi_in[i*NY+1] - 3.0*x;
|
|
|
|
phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
iplus = (i+1) % NX;
|
|
|
|
iminus = (i-1) % NX;
|
|
|
|
if (iminus < 0) iminus += NX;
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
delta = phi_in[iplus*NY] + phi_in[iminus*NY] + phi_in[i*NY+1] + phi_in[i*NY+jtop] - 4.0*x;
|
2022-04-12 19:20:18 +02:00
|
|
|
phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY] + phi_in[iminus*NY] + phi_in[i*NY+1] - 3.0*x;
|
|
|
|
phi_out[i*NY] = x - tc[i*NY]*(x - phi_in[i*NY+1]) - KAPPA_TOPBOT*x - GAMMA_TOPBOT*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
delta = phi_in[iplus*NY] + phi_in[iminus*NY] + phi_in[i*NY+1] + phi_in[i*NY+jtop] - 4.0*x;
|
2022-04-12 19:20:18 +02:00
|
|
|
if (i==0) phi_out[0] = x - tc[0]*(x - phi_in[NY]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
else phi_out[i*NY] = -y + 2*x + tcc[i*NY]*delta - KAPPA*x - tgamma[i*NY]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
/* case of comparisons - top of bottom half */
|
|
|
|
if (COMPARISON) for (i=0; i<NX; i++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[i*NY+jtop] != 0)){
|
|
|
|
x = phi_in[i*NY+jtop];
|
|
|
|
y = psi_in[i*NY+jtop];
|
|
|
|
|
|
|
|
switch (B_COND) {
|
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
iplus = i+1; if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = i-1; if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jtop] + phi_in[iminus*NY+jtop] + phi_in[i*NY+jtop-1] - 3.0*x;
|
|
|
|
phi_out[i*NY+jtop] = -y + 2*x + tcc[i*NY+jtop]*delta - KAPPA*x - tgamma[i*NY+jtop]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
iplus = (i+1) % NX;
|
|
|
|
iminus = (i-1) % NX;
|
|
|
|
if (iminus < 0) iminus += NX;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jtop] + phi_in[iminus*NY+jtop] + phi_in[i*NY+jtop-1] + phi_in[i*NY] - 4.0*x;
|
|
|
|
phi_out[i*NY+jtop] = -y + 2*x + tcc[i*NY+jtop]*delta - KAPPA*x - tgamma[i*NY+jtop]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jtop] + phi_in[iminus*NY+jtop] + phi_in[i*NY+jtop-1] - 3.0*x;
|
|
|
|
phi_out[i*NY+jtop] = x - tc[i*NY+jtop]*(x - phi_in[i*NY+jtop-1]) - KAPPA_TOPBOT*x - GAMMA_TOPBOT*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jtop] + phi_in[iminus*NY+jtop] + phi_in[i*NY+jtop-1] + phi_in[i*NY] - 4.0*x;
|
|
|
|
if (i==0) phi_out[jtop] = x - tc[jtop]*(x - phi_in[1*NY+jtop]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
else phi_out[i*NY+jtop] = -y + 2*x + tcc[i*NY+jtop]*delta - KAPPA*x - tgamma[i*NY+jtop]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* case of comparisons - bottom of top half */
|
|
|
|
if (COMPARISON) for (i=0; i<NX; i++){
|
|
|
|
if ((TWOSPEEDS)||(xy_in[i*NY+jbot] != 0)){
|
|
|
|
x = phi_in[i*NY+jbot];
|
|
|
|
y = psi_in[i*NY+jbot];
|
|
|
|
|
|
|
|
switch (B_COND) {
|
|
|
|
case (BC_DIRICHLET):
|
|
|
|
{
|
|
|
|
iplus = i+1; if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = i-1; if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jbot] + phi_in[iminus*NY+jbot] + phi_in[i*NY+jbot+1] - 3.0*x;
|
|
|
|
phi_out[i*NY+jbot] = -y + 2*x + tcc[i*NY+jbot]*delta - KAPPA*x - tgamma[i*NY+jbot]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_PERIODIC):
|
|
|
|
{
|
|
|
|
iplus = (i+1) % NX;
|
|
