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1 | 145 | equemene | #!/usr/bin/env python
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2 | 145 | equemene | #
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3 | 145 | equemene | # Ising2D model using PyOpenCL
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4 | 145 | equemene | #
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5 | 145 | equemene | # CC BY-NC-SA 2011 : <emmanuel.quemener@ens-lyon.fr>
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6 | 145 | equemene | #
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7 | 145 | equemene | # Thanks to Andreas Klockner for PyOpenCL:
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8 | 145 | equemene | # http://mathema.tician.de/software/pyopencl
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9 | 145 | equemene | #
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10 | 145 | equemene | # Interesting links:
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11 | 145 | equemene | # http://viennacl.sourceforge.net/viennacl-documentation.html
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12 | 145 | equemene | # http://enja.org/2011/02/22/adventures-in-pyopencl-part-1-getting-started-with-python/
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13 | 145 | equemene | |
14 | 145 | equemene | import pyopencl as cl |
15 | 145 | equemene | import numpy |
16 | 145 | equemene | from PIL import Image |
17 | 145 | equemene | import time,string |
18 | 145 | equemene | from numpy.random import randint as nprnd |
19 | 145 | equemene | import sys |
20 | 145 | equemene | import getopt |
21 | 145 | equemene | import matplotlib.pyplot as plt |
22 | 145 | equemene | |
23 | 145 | equemene | # Size of micro blocks
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24 | 145 | equemene | BSZ=16
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25 | 145 | equemene | |
26 | 145 | equemene | # 2097152 on HD5850 (with 1GB of RAM)
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27 | 145 | equemene | # 262144 on GT218
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28 | 145 | equemene | #STEP=262144
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29 | 145 | equemene | #STEP=1048576
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30 | 145 | equemene | #STEP=2097152
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31 | 145 | equemene | #STEP=4194304
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32 | 145 | equemene | #STEP=8388608
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33 | 145 | equemene | STEP=16777216
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34 | 145 | equemene | #STEP=268435456
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35 | 145 | equemene | |
36 | 145 | equemene | # Flag to define LAPIMAGE between iteration on OpenCL kernel calls
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37 | 145 | equemene | #LAPIMAGE=True
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38 | 145 | equemene | LAPIMAGE=False
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39 | 145 | equemene | |
40 | 145 | equemene | # Version 2 of kernel : much optimize one
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41 | 145 | equemene | # a string template is used to replace BSZ (named $block_size) by its value
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42 | 145 | equemene | KERNEL_CODE_ORIG=string.Template("""
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43 | 145 | equemene | #define BSZ $block_size
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44 | 145 | equemene |
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45 | 145 | equemene | /* Marsaglia RNG very simple implementation */
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46 | 145 | equemene | #define znew (z=36969*(z&65535)+(z>>16))
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47 | 145 | equemene | #define wnew (w=18000*(w&65535)+(w>>16))
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48 | 145 | equemene | #define MWC ((znew<<16)+wnew )
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49 | 145 | equemene | #define MWCfp (float)(MWC * 2.328306435454494e-10f)
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50 | 145 | equemene |
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51 | 145 | equemene | __kernel void MainLoop(__global int *s,float J,float B,float T,uint size,
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52 | 145 | equemene | uint iterations,uint seed_w,uint seed_z)
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53 | 145 | equemene | {
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54 | 145 | equemene | uint base_idx=(uint)(BSZ*get_global_id(0));
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55 | 145 | equemene | uint base_idy=(uint)(BSZ*get_global_id(1));
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56 | 145 | equemene | uint base_id=base_idx+base_idy*size;
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57 | 145 | equemene |
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58 | 145 | equemene | uint z=seed_z+(uint)get_global_id(0);
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59 | 145 | equemene | uint w=seed_w+(uint)get_global_id(1);
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60 | 145 | equemene |
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61 | 145 | equemene | for (uint i=0;i<iterations;i++)
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62 | 145 | equemene | {
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63 | 145 | equemene | uint x=(uint)(MWC%BSZ);
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64 | 145 | equemene | uint y=(uint)(MWC%BSZ);
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65 | 145 | equemene |
