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authorAdrian Kummerlaender2019-06-12 21:01:42 +0200
committerAdrian Kummerlaender2019-06-12 21:01:42 +0200
commit9cf82f641b8982df526107b99d883545ee02fe20 (patch)
treedb2374c187047713d19be62c4b1862b9af5065f9
parent835824b80e82f471dc7ea6d22dedf485ad44c654 (diff)
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Restructuring
-rw-r--r--D2Q9.py (renamed from codegen_lbm.py)60
-rw-r--r--implosion.py242
-rw-r--r--notebook/inspect_opencl_layout.ipynb (renamed from inspect_opencl_layout.ipynb)0
-rw-r--r--notebook/lbm_codegen.ipynb (renamed from lbm_codegen.ipynb)0
-rw-r--r--notebook/lbm_codegen_d3q19.ipynb (renamed from lbm_codegen_d3q19.ipynb)0
-rw-r--r--symbolic/D2Q9.py (renamed from lbm_d2q9.py)0
6 files changed, 38 insertions, 264 deletions
diff --git a/codegen_lbm.py b/D2Q9.py
index a71fc15..173f1b7 100644
--- a/codegen_lbm.py
+++ b/D2Q9.py
@@ -2,18 +2,13 @@ import pyopencl as cl
mf = cl.mem_flags
import numpy
-import time
-
-import matplotlib
-import matplotlib.pyplot as plt
-matplotlib.use('AGG')
import sympy
-import lbm_d2q9 as D2Q9
+import symbolic.D2Q9 as D2Q9
from mako.template import Template
-class D2Q9_BGK_Lattice:
+class Lattice:
def idx(self, x, y):
return y * self.nX + x;
@@ -79,54 +74,5 @@ class D2Q9_BGK_Lattice:
self.program.collect_moments(self.queue, (self.nX,self.nY), (32,1), self.cl_pop_b, self.cl_moments)
else:
self.program.collect_moments(self.queue, (self.nX,self.nY), (32,1), self.cl_pop_a, self.cl_moments)
- cl.enqueue_copy(LBM.queue, moments, LBM.cl_moments).wait();
+ cl.enqueue_copy(self.queue, moments, self.cl_moments).wait();
return moments
-
-
-def MLUPS(cells, steps, time):
- return cells * steps / time * 1e-6
-
-def generate_moment_plots(lattice, moments):
- for i, m in enumerate(moments):
- print("Generating plot %d of %d." % (i+1, len(moments)))
-
- density = numpy.ndarray(shape=(lattice.nY-2, lattice.nX-2))
- for y in range(1,lattice.nY-1):
- for x in range(1,lattice.nX-1):
- density[y-1,x-1] = m[0,lattice.idx(x,y)]
-
- plt.figure(figsize=(10, 10))
- plt.imshow(density, origin='lower', vmin=0.2, vmax=2.0, cmap=plt.get_cmap('seismic'))
- plt.savefig("result/density_" + str(i) + ".png", bbox_inches='tight', pad_inches=0)
-
-def box(nX, nY, x, y):
- if x == 1 or y == 1 or x == nX-2 or y == nY-2:
- return 2
- else:
- return 1
-
-nUpdates = 1000
-nStat = 100
-
-moments = []
-
-print("Initializing simulation...\n")
-
-LBM = D2Q9_BGK_Lattice(nX = 1024, nY = 1024, tau = 0.8, geometry = box)
-
-print("Starting simulation using %d cells...\n" % LBM.nCells)
-
-lastStat = time.time()
-
-for i in range(1,nUpdates+1):
- LBM.evolve()
-
- if i % nStat == 0:
- LBM.sync()
- print("i = %4d; %3.0f MLUPS" % (i, MLUPS(LBM.nCells, nStat, time.time() - lastStat)))
- moments.append(LBM.get_moments())
- lastStat = time.time()
-
-print("\nConcluded simulation.\n")
-
-generate_moment_plots(LBM, moments)
diff --git a/implosion.py b/implosion.py
index c70f21a..75e9640 100644
--- a/implosion.py
+++ b/implosion.py
@@ -1,228 +1,56 @@
-import pyopencl as cl
-mf = cl.mem_flags
-
-from string import Template
-
import numpy
-import matplotlib.pyplot as plt
-
import time
-kernel = """
-float constant w[9] = {
- 1./36., 1./9., 1./36.,
- 1./9. , 4./9., 1./9. ,
- 1./36 , 1./9., 1./36.