|
|
iminus = (i-1) % NX;
|
|
|
|
if (iminus < 0) iminus += NX;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jbot] + phi_in[iminus*NY+jbot] + phi_in[i*NY+jbot+1] + phi_in[i*NY+jbot] - 4.0*x;
|
|
|
|
phi_out[i*NY+jbot] = -y + 2*x + tcc[i*NY+jbot]*delta - KAPPA*x - tgamma[i*NY+jbot]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_ABSORBING):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jbot] + phi_in[iminus*NY+jbot] + phi_in[i*NY+jbot+1] - 3.0*x;
|
|
|
|
phi_out[i*NY+jbot] = x - tc[i*NY+jbot]*(x - phi_in[i*NY+jbot+1]) - KAPPA_TOPBOT*x - GAMMA_TOPBOT*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
case (BC_VPER_HABS):
|
|
|
|
{
|
|
|
|
iplus = (i+1); if (iplus == NX) iplus = NX-1;
|
|
|
|
iminus = (i-1); if (iminus == -1) iminus = 0;
|
|
|
|
|
|
|
|
delta = phi_in[iplus*NY+jbot] + phi_in[iminus*NY+jbot] + phi_in[i*NY+jbot+1] + phi_in[i*NY+NY-1] - 4.0*x;
|
|
|
|
if (i==0) phi_out[jbot] = x - tc[jbot]*(x - phi_in[NY]) - KAPPA_SIDES*x - GAMMA_SIDES*(x-y);
|
|
|
|
else phi_out[i*NY+jbot] = -y + 2*x + tcc[i*NY+jbot]*delta - KAPPA*x - tgamma[i*NY+jbot]*(x-y);
|
|
|
|
break;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
/* add oscillating boundary condition on the left corners */
|
|
|
|
if (OSCILLATE_LEFT)
|
|
|
|
{
|
2022-08-20 16:02:07 +02:00
|
|
|
phi_out[0] = oscillating_bc(time);
|
|
|
|
phi_out[NY-1] = oscillating_bc(time);
|
2022-04-12 19:20:18 +02:00
|
|
|
}
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
/* for debugging purposes/if there is a risk of blow-up */
|
|
|
|
if (FLOOR) for (i=0; i<NX; i++){
|
|
|
|
for (j=0; j<NY; j++){
|
|
|
|
if (xy_in[i*NY+j] != 0)
|
|
|
|
{
|
|
|
|
if (phi_out[i*NY+j] > VMAX) phi_out[i*NY+j] = VMAX;
|
|
|
|
if (phi_out[i*NY+j] < -VMAX) phi_out[i*NY+j] = -VMAX;
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
|
2022-07-17 13:50:13 +02:00
|
|
|
void evolve_wave(double phi[NX*NY], double psi[NX*NY], double tmp[NX*NY], short int xy_in[NX*NY],
|
2022-08-20 16:02:07 +02:00
|
|
|
double tc[NX*NY], double tcc[NX*NY], double tgamma[NX*NY], t_laplacian laplace[NX*NY], t_laplacian laplace1[NX*NY],
|
|
|
|
t_laplacian laplace2[NX*NY])
|
2022-04-12 19:20:18 +02:00
|
|
|
/* time step of field evolution */
|
|
|
|
/* phi is value of field at time t, psi at time t-1 */
|
|
|
|
{
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRECOMPUTE_BC)
|
|
|
|
{
|
|
|
|
// evolve_wave_half_new(phi, psi, phi_tmp, psi_tmp, xy_in, tc, tcc, tgamma, laplace);
|
|
|
|
// evolve_wave_half_new(phi_tmp, psi_tmp, phi, psi, xy_in, tc, tcc, tgamma, laplace_tmp);
|
|
|
|
evolve_wave_half_new(phi, psi, tmp, xy_in, tc, tcc, tgamma, laplace);
|
|
|
|
evolve_wave_half_new(tmp, phi, psi, xy_in, tc, tcc, tgamma, laplace1);
|
|
|
|
evolve_wave_half_new(psi, tmp, phi, xy_in, tc, tcc, tgamma, laplace2);
|
|
|
|
}
|
|
|
|
else
|
|
|
|
{
|
|
|
|
// evolve_wave_half(phi, psi, phi_tmp, psi_tmp, xy_in, tc, tcc, tgamma);
|
|
|
|
// evolve_wave_half(phi_tmp, psi_tmp, phi, psi, xy_in, tc, tcc, tgamma);
|
|
|
|
evolve_wave_half(phi, psi, tmp, xy_in, tc, tcc, tgamma);
|
|
|
|
evolve_wave_half(tmp, phi, psi, xy_in, tc, tcc, tgamma);
|
|
|
|
evolve_wave_half(psi, tmp, phi, xy_in, tc, tcc, tgamma);
|
|
|
|
}
|
2022-04-12 19:20:18 +02:00