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66 | 145 | equemene | int p=s[base_id+x+size*y];
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67 | 145 | equemene |
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68 | 145 | equemene | int u=s[((base_idx+x)%size)+size*((base_idy+y-1)%size)];
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69 | 145 | equemene | int d=s[((base_idx+x)%size)+size*((base_idy+y+1)%size)];
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70 | 145 | equemene | int l=s[((base_idx+x-1)%size)+size*((base_idy+y)%size)];
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71 | 145 | equemene | int r=s[((base_idx+x+1)%size)+size*((base_idy+y)%size)];
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72 | 145 | equemene |
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73 | 145 | equemene | float DeltaE=p*(2.0f*J*(float)(u+d+l+r)+B);
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74 | 145 | equemene |
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75 | 145 | equemene | float factor= ((DeltaE < 0.0f) || (MWCfp < exp(-DeltaE/T))) ? -1:1;
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76 | 145 | equemene |
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77 | 145 | equemene | s[base_id+x+size*y]= factor*p;
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78 | 145 | equemene | }
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79 | 145 | equemene |
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80 | 145 | equemene | }
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81 | 145 | equemene | """)
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82 | 145 | equemene | |
83 | 145 | equemene | # Version 2 of kernel : much optimize one
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84 | 145 | equemene | # a string template is used to replace BSZ (named $block_size) by its value
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85 | 145 | equemene | KERNEL_CODE=string.Template("""
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86 | 145 | equemene | #define BSZ $block_size
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87 | 145 | equemene |
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88 | 145 | equemene | /* Marsaglia RNG very simple implementation */
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89 | 145 | equemene | #define znew (z=36969*(z&65535)+(z>>16))
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90 | 145 | equemene | #define wnew (w=18000*(w&65535)+(w>>16))
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91 | 145 | equemene | #define MWC ((znew<<16)+wnew )
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92 | 145 | equemene | #define MWCfp (float)(MWC * 2.328306435454494e-10f)
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93 | 145 | equemene |
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94 | 145 | equemene | __kernel void MainLoop(__global int *s,float J,float B,float T,uint size,
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95 | 145 | equemene | uint iterations,uint seed_w,uint seed_z)
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96 | 145 | equemene | {
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97 | 145 | equemene | private uint z=seed_z+(uint)get_global_id(0);
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98 | 145 | equemene | private uint w=seed_w+(uint)get_global_id(1);
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99 | 145 | equemene |
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100 | 145 | equemene | private uint x,y,base,size2;
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101 | 145 | equemene | private int p,u,d,l,r,factor;
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102 | 145 | equemene | private float DeltaE;
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103 | 145 | equemene |
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104 | 145 | equemene | for (uint i=0;i<iterations/2;i++)
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105 | 145 | equemene | {
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106 | 145 | equemene | // Odd pixel
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107 | 145 | equemene | base=2*(uint)get_global_id(0);
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108 | 145 | equemene |
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109 | 145 | equemene | x=base%size;
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110 | 145 | equemene | y=base/size;
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111 | 145 | equemene |
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112 | 145 | equemene | p=s[base];
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113 | 145 | equemene |
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114 | 145 | equemene | u= (y== 0) ? s[x+size*(size-1)]:s[base-size];
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115 | 145 | equemene | d= (y==size-1) ? s[x]:s[base+size];
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116 | 145 | equemene | l= (x== 0) ? s[y*size+size-1]:s[base-1];
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117 | 145 | equemene | r= (x==size-1) ? s[y*size]:s[base+1];
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118 | 145 | equemene |
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119 | 145 | equemene | DeltaE=p*(2e0f*J*(float)(u+d+l+r)+B);
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120 | 145 | equemene |
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121 | 145 | equemene | factor= ((DeltaE < 0e0f) || (MWCfp < exp(-DeltaE/T))) ? -1:1;
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122 | 145 | equemene |
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123 | 145 | equemene | s[base]= factor*p;