-};
-
-unsigned int indexOfDirection(int i, int j) {
- return (i+1) + 3*(1-j);
-}
-
-unsigned int indexOfCell(int x, int y)
-{
- return y * $nX + x;
-}
-
-unsigned int idx(int x, int y, int i, int j) {
- return indexOfDirection(i,j)*$nCells + indexOfCell(x,y);
-}
-
-__global float f_i(__global __read_only float* f, int x, int y, int i, int j) {
- return f[idx(x,y,i,j)];
-}
-
-float comp(int i, int j, float2 v) {
- return i*v.x + j*v.y;
-}
-
-float sq(float x) {
- return x*x;
-}
-
-float f_eq(float w, float d, float2 v, int i, int j, float dotv) {
- return w * d * (1.f + 3.f*comp(i,j,v) + 4.5f*sq(comp(i,j,v)) - 1.5f*dotv);
-}
-
-__kernel void collide_and_stream(__global __write_only float* f_a,
- __global __read_only float* f_b,
- __global __write_only float* moments,
- __global __read_only int* material)
-{
- const unsigned int gid = indexOfCell(get_global_id(0), get_global_id(1));
-
- const uint2 cell = (uint2)(get_global_id(0), get_global_id(1));
-
- const int m = material[gid];
-
- if ( m == 0 ) {
- return;
- }
-
- float f0 = f_i(f_b, cell.x+1, cell.y-1, -1, 1);
- float f1 = f_i(f_b, cell.x , cell.y-1, 0, 1);
- float f2 = f_i(f_b, cell.x-1, cell.y-1, 1, 1);
- float f3 = f_i(f_b, cell.x+1, cell.y , -1, 0);
- float f4 = f_i(f_b, cell.x , cell.y , 0, 0);
- float f5 = f_i(f_b, cell.x-1, cell.y , 1, 0);
- float f6 = f_i(f_b, cell.x+1, cell.y+1, -1,-1);
- float f7 = f_i(f_b, cell.x , cell.y+1, 0,-1);
- float f8 = f_i(f_b, cell.x-1, cell.y+1, 1,-1);
-
- const float d = f0 + f1 + f2 + f3 + f4 + f5 + f6 + f7 + f8;
-
- float2 v = (float2)(
- (f5 - f3 + f2 - f6 + f8 - f0) / d,
- (f1 - f7 + f2 - f6 - f8 + f0) / d
- );
-
- if ( m == 2 ) {
- v = (float2)(0.0f, 0.0f);
- }
-
- const float dotv = dot(v,v);
-
- f0 += $omega * (f_eq(w[0], d,v,-1, 1, dotv) - f0);
- f1 += $omega * (f_eq(w[1], d,v, 0, 1, dotv) - f1);
- f2 += $omega * (f_eq(w[2], d,v, 1, 1, dotv) - f2);
- f3 += $omega * (f_eq(w[3], d,v,-1, 0, dotv) - f3);
- f4 += $omega * (f_eq(w[4], d,v, 0, 0, dotv) - f4);
- f5 += $omega * (f_eq(w[5], d,v, 1, 0, dotv) - f5);
- f6 += $omega * (f_eq(w[6], d,v,-1,-1, dotv) - f6);
- f7 += $omega * (f_eq(w[7], d,v, 0,-1, dotv) - f7);
- f8 += $omega * (f_eq(w[8], d,v, 1,-1, dotv) - f8);
-
- f_a[0*$nCells + gid] = f0;
- f_a[1*$nCells + gid] = f1;
- f_a[2*$nCells + gid] = f2;
- f_a[3*$nCells + gid] = f3;