|
|
|
}
|
|
|
|
|
|
|
|
|
2022-05-14 20:58:08 +02:00
|
|
|
void draw_color_bar_palette(int plot, double range, int palette, int fade, double fade_value)
|
2022-04-12 19:20:18 +02:00
|
|
|
{
|
2023-01-22 16:49:04 +01:00
|
|
|
double width = 0.1;
|
|
|
|
// double width = 0.14;
|
2022-05-14 20:58:08 +02:00
|
|
|
// double width = 0.2;
|
|
|
|
|
2023-01-22 16:49:04 +01:00
|
|
|
width *= (double)NX/(double)WINWIDTH;
|
|
|
|
|
2022-05-14 20:58:08 +02:00
|
|
|
if (ROTATE_COLOR_SCHEME)
|
|
|
|
draw_color_scheme_palette_3d(-1.0, -0.8, XMAX - 0.1, -1.0, plot, -range, range, palette, fade, fade_value);
|
|
|
|
else
|
|
|
|
draw_color_scheme_palette_3d(XMAX - 1.5*width, YMIN + 0.1, XMAX - 0.5*width, YMAX - 0.1, plot, -range, range, palette, fade, fade_value);
|
2022-04-12 19:20:18 +02:00
|
|
|
}
|
|
|
|
|
2022-06-25 15:49:37 +02:00
|
|
|
void viewpoint_schedule(int i)
|
|
|
|
/* change position of observer */
|
|
|
|
{
|
|
|
|
int j;
|
|
|
|
double angle, ca, sa;
|
|
|
|
static double observer_initial[3];
|
|
|
|
static int first = 1;
|
|
|
|
|
|
|
|
if (first)
|
|
|
|
{
|
|
|
|
for (j=0; j<3; j++) observer_initial[j] = observer[j];
|
|
|
|
first = 0;
|
|
|
|
}
|
|
|
|
|
|
|
|
angle = (ROTATE_ANGLE*DPI/360.0)*(double)i/(double)NSTEPS;
|
|
|
|
ca = cos(angle);
|
|
|
|
sa = sin(angle);
|
|
|
|
observer[0] = ca*observer_initial[0] - sa*observer_initial[1];
|
|
|
|
observer[1] = sa*observer_initial[0] + ca*observer_initial[1];
|
|
|
|
printf("Angle %.3lg, Observer position (%.3lg, %.3lg, %.3lg)\n", angle, observer[0], observer[1], observer[2]);
|
|
|
|
}
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
void animation()
|
|
|
|
{
|
2023-01-22 16:49:04 +01:00
|
|
|
double time, scale, ratio, startleft[2], startright[2], sign = 1.0, r2, xy[2], fade_value, yshift, speed = 0.0, a, b, c, angle, lambda1;
|
|
|
|
double *phi, *psi, *tmp, *color_scale, *tc, *tcc, *tgamma;
|
|
|
|
// double *total_energy;
|
2022-04-12 19:20:18 +02:00
|
|
|
short int *xy_in;
|
|
|
|
int i, j, s, sample_left[2], sample_right[2], period = 0, fade;
|
|
|
|
static int counter = 0;
|
|
|
|
long int wave_value;
|
|
|
|
t_wave *wave;
|
2022-08-20 16:02:07 +02:00
|
|
|
t_laplacian *laplace, *laplace1, *laplace2;
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
if (SAVE_TIME_SERIES)
|
|
|
|
{
|
|
|
|
time_series_left = fopen("wave_left.dat", "w");
|
|
|
|
time_series_right = fopen("wave_right.dat", "w");
|
|
|
|
}
|
|
|
|
|
|
|
|
/* Since NX and NY are big, it seemed wiser to use some memory allocation here */
|
|
|
|
xy_in = (short int *)malloc(NX*NY*sizeof(short int));
|
|
|
|
phi = (double *)malloc(NX*NY*sizeof(double));
|
|
|
|
psi = (double *)malloc(NX*NY*sizeof(double));
|
2022-07-17 13:50:13 +02:00
|
|
|
tmp = (double *)malloc(NX*NY*sizeof(double));
|
2023-01-22 16:49:04 +01:00
|
|
|
// total_energy = (double *)malloc(NX*NY*sizeof(double));
|
2022-04-12 19:20:18 +02:00
|
|
|
color_scale = (double *)malloc(NX*NY*sizeof(double));
|
|
|
|
tc = (double *)malloc(NX*NY*sizeof(double));
|
|
|
|
tcc = (double *)malloc(NX*NY*sizeof(double));
|
|
|
|
tgamma = (double *)malloc(NX*NY*sizeof(double));
|
|
|
|
|
|
|
|
wave = (t_wave *)malloc(NX*NY*sizeof(t_wave));
|
|
|
|
|