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124 | 145 | equemene | barrier(CLK_GLOBAL_MEM_FENCE);
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125 | 145 | equemene |
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126 | 145 | equemene | // Even pixel
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127 | 145 | equemene |
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128 | 145 | equemene | base=2*(uint)get_global_id(0)+1;
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129 | 145 | equemene |
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130 | 145 | equemene | x=base%size;
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131 | 145 | equemene | y=base/size;
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132 | 145 | equemene |
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133 | 145 | equemene | p=s[base];
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134 | 145 | equemene | u= (y== 0) ? s[x+size*(size-1)]:s[base-size];
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135 | 145 | equemene | d= (y==size-1) ? s[x]:s[base+size];
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136 | 145 | equemene | l= (x== 0) ? s[y*size+size-1]:s[base-1];
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137 | 145 | equemene | r= (x==size-1) ? s[y*size]:s[base+1];
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138 | 145 | equemene |
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139 | 145 | equemene | DeltaE=p*(2e0f*J*(float)(u+d+l+r)+B);
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140 | 145 | equemene |
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141 | 145 | equemene | factor= ((DeltaE < 0e0f) || (MWCfp < exp(-DeltaE/T))) ? -1:1;
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142 | 145 | equemene |
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143 | 145 | equemene | s[base]= factor*p;
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144 | 145 | equemene | barrier(CLK_GLOBAL_MEM_FENCE);
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145 | 145 | equemene | }
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146 | 145 | equemene |
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147 | 145 | equemene | }
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148 | 145 | equemene | """)
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149 | 145 | equemene | |
150 | 145 | equemene | def ImageOutput(sigma,prefix): |
151 | 145 | equemene | Max=sigma.max() |
152 | 145 | equemene | Min=sigma.min() |
153 | 145 | equemene | |
154 | 145 | equemene | # Normalize value as 8bits Integer
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155 | 145 | equemene | SigmaInt=(255*(sigma-Min)/(Max-Min)).astype('uint8') |
156 | 145 | equemene | image = Image.fromarray(SigmaInt) |
157 | 145 | equemene | image.save("%s.jpg" % prefix)
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158 | 145 | equemene | |
159 | 145 | equemene | def CheckLattice(sigma): |
160 | 145 | equemene | |
161 | 145 | equemene | over=sigma[sigma>1]
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162 | 145 | equemene | under=sigma[sigma<-1]
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163 | 145 | equemene | |
164 | 145 | equemene | if (over.size+under.size) > 0: |
165 | 145 | equemene | print "Problem on Lattice on %i spin(s)." % (over.size+under.size) |
166 | 145 | equemene | else:
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167 | 145 | equemene | print "No problem on Lattice" |
168 | 145 | equemene | |
169 | 145 | equemene | def Metropolis(sigma,J,B,T,iterations,Device,Divider): |
170 | 145 | equemene | |
171 | 145 | equemene | kernel_params = {'block_size':sigma.shape[0]/Divider} |
172 | 145 | equemene | |
173 | 145 | equemene | # Je detecte un peripherique GPU dans la liste des peripheriques
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174 | 145 | equemene | Id=1
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175 | 145 | equemene | HasXPU=False
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176 | 145 | equemene | for platform in cl.get_platforms(): |
177 | 145 | equemene | for device in platform.get_devices(): |
178 | 145 | equemene | if Id==Device:
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179 | 145 | equemene | XPU=device |
180 | 145 | equemene | print "CPU/GPU selected: ",device.name.lstrip() |
181 | 145 | equemene | HasXPU=True
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182 | 145 | equemene | Id+=1
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183 | 145 | equemene | |
184 | 145 | equemene | if HasXPU==False: |
185 | 145 | equemene | print "No XPU #%i found in all of %i devices, sorry..." % (Device,Id-1) |
186 | 145 | equemene | sys.exit() |
187 | 145 | equemene | |
188 | 145 | equemene | ctx = cl.Context([XPU]) |
189 | 145 | equemene | queue = cl.CommandQueue(ctx, |
190 | 145 | equemene | properties=cl.command_queue_properties.PROFILING_ENABLE) |
191 | 145 | equemene | |
192 | 145 | equemene | # Je recupere les flag possibles pour les buffers
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193 | 145 | equemene | mf = cl.mem_flags |
194 | 145 | equemene | |
195 | 145 | equemene | sigmaCL = cl.Buffer(ctx, mf.WRITE_ONLY | mf.COPY_HOST_PTR, hostbuf=sigma) |
196 | 145 | equemene | #sigmaCL = cl.Buffer(ctx, mf.READ_WRITE, sigma.nbytes)
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197 | 145 | equemene | # Program based on Kernel2
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198 | 145 | equemene | MetropolisCL = cl.Program(ctx,KERNEL_CODE.substitute(kernel_params)).build() |
199 | 145 | equemene | |
200 | 145 | equemene | divide=Divider*Divider |
201 | 145 | equemene | step=STEP/divide |
202 | 145 | equemene | i=0
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203 | 145 | equemene | duration=0.