- f_a[4*$nCells + gid] = f4;
- f_a[5*$nCells + gid] = f5;
- f_a[6*$nCells + gid] = f6;
- f_a[7*$nCells + gid] = f7;
- f_a[8*$nCells + gid] = f8;
-
- moments[1*gid] = d;
- moments[2*gid] = v.x;
- moments[3*gid] = v.y;
-}"""
-
-class D2Q9_BGK_Lattice:
- def idx(self, x, y):
- return y * self.nX + x;
-
- def __init__(self, nX, nY):
- self.nX = nX
- self.nY = nY
- self.nCells = nX * nY
- self.tick = True
-
- self.platform = cl.get_platforms()[0]
- self.context = cl.Context(properties=[(cl.context_properties.PLATFORM, self.platform)])
- self.queue = cl.CommandQueue(self.context)
-
- self.np_pop_a = numpy.ndarray(shape=(9, self.nCells), dtype=numpy.float32)
- self.np_pop_b = numpy.ndarray(shape=(9, self.nCells), dtype=numpy.float32)
-
- self.np_moments = numpy.ndarray(shape=(3, self.nCells), dtype=numpy.float32)
- self.np_material = numpy.ndarray(shape=(self.nCells, 1), dtype=numpy.int32)
-
- self.setup_geometry()
-
- self.equilibrilize()
- self.setup_anomaly()
-
- self.cl_pop_a = cl.Buffer(self.context, mf.READ_WRITE | mf.USE_HOST_PTR, hostbuf=self.np_pop_a)
- self.cl_pop_b = cl.Buffer(self.context, mf.READ_WRITE | mf.USE_HOST_PTR, hostbuf=self.np_pop_b)
-
- self.cl_material = cl.Buffer(self.context, mf.READ_ONLY | mf.USE_HOST_PTR, hostbuf=self.np_material)
- self.cl_moments = cl.Buffer(self.context, mf.READ_WRITE | mf.USE_HOST_PTR, hostbuf=self.np_moments)
-
- self.build_kernel()
-
- def setup_geometry(self):
- self.np_material[:] = 0
- for x in range(1,self.nX-1):
- for y in range(1,self.nY-1):
- if x == 1 or y == 1 or x == self.nX-2 or y == self.nY-2:
- self.np_material[self.idx(x,y)] = 2
- else:
- self.np_material[self.idx(x,y)] = 1
-
- def equilibrilize(self):
- self.np_pop_a[(0,2,6,8),:] = 1./36.
- self.np_pop_a[(1,3,5,7),:] = 1./9.
- self.np_pop_a[4,:] = 4./9.
-
- self.np_pop_b[(0,2,6,8),:] = 1./36.
- self.np_pop_b[(1,3,5,7),:] = 1./9.
- self.np_pop_b[4,:] = 4./9.
-
- def setup_anomaly(self):
- bubbles = [ [ self.nX//4, self.nY//4],
- [ self.nX//4,self.nY-self.nY//4],
- [self.nX-self.nX//4, self.nY//4],
- [self.nX-self.nX//4,self.nY-self.nY//4] ]
-
- for x in range(0,self.nX-1):
- for y in range(0,self.nY-1):
- for [a,b] in bubbles:
- if numpy.sqrt((x-a)*(x-a)+(y-b)*(y-b)) < self.nX//10:
- self.np_pop_a[:,self.idx(x,y)] = 1./24.
- self.np_pop_b[:,self.idx(x,y)] = 1./24.