2022-08-20 16:02:07 +02:00
|
|
|
laplace = (t_laplacian *)malloc(NX*NY*sizeof(t_laplacian));
|
|
|
|
laplace1 = (t_laplacian *)malloc(NX*NY*sizeof(t_laplacian));
|
|
|
|
laplace2 = (t_laplacian *)malloc(NX*NY*sizeof(t_laplacian));
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
/* initialise positions and radii of circles */
|
2022-08-20 16:02:07 +02:00
|
|
|
if (COMPARISON)
|
|
|
|
{
|
|
|
|
if ((B_DOMAIN == D_CIRCLES)||(B_DOMAIN == D_CIRCLES_IN_RECT))
|
|
|
|
ncircles = init_circle_config_pattern(circles, CIRCLE_PATTERN);
|
|
|
|
else if (B_DOMAIN == D_POLYGONS) ncircles = init_polygon_config_pattern(polygons, CIRCLE_PATTERN);
|
|
|
|
|
|
|
|
if ((B_DOMAIN_B == D_CIRCLES)||(B_DOMAIN_B == D_CIRCLES_IN_RECT))
|
|
|
|
ncircles_b = init_circle_config_pattern(circles_b, CIRCLE_PATTERN_B);
|
|
|
|
else if (B_DOMAIN_B == D_POLYGONS) ncircles_b = init_polygon_config_pattern(polygons_b, CIRCLE_PATTERN_B);
|
|
|
|
/* TO DO: adapt to different polygon patterns */
|
|
|
|
}
|
|
|
|
else
|
|
|
|
{
|
|
|
|
if ((B_DOMAIN == D_CIRCLES)||(B_DOMAIN == D_CIRCLES_IN_RECT)) ncircles = init_circle_config(circles);
|
|
|
|
else if (B_DOMAIN == D_POLYGONS) ncircles = init_polygon_config(polygons);
|
|
|
|
}
|
2022-04-12 19:20:18 +02:00
|
|
|
printf("Polygons initialized\n");
|
|
|
|
|
|
|
|
/* initialise polyline for von Koch and similar domains */
|
|
|
|
npolyline = init_polyline(MDEPTH, polyline);
|
|
|
|
for (i=0; i<npolyline; i++) printf("vertex %i: (%.3f, %.3f)\n", i, polyline[i].x, polyline[i].y);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (COMPARISON) npolyline_b = init_polyline(MDEPTH, polyline);
|
2022-10-18 23:28:20 +02:00
|
|
|
|
|
|
|
npolyrect = init_polyrect(polyrect);
|
|
|
|
for (i=0; i<npolyrect; i++) printf("polyrect vertex %i: (%.3f, %.3f) - (%.3f, %.3f)\n", i, polyrect[i].x1, polyrect[i].y1, polyrect[i].x2, polyrect[i].y2);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
2023-01-22 16:49:04 +01:00
|
|
|
init_polyrect_arc(polyrectrot, polyarc, &npolyrect_rot, &npolyarc);
|
|
|
|
printf("Rotated rectangles and arcs initialized\n");
|
|
|
|
printf("%i rotated rectangles, %i arcs\n", npolyrect_rot, npolyarc);
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
courant2 = COURANT*COURANT;
|
|
|
|
courantb2 = COURANTB*COURANTB;
|
2022-08-20 16:02:07 +02:00
|
|
|
c = COURANT*(XMAX - XMIN)/(double)NX;
|
|
|
|
// a = 0.015;
|
|
|
|
// b = 0.0003;
|
|
|
|
// a = 0.04;
|
|
|
|
// b = 0.0018;
|
|
|
|
a = 0.05;
|
|
|
|
b = 0.0016;
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
/* initialize color scale, for option RESCALE_COLOR_IN_CENTER */
|
|
|
|
if (RESCALE_COLOR_IN_CENTER)
|
|
|
|
{
|
|
|
|
for (i=0; i<NX; i++)
|
|
|
|
for (j=0; j<NY; j++)
|
|
|
|
{
|
|
|
|
ij_to_xy(i, j, xy);
|
|
|
|
r2 = xy[0]*xy[0] + xy[1]*xy[1];
|
|
|
|
color_scale[i*NY+j] = 1.0 - exp(-4.0*r2/LAMBDA*LAMBDA);
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
/* initialize wave with a drop at one point, zero elsewhere */
|
|
|
|
// init_circular_wave(0.0, -LAMBDA, phi, psi, xy_in);
|
2022-08-20 16:02:07 +02:00
|
|
|
|
|
|
|
/* initialize coordinates of neighbours for discrete Laplacian */
|
|
|
|
if (PRECOMPUTE_BC)
|
|
|
|
{
|
|
|
|
init_laplacian_coords(laplace, phi);