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204 | 145 | equemene | while (step*i < iterations/divide):
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205 | 145 | equemene | |
206 | 145 | equemene | # Call OpenCL kernel
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207 | 145 | equemene | # sigmaCL is lattice translated in CL format
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208 | 145 | equemene | # step is number of iterations
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209 | 145 | equemene | |
210 | 145 | equemene | start_time=time.time() |
211 | 145 | equemene | |
212 | 145 | equemene | CLLaunch=MetropolisCL.MainLoop(queue, |
213 | 145 | equemene | (numpy.int32(sigma.shape[0]*sigma.shape[1]/2),1),None, |
214 | 145 | equemene | sigmaCL, |
215 | 145 | equemene | numpy.float32(J),numpy.float32(B), |
216 | 145 | equemene | numpy.float32(T), |
217 | 145 | equemene | numpy.uint32(sigma.shape[0]),
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218 | 145 | equemene | numpy.uint32(step), |
219 | 145 | equemene | numpy.uint32(2008),
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220 | 145 | equemene | numpy.uint32(1010))
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221 | 145 | equemene | |
222 | 145 | equemene | CLLaunch.wait() |
223 | 145 | equemene | # elapsed = 1e-9*(CLLaunch.profile.end - CLLaunch.profile.start)
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224 | 145 | equemene | elapsed = time.time()-start_time |
225 | 145 | equemene | print "Iteration %i with T=%f and %i iterations in %f: " % (i,T,step,elapsed) |
226 | 145 | equemene | if LAPIMAGE:
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227 | 145 | equemene | cl.enqueue_copy(queue, sigma, sigmaCL).wait() |
228 | 145 | equemene | checkLattice(sigma) |
229 | 145 | equemene | ImageOutput(sigma,"Ising2D_GPU_OddEven_%i_%1.1f_%.3i_Lap" % (SIZE,T,i))
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230 | 145 | equemene | i=i+1
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231 | 145 | equemene | duration=duration+elapsed |
232 | 145 | equemene | |
233 | 145 | equemene | cl.enqueue_copy(queue, sigma,sigmaCL).wait() |
234 | 145 | equemene | CheckLattice(sigma) |
235 | 145 | equemene | sigmaCL.release() |
236 | 145 | equemene | |
237 | 145 | equemene | return(duration)
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238 | 145 | equemene | |
239 | 145 | equemene | def Magnetization(sigma,M): |
240 | 145 | equemene | return(numpy.sum(sigma)/(sigma.shape[0]*sigma.shape[1]*1.0)) |
241 | 145 | equemene | |
242 | 145 | equemene | def Energy(sigma,J,B): |
243 | 145 | equemene | # Copy & Cast values
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244 | 145 | equemene | E=numpy.copy(sigma).astype(numpy.float32) |
245 | 145 | equemene | |
246 | 145 | equemene | # Slice call to estimate Energy
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247 | 145 | equemene | E[1:-1,1:-1]=E[1:-1,1:-1]*(2.0*J*(E[:-2,1:-1]+E[2:,1:-1]+ |
248 | 145 | equemene | E[1:-1,:-2]+E[1:-1,2:])+B) |
249 | 145 | equemene | |
250 | 145 | equemene | # Clean perimeter
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251 | 145 | equemene | E[:,0]=0 |
252 | 145 | equemene | E[:,-1]=0 |
253 | 145 | equemene | E[0,:]=0 |
254 | 145 | equemene | E[-1,:]=0 |
255 | 145 | equemene | |
256 | 145 | equemene | Energy=numpy.sum(E) |
257 | 145 | equemene | |
258 | 145 | equemene | return(Energy/(E.shape[0]*E.shape[1]*1.0)) |
259 | 145 | equemene | |
260 | 145 | equemene | def CriticalT(T,E): |
261 | 145 | equemene | |
262 | 145 | equemene | Epoly=numpy.poly1d(numpy.polyfit(T,E,T.size/3))
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263 | 145 | equemene | dEpoly=numpy.diff(Epoly(T)) |
264 | 145 | equemene | dEpoly=numpy.insert(dEpoly,0,0) |
265 | 145 | equemene | return(T[numpy.argmin(dEpoly)])
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266 | 145 | equemene | |
267 | 145 | equemene | def PolyFitE(T,E): |
268 | 145 | equemene | |
269 | 145 | equemene | Epoly=numpy.poly1d(numpy.polyfit(T,E,T.size/3))
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270 | 145 | equemene | return(Epoly(T))
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271 | 145 | equemene | |
272 | 145 | equemene | def DisplayCurves(T,E,M,J,B): |
273 | 145 | equemene | |
274 | 145 | equemene | plt.xlabel("Temperature")
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275 | 145 | equemene | plt.ylabel("Energy")
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276 | 145 | equemene | |
277 | 145 | equemene | Experience,=plt.plot(T,E,label="Energy")
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278 | 145 | equemene | |
279 | 145 | equemene | plt.legend() |
280 | 145 | equemene | plt.show() |
281 | 145 | equemene | |
282 | 145 | equemene | if __name__=='__main__': |
283 | 145 | equemene | |
284 | 145 | equemene | # Set defaults values
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285 | 145 | equemene | # Coupling factor
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286 | 145 | equemene | J=1.