-
- def build_kernel(self):
- self.program = cl.Program(self.context, Template(kernel).substitute({
- 'nX' : self.nX,
- 'nY' : self.nY,
- 'nCells': self.nCells,
- 'omega': 1.0/0.8
- })).build() #'-cl-single-precision-constant -cl-fast-relaxed-math')
-
- def evolve(self):
- if self.tick:
- self.tick = False
- self.program.collide_and_stream(self.queue, (self.nX,self.nY), (64,1), self.cl_pop_a, self.cl_pop_b, self.cl_moments, self.cl_material)
- else:
- self.tick = True
- self.program.collide_and_stream(self.queue, (self.nX,self.nY), (64,1), self.cl_pop_b, self.cl_pop_a, self.cl_moments, self.cl_material)
-
- def sync(self):
- self.queue.finish()
-
- def show(self, i):
- cl.enqueue_copy(LBM.queue, LBM.np_moments, LBM.cl_moments).wait();
-
- density = numpy.ndarray(shape=(self.nX-2, self.nY-2))
- for y in range(1,self.nY-1):
- for x in range(1,self.nX-1):
- density[x-1,y-1] = self.np_moments[0,self.idx(x,y)]
-
- plt.imshow(density, vmin=0.2, vmax=2.0, cmap=plt.get_cmap("seismic"))
- plt.savefig("result/density_" + str(i) + ".png")
+import matplotlib
+import matplotlib.pyplot as plt
+matplotlib.use('AGG')
+from D2Q9 import Lattice
def MLUPS(cells, steps, time):
return cells * steps / time * 1e-6
+def generate_moment_plots(lattice, moments):
+ for i, m in enumerate(moments):
+ print("Generating plot %d of %d." % (i+1, len(moments)))
+
+ density = numpy.ndarray(shape=(lattice.nY-2, lattice.nX-2))
+ for y in range(1,lattice.nY-1):
+ for x in range(1,lattice.nX-1):
+ density[y-1,x-1] = m[0,lattice.idx(x,y)]
+
+ plt.figure(figsize=(10, 10))
+ plt.imshow(density, origin='lower', vmin=0.2, vmax=2.0, cmap=plt.get_cmap('seismic'))
+ plt.savefig("result/density_" + str(i) + ".png", bbox_inches='tight', pad_inches=0)
+
+def box(nX, nY, x, y):
+ if x == 1 or y == 1 or x == nX-2 or y == nY-2:
+ return 2
+ else:
+ return 1
+
nUpdates = 1000
-nStat = 100
+nStat = 100
+
+moments = []
print("Initializing simulation...\n")
-LBM = D2Q9_BGK_Lattice(1024, 1024)
+lattice = Lattice(nX = 1024, nY = 1024, tau = 0.8, geometry = box)
-print("Starting simulation using %d cells...\n" % LBM.nCells)
+print("Starting simulation using %d cells...\n" % lattice.nCells)
lastStat = time.time()
for i in range(1,nUpdates+1):
+ lattice.evolve()
+
if i % nStat == 0:
- LBM.sync()
- #LBM.show(i)
- print("i = %4d; %3.0f MLUPS" % (i, MLUPS(LBM.nCells, nStat, time.time() - lastStat)))
+ lattice.sync()
+ print("i = %4d; %3.0f MLUPS" % (i, MLUPS(lattice.nCells, nStat, time.time() - lastStat)))
+ moments.append(lattice.get_moments())
lastStat = time.time()
- LBM.evolve()
+print("\nConcluded simulation.\n")
-LBM.show(nUpdates)
+generate_moment_plots(lattice, moments)
diff --git a/inspect_opencl_layout.ipynb b/notebook/inspect_opencl_layout.ipynb
index 521f93a..521f93a 100644
--- a/inspect_opencl_layout.ipynb
+++ b/notebook/inspect_opencl_layout.ipynb
diff --git a/lbm_codegen.ipynb b/notebook/lbm_codegen.ipynb
index e1593c0..e1593c0 100644
--- a/lbm_codegen.ipynb
+++ b/notebook/lbm_codegen.ipynb
diff --git a/lbm_codegen_d3q19.ipynb b/notebook/lbm_codegen_d3q19.ipynb
index face58f..face58f 100644
--- a/lbm_codegen_d3q19.ipynb
+++ b/notebook/lbm_codegen_d3q19.ipynb
diff --git a/lbm_d2q9.py b/symbolic/D2Q9.py
index a3c2503..a3c2503 100644
--- a/lbm_d2q9.py
+++ b/symbolic/D2Q9.py