|
|
|
|
init_laplacian_coords(laplace1, tmp);
|
|
|
|
init_laplacian_coords(laplace2, psi);
|
|
|
|
}
|
2022-04-12 19:20:18 +02:00
|
|
|
|
2023-01-22 16:49:04 +01:00
|
|
|
|
|
|
|
init_wave_fields(wave);
|
|
|
|
|
|
|
|
/* initialize total energy table - no longer needed */
|
|
|
|
// if ((ZPLOT == P_MEAN_ENERGY)||(ZPLOT_B == P_MEAN_ENERGY)||(ZPLOT == P_LOG_MEAN_ENERGY)||(ZPLOT_B == P_LOG_MEAN_ENERGY))
|
|
|
|
// for (i=0; i<NX; i++)
|
|
|
|
// for (j=0; j<NY; j++)
|
|
|
|
// total_energy[i*NY+j] = 0.0;
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
ratio = (XMAX - XMIN)/8.4; /* for Tokarsky billiard */
|
|
|
|
|
|
|
|
|
|
|
|
// init_circular_wave_mod(polyline[85].x, polyline[85].y, phi, psi, xy_in);
|
2023-01-22 16:49:04 +01:00
|
|
|
// init_circular_wave_mod(LAMBDA*cos(APOLY*PID), LAMBDA*sin(APOLY*PID), phi, psi, xy_in);
|
|
|
|
lambda1 = LAMBDA;
|
|
|
|
angle = DPI/(double)NPOLY;
|
|
|
|
init_circular_wave_mod(lambda1*cos(0.5*angle), lambda1*sin(0.5*angle), phi, psi, xy_in);
|
|
|
|
for (j=1; j<NPOLY; j++)
|
|
|
|
add_circular_wave_mod(1.0, lambda1*cos(((double)j+0.5)*angle), lambda1*sin(((double)j+0.5)*angle), phi, psi, xy_in);
|
|
|
|
|
2022-10-18 23:28:20 +02:00
|
|
|
// init_wave_flat_mod(phi, psi, xy_in);
|
2022-06-25 15:49:37 +02:00
|
|
|
// add_circular_wave_mod(1.0, 1.0, 0.0, phi, psi, xy_in);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
// printf("Wave initialized\n");
|
|
|
|
|
|
|
|
|
|
|
|
/* initialize table of wave speeds/dissipation */
|
2022-05-14 20:58:08 +02:00
|
|
|
init_speed_dissipation(xy_in, tc, tcc, tgamma);
|
|
|
|
|
|
|
|
init_zfield(phi, psi, xy_in, ZPLOT, wave, 0);
|
|
|
|
init_cfield(phi, psi, xy_in, CPLOT, wave, 0);
|
|
|
|
|
|
|
|
if (DOUBLE_MOVIE)
|
|
|
|
{
|
|
|
|
init_zfield(phi, psi, xy_in, ZPLOT_B, wave, 1);
|
|
|
|
init_cfield(phi, psi, xy_in, CPLOT_B, wave, 1);
|
2022-04-12 19:20:18 +02:00
|
|
|
}
|
|
|
|
|
|
|
|
blank();
|
|
|
|
glColor3f(0.0, 0.0, 0.0);
|
2022-05-14 20:58:08 +02:00
|
|
|
draw_wave_3d(0, phi, psi, xy_in, wave, ZPLOT, CPLOT, COLOR_PALETTE, 0, 1.0, 1);
|
2022-04-12 19:20:18 +02:00
|
|
|
// draw_billiard();
|
|
|
|
|
|
|
|
|
2022-05-14 20:58:08 +02:00
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT, COLORBAR_RANGE, COLOR_PALETTE, 0, 1.0);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
glutSwapBuffers();
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
sleep(SLEEP1);
|
|
|
|
|
|
|
|
for (i=0; i<=INITIAL_TIME + NSTEPS; i++)
|
|
|
|
{
|
2022-05-14 20:58:08 +02:00
|
|
|
global_time++;
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
//printf("%d\n",i);
|
|
|
|
/* compute the variance of the field to adjust color scheme */
|
|
|
|
/* the color depends on the field divided by sqrt(1 + variance) */
|
|
|
|
if (SCALE)
|
|
|
|
{
|
|
|
|
scale = sqrt(1.0 + compute_variance_mod(phi,psi, xy_in));
|
|
|
|
// printf("Scaling factor: %5lg\n", scale);
|
|
|
|
}
|
|
|
|
else scale = 1.0;
|
|
|
|
|
2022-06-25 15:49:37 +02:00
|
|
|
if (ROTATE_VIEW)
|
|
|
|
{
|
|
|
|
viewpoint_schedule(i - INITIAL_TIME);
|
|
|
|
reset_view = 1;
|
|
|
|
}
|
|
|
|
|
2022-05-14 20:58:08 +02:00
|
|
|
draw_wave_3d(0, phi, psi, xy_in, wave, ZPLOT, CPLOT, COLOR_PALETTE, 0, 1.0, 1);