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287 | 145 | equemene | # External Magnetic Field is null
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288 | 145 | equemene | B=0.
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289 | 145 | equemene | # Size of Lattice
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290 | 145 | equemene | Size=256
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291 | 145 | equemene | # Default Temperatures (start, end, step)
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292 | 145 | equemene | Tmin=0.1
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293 | 145 | equemene | Tmax=5
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294 | 145 | equemene | Tstep=0.1
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295 | 145 | equemene | # Default Number of Iterations
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296 | 145 | equemene | Iterations=Size*Size |
297 | 145 | equemene | # Default Device is first one
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298 | 145 | equemene | Device=1
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299 | 145 | equemene | # Default Divider
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300 | 145 | equemene | Divider=Size/16
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301 | 145 | equemene | |
302 | 145 | equemene | # Curves is True to print the curves
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303 | 145 | equemene | Curves=False
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304 | 145 | equemene | |
305 | 145 | equemene | OCL_vendor={} |
306 | 145 | equemene | OCL_type={} |
307 | 145 | equemene | OCL_description={} |
308 | 145 | equemene | |
309 | 145 | equemene | try:
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310 | 145 | equemene | import pyopencl as cl |
311 | 145 | equemene | |
312 | 145 | equemene | print "\nHere are available OpenCL devices:" |
313 | 145 | equemene | Id=1
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314 | 145 | equemene | for platform in cl.get_platforms(): |
315 | 145 | equemene | for device in platform.get_devices(): |
316 | 145 | equemene | OCL_vendor[Id]=platform.vendor.lstrip().rstrip() |
317 | 145 | equemene | #OCL_type[Id]=cl.device_type.to_string(device.type)
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318 | 145 | equemene | OCL_type[Id]="xPU"
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319 | 145 | equemene | OCL_description[Id]=device.name.lstrip().rstrip() |
320 | 145 | equemene | print "* Device #%i from %s of type %s : %s" % (Id,OCL_vendor[Id],OCL_type[Id],OCL_description[Id]) |
321 | 145 | equemene | Id=Id+1
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322 | 145 | equemene | OCL_MaxDevice=Id-1
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323 | 145 | equemene | print
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324 | 145 | equemene | |
325 | 145 | equemene | except ImportError: |
326 | 145 | equemene | print "Your platform does not seem to support OpenCL" |
327 | 145 | equemene | sys.exit(0)
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328 | 145 | equemene | |
329 | 145 | equemene | try:
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330 | 145 | equemene | opts, args = getopt.getopt(sys.argv[1:],"hcj:b:z:i:s:e:p:d:v:",["coupling=","magneticfield=","size=","iterations=","tempstart=","tempend=","tempstep=","units",'device=']) |
331 | 145 | equemene | except getopt.GetoptError:
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332 | 145 | equemene | print '%s -d <Device Id> -j <Coupling Factor> -b <Magnetic Field> -z <Size of Square Lattice> -i <Iterations> -s <Minimum Temperature> -e <Maximum Temperature> -p <steP Temperature> -v <diVider> -c (Print Curves)' % sys.argv[0] |
333 | 145 | equemene | sys.exit(2)
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334 | 145 | equemene | |
335 | 145 | equemene | for opt, arg in opts: |
336 | 145 | equemene | if opt == '-h': |
337 | 145 | equemene | print '%s -d <Device Id> -j <Coupling Factor> -b <Magnetic Field> -z <Size of Square Lattice> -i <Iterations> -s <Minimum Temperature> -e <Maximum Temperature> -p <steP Temperature> -v <diVider> -c (Print Curves)' % sys.argv[0] |
338 | 145 | equemene | sys.exit() |
339 | 145 | equemene | elif opt == '-c': |
340 | 145 | equemene | Curves=True
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341 | 145 | equemene | elif opt in ("-d", "--device"): |
342 | 145 | equemene | Device = int(arg)
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343 | 145 | equemene | if Device>OCL_MaxDevice:
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344 | 145 | equemene | "Device #%s seems not to be available !"