|
2022-04-12 19:20:18 +02:00
|
|
|
for (j=0; j<NVID; j++)
|
|
|
|
{
|
2022-08-20 16:02:07 +02:00
|
|
|
evolve_wave(phi, psi, tmp, xy_in, tc, tcc, tgamma, laplace, laplace1, laplace2);
|
2022-04-12 19:20:18 +02:00
|
|
|
if (SAVE_TIME_SERIES)
|
|
|
|
{
|
|
|
|
wave_value = (long int)(phi[sample_left[0]*NY+sample_left[1]]*1.0e16);
|
|
|
|
fprintf(time_series_left, "%019ld\n", wave_value);
|
|
|
|
wave_value = (long int)(phi[sample_right[0]*NY+sample_right[1]]*1.0e16);
|
|
|
|
fprintf(time_series_right, "%019ld\n", wave_value);
|
|
|
|
if ((j == 0)&&(i%10 == 0)) printf("Frame %i of %i\n", i, NSTEPS);
|
|
|
|
// fprintf(time_series_right, "%.15f\n", phi[sample_right[0]][sample_right[1]]);
|
|
|
|
}
|
|
|
|
// if (i % 10 == 9) oscillate_linear_wave(0.2*scale, 0.15*(double)(i*NVID + j), -1.5, YMIN, -1.5, YMAX, phi, psi);
|
|
|
|
}
|
|
|
|
|
|
|
|
// draw_billiard();
|
|
|
|
|
2022-05-14 20:58:08 +02:00
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT, COLORBAR_RANGE, COLOR_PALETTE, fade, fade_value);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
/* add oscillating waves */
|
2022-08-20 16:02:07 +02:00
|
|
|
// if ((ADD_OSCILLATING_SOURCE)&&(i%OSCILLATING_SOURCE_PERIOD == OSCILLATING_SOURCE_PERIOD - 1))
|
|
|
|
if ((ADD_OSCILLATING_SOURCE)&&(i%OSCILLATING_SOURCE_PERIOD == 1))
|
2022-04-12 19:20:18 +02:00
|
|
|
{
|
2022-08-20 16:02:07 +02:00
|
|
|
// add_circular_wave_mod(1.0, -1.0, 0.0, phi, psi, xy_in);
|
2022-04-12 19:20:18 +02:00
|
|
|
// add_circular_wave(1.0, -1.5*LAMBDA, 0.0, phi, psi, xy_in);
|
|
|
|
// add_circular_wave(-1.0, 0.6*cos((double)(period)*DPI/3.0), 0.6*sin((double)(period)*DPI/3.0), phi, psi, xy_in);
|
2022-11-20 23:17:39 +01:00
|
|
|
// yshift = (double)period*a + (double)(period*period)*b;
|
|
|
|
if (ALTERNATE_OSCILLATING_SOURCE) sign = -sign;
|
2023-01-22 16:49:04 +01:00
|
|
|
for (j=0; j<NPOLY; j++)
|
|
|
|
add_circular_wave_mod(sign, lambda1*cos(((double)j+0.5)*angle), lambda1*sin(((double)j+0.5)*angle), phi, psi, xy_in);
|
2022-08-20 16:02:07 +02:00
|
|
|
// speed = (a + 2.0*(double)(period)*b)/((double)(NVID));
|
|
|
|
// speed = 0.55*(a + 2.0*(double)(period)*b)/((double)(NVID*OSCILLATING_SOURCE_PERIOD));
|
2022-11-20 23:17:39 +01:00
|
|
|
// speed = (a + 2.0*(double)(period)*b)/((double)(3*NVID*OSCILLATING_SOURCE_PERIOD));
|
|
|
|
// printf("v = %.3lg, c = %.3lg\n", speed, c);
|
|
|
|
// speed = speed/c;
|
|
|
|
// sign = -sign;
|
|
|
|
// period++;
|
2022-04-12 19:20:18 +02:00
|
|
|
}
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 0, 1.0);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
2023-01-22 16:49:04 +01:00
|
|
|
if (!((NO_EXTRA_BUFFER_SWAP)&&(MOVIE))) glutSwapBuffers();
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
if (MOVIE)
|
|
|
|
{
|
|
|
|
if (i >= INITIAL_TIME) save_frame();
|
2023-01-22 16:49:04 +01:00
|
|
|
// if (i >= INITIAL_TIME) save_frame_counter(i);
|
|
|
|
// if (i >= INITIAL_TIME) save_frame_counter(NSTEPS + MID_FRAMES + 1 + counter);
|
2022-04-12 19:20:18 +02:00
|
|
|
else printf("Initial phase time %i of %i\n", i, INITIAL_TIME);
|
|
|
|
|
|
|
|
if ((i >= INITIAL_TIME)&&(DOUBLE_MOVIE))
|
|
|
|
{
|
2022-05-14 20:58:08 +02:00
|
|
|
draw_wave_3d(1, phi, psi, xy_in, wave, ZPLOT_B, CPLOT_B, COLOR_PALETTE_B, 0, 1.0, 1);
|
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT_B, COLORBAR_RANGE_B, COLOR_PALETTE_B, 0, 1.0);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 0, 1.0);
|
2022-04-12 19:20:18 +02:00
|
|
|
glutSwapBuffers();
|
|
|
|
save_frame_counter(NSTEPS + MID_FRAMES + 1 + counter);
|
2023-01-22 16:49:04 +01:00
|
|
|
// save_frame_counter(i);
|
2022-04-12 19:20:18 +02:00
|
|
|
counter++;
|
|
|
|
}
|
2023-01-22 16:49:04 +01:00
|
|
|
else if (NO_EXTRA_BUFFER_SWAP) glutSwapBuffers();
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
/* it seems that saving too many files too fast can cause trouble with the file system */
|
|
|
|
/* so this is to make a pause from time to time - parameter PAUSE may need adjusting */
|
|
|
|
if (i % PAUSE == PAUSE - 1)
|
|
|
|
{
|
|
|
|
printf("Making a short pause\n");
|
|
|
|
sleep(PSLEEP);
|
|
|
|
s = system("mv wave*.tif tif_wave/");
|
|
|
|
}
|
|
|
|
}
|
2022-08-20 16:02:07 +02:00
|
|
|
else printf("Computing frame %i\n", i);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
}
|
|
|
|
|
|
|
|
if (MOVIE)
|
|
|
|
{
|
|
|
|
if (DOUBLE_MOVIE)
|
|
|
|
{
|
2022-05-14 20:58:08 +02:00
|
|
|
draw_wave_3d(0, phi, psi, xy_in, wave, ZPLOT, CPLOT, COLOR_PALETTE, 0, 1.0, 1);
|
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT, COLORBAR_RANGE, COLOR_PALETTE, 0, 1.0);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 0, 1.0);
|
2022-04-12 19:20:18 +02:00
|
|
|
glutSwapBuffers();
|
|
|
|
|
|
|
|
if (!FADE) for (i=0; i<MID_FRAMES; i++) save_frame();
|
|
|
|
else for (i=0; i<MID_FRAMES; i++)
|
|
|
|
{
|
2022-06-25 15:49:37 +02:00
|
|
|
if ((ROTATE_VIEW)&&(ROTATE_VIEW_WHILE_FADE))
|
|
|
|
{
|
|
|
|
viewpoint_schedule(NSTEPS - INITIAL_TIME + i);
|
|
|
|
reset_view = 1;
|
|
|
|
}
|
2022-05-14 20:58:08 +02:00
|
|
|
fade_value = 1.0 - (double)i/(double)MID_FRAMES;
|
|
|
|
draw_wave_3d(0, phi, psi, xy_in, wave, ZPLOT, CPLOT, COLOR_PALETTE, 1, fade_value, 0);
|
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT, COLORBAR_RANGE, COLOR_PALETTE, 1, fade_value);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 1, fade_value);
|
2023-01-22 16:49:04 +01:00
|
|
|
if (!NO_EXTRA_BUFFER_SWAP) glutSwapBuffers();
|
2022-04-12 19:20:18 +02:00
|
|
|
save_frame_counter(NSTEPS + i + 1);
|
|
|
|
}
|
2023-01-22 16:49:04 +01:00
|
|
|
|
|
|
|
if ((ROTATE_VIEW)&&(ROTATE_VIEW_WHILE_FADE))
|
|
|
|
{
|
|
|
|
viewpoint_schedule(NSTEPS - INITIAL_TIME);
|
|
|
|
reset_view = 1;
|
|
|
|
}
|
2022-05-14 20:58:08 +02:00
|
|
|
draw_wave_3d(1, phi, psi, xy_in, wave, ZPLOT_B, CPLOT_B, COLOR_PALETTE_B, 0, 1.0, 1);
|
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT_B, COLORBAR_RANGE_B, COLOR_PALETTE_B, 0, 1.0);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 0, 1.0);
|
2022-04-12 19:20:18 +02:00
|
|
|
glutSwapBuffers();
|
|
|
|
|
|
|
|
if (!FADE) for (i=0; i<END_FRAMES; i++) save_frame_counter(NSTEPS + MID_FRAMES + 1 + counter + i);
|
|
|
|
else for (i=0; i<END_FRAMES; i++)
|
|
|
|
{
|
2022-06-25 15:49:37 +02:00
|
|
|
if ((ROTATE_VIEW)&&(ROTATE_VIEW_WHILE_FADE))
|
|
|
|
{
|
|
|
|
viewpoint_schedule(NSTEPS - INITIAL_TIME + i);
|
|
|
|
reset_view = 1;
|
|
|
|
}
|
2022-05-14 20:58:08 +02:00