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345 | 145 | equemene | sys.exit() |
346 | 145 | equemene | elif opt in ("-j", "--coupling"): |
347 | 145 | equemene | J = float(arg)
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348 | 145 | equemene | elif opt in ("-b", "--magneticfield"): |
349 | 145 | equemene | B = float(arg)
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350 | 145 | equemene | elif opt in ("-s", "--tempmin"): |
351 | 145 | equemene | Tmin = float(arg)
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352 | 145 | equemene | elif opt in ("-e", "--tempmax"): |
353 | 145 | equemene | Tmax = arg |
354 | 145 | equemene | elif opt in ("-p", "--tempstep"): |
355 | 145 | equemene | Tstep = numpy.uint32(arg) |
356 | 145 | equemene | elif opt in ("-i", "--iterations"): |
357 | 145 | equemene | Iterations = int(arg)
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358 | 145 | equemene | elif opt in ("-z", "--size"): |
359 | 145 | equemene | Size = int(arg)
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360 | 145 | equemene | elif opt in ("-v", "--divider"): |
361 | 145 | equemene | Divider = int(arg)
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362 | 145 | equemene | |
363 | 145 | equemene | print "Here are parameters of simulation:" |
364 | 145 | equemene | print "* Device selected #%s: %s of type %s from %s" % (Device,OCL_description[Device],OCL_type[Device],OCL_vendor[Device]) |
365 | 145 | equemene | print "* Coupling Factor J : %s" % J |
366 | 145 | equemene | print "* Magnetic Field B : %s" % B |
367 | 145 | equemene | print "* Size of lattice : %sx%s" % (Size,Size) |
368 | 145 | equemene | print "* Parallel computing : %sx%s" % (Divider,Divider) |
369 | 145 | equemene | print "* Iterations : %s" % Iterations |
370 | 145 | equemene | print "* Temperatures from %s to %s by %s" % (Tmin,Tmax,Tstep) |
371 | 145 | equemene | |
372 | 145 | equemene | LAPIMAGE=False
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373 | 145 | equemene | |
374 | 145 | equemene | if Iterations<STEP:
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375 | 145 | equemene | STEP=Iterations |
376 | 145 | equemene | |
377 | 145 | equemene | sigmaIn=numpy.where(numpy.random.randn(Size,Size)>0,1,-1).astype(numpy.int32) |
378 | 145 | equemene | |
379 | 145 | equemene | ImageOutput(sigmaIn,"Ising2D_GPU_Local_%i_Initial" % (Size))
|
380 | 145 | equemene | |
381 | 145 | equemene | |
382 | 145 | equemene | Trange=numpy.arange(Tmin,Tmax+Tstep,Tstep) |
383 | 145 | equemene | |
384 | 145 | equemene | E=[] |
385 | 145 | equemene | M=[] |
386 | 145 | equemene | |
387 | 145 | equemene | for T in Trange: |
388 | 145 | equemene | sigma=numpy.copy(sigmaIn) |
389 | 145 | equemene | duration=Metropolis(sigma,J,B,T,Iterations,Device,Divider) |
390 | 145 | equemene | E=numpy.append(E,Energy(sigma,J,B)) |
391 | 145 | equemene | M=numpy.append(M,Magnetization(sigma,B)) |
392 | 145 | equemene | ImageOutput(sigma,"Ising2D_GPU_OddEven_%i_%1.1f_Final" % (Size,T))
|
393 | 145 | equemene | print "GPU/CPU Time : %f" % (duration) |
394 | 145 | equemene | print "Total Energy at Temperature %f : %f" % (T,E[-1]) |
395 | 145 | equemene | print "Total Magnetization at Temperature %f : %f" % (T,M[-1]) |
396 | 145 | equemene | |
397 | 145 | equemene | # Save output
|
398 | 145 | equemene | numpy.savez("Ising2D_GPU_Global_%i_%.8i" % (Size,Iterations),(Trange,E,M))
|
399 | 145 | equemene | |
400 | 145 | equemene | # Estimate Critical temperature
|
401 | 145 | equemene | print "The critical temperature on %ix%i lattice with J=%f, B=%f is %f " % (Size,Size,J,B,CriticalT(Trange,E)) |
402 | 145 | equemene | |
403 | 145 | equemene | if Curves:
|
404 | 145 | equemene | DisplayCurves(Trange,E,M,J,B) |
405 | 145 | equemene |