|
|
|
fade_value = 1.0 - (double)i/(double)END_FRAMES;
|
|
|
|
draw_wave_3d(1, phi, psi, xy_in, wave, ZPLOT_B, CPLOT_B, COLOR_PALETTE_B, 1, fade_value, 0);
|
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT_B, COLORBAR_RANGE_B, COLOR_PALETTE_B, 1, fade_value);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 1, fade_value);
|
2022-04-12 19:20:18 +02:00
|
|
|
glutSwapBuffers();
|
|
|
|
save_frame_counter(NSTEPS + MID_FRAMES + 1 + counter + i);
|
|
|
|
}
|
|
|
|
}
|
|
|
|
else
|
|
|
|
{
|
|
|
|
if (!FADE) for (i=0; i<END_FRAMES; i++) save_frame_counter(NSTEPS + MID_FRAMES + 1 + counter + i);
|
|
|
|
else for (i=0; i<END_FRAMES; i++)
|
|
|
|
{
|
2023-01-22 16:49:04 +01:00
|
|
|
if ((ROTATE_VIEW)&&(ROTATE_VIEW_WHILE_FADE))
|
|
|
|
{
|
|
|
|
viewpoint_schedule(NSTEPS - INITIAL_TIME + i);
|
|
|
|
reset_view = 1;
|
|
|
|
}
|
2022-05-14 20:58:08 +02:00
|
|
|
fade_value = 1.0 - (double)i/(double)END_FRAMES;
|
|
|
|
draw_wave_3d(0, phi, psi, xy_in, wave, ZPLOT, CPLOT, COLOR_PALETTE, 1, fade_value, 0);
|
|
|
|
if (DRAW_COLOR_SCHEME) draw_color_bar_palette(CPLOT, COLORBAR_RANGE, COLOR_PALETTE, 1, fade_value);
|
2022-08-20 16:02:07 +02:00
|
|
|
if (PRINT_SPEED) print_speed_3d(speed, 1, fade_value);
|
2022-04-12 19:20:18 +02:00
|
|
|
glutSwapBuffers();
|
|
|
|
save_frame_counter(NSTEPS + 1 + counter + i);
|
|
|
|
}
|
|
|
|
}
|
|
|
|
|
|
|
|
s = system("mv wave*.tif tif_wave/");
|
|
|
|
}
|
|
|
|
|
|
|
|
free(xy_in);
|
|
|
|
free(phi);
|
|
|
|
free(psi);
|
2022-07-17 13:50:13 +02:00
|
|
|
free(tmp);
|
2023-01-22 16:49:04 +01:00
|
|
|
// free(total_energy);
|
2022-04-12 19:20:18 +02:00
|
|
|
free(color_scale);
|
|
|
|
free(tc);
|
|
|
|
free(tcc);
|
|
|
|
free(tgamma);
|
|
|
|
|
|
|
|
free(wave);
|
2022-08-20 16:02:07 +02:00
|
|
|
free(laplace);
|
|
|
|
free(laplace1);
|
|
|
|
free(laplace2);
|
2022-04-12 19:20:18 +02:00
|
|
|
|
|
|
|
|
|
|
|
if (SAVE_TIME_SERIES)
|
|
|
|
{
|
|
|
|
fclose(time_series_left);
|
|
|
|
fclose(time_series_right);
|
|
|
|
}
|
|
|
|
|
|
|
|
|
|
|
|
}
|
|
|
|
|
|
|
|
|
|
|
|
void display(void)
|
|
|
|
{
|
2022-05-14 20:58:08 +02:00
|
|
|
time_t rawtime;
|
|
|
|
struct tm * timeinfo;
|
|
|
|
|
|
|
|
time(&rawtime);
|
|
|
|
timeinfo = localtime(&rawtime);
|
|
|
|
|
2022-04-12 19:20:18 +02:00
|
|
|
glPushMatrix();
|
|
|
|
|
|
|
|
blank();
|
|
|
|
glutSwapBuffers();
|
|
|
|
blank();
|
|
|
|
glutSwapBuffers();
|
|
|
|
|
|
|
|
animation();
|
|
|
|
sleep(SLEEP2);
|
|
|
|
|
|
|
|
glPopMatrix();
|
|
|
|
|
|
|
|
glutDestroyWindow(glutGetWindow());
|
2022-05-14 20:58:08 +02:00
|
|
|
|
|
|
|
printf("Start local time and date: %s", asctime(timeinfo));
|
|
|
|
time(&rawtime);
|
|
|
|
timeinfo = localtime(&rawtime);
|
|
|
|
printf("Current local time and date: %s", asctime(timeinfo));
|
2022-04-12 19:20:18 +02:00
|
|
|
}
|
|
|
|
|
|
|
|
|
|
|
|
int main(int argc, char** argv)
|
|
|
|
{
|
|
|
|
glutInit(&argc, argv);
|
|
|
|
glutInitDisplayMode(GLUT_RGB | GLUT_DOUBLE | GLUT_DEPTH);
|
|
|
|
glutInitWindowSize(WINWIDTH,WINHEIGHT);
|
|
|
|
glutCreateWindow("Wave equation in a planar domain");
|
|
|
|
|
|
|
|
init_3d();
|
|
|
|
|
|
|
|
glutDisplayFunc(display);
|
|
|
|
|
|
|
|
glutMainLoop();
|
|
|
|
|
|
|
|
return 0;
|
|
|
|
}
|
|
|
|
|