Merge branch 'master' of github.com:L-Nafaryus/anisotrope-cube
Merge: forgotten pull request
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commit
5ac5231574
2
.gitignore
vendored
2
.gitignore
vendored
@ -2,6 +2,8 @@ __pycache__
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build/
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logs/
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storage/
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*.gz
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*.xz
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*.fls
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*.aux
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*.bbl
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@ -59,9 +59,10 @@ class ViscousLayers(Parameters):
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##
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structures = [
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#"simple",
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#"bodyCentered",
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"bodyCentered",
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"faceCentered"
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]
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class simple:
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theta = [c * 0.01 for c in range(1, 28 + 1)]
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directions = [
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@ -138,7 +139,7 @@ class faceCentered:
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[1, 1, 1]
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]
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fillet = True
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fineness = 1
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fineness = 3
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parameters = Parameters(
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minSize = 0.005,
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maxSize = 0.05,
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@ -155,7 +156,7 @@ class faceCentered:
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checkChartBoundary = False
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)
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viscousLayers = ViscousLayers(
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thickness = 0.001,
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thickness = 0.001, # Failing on 0.13-111
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numberOfLayers = 2,
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stretchFactor = 1.2,
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isFacesToIgnore = True,
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79
extra/theta-flowrate.py
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79
extra/theta-flowrate.py
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@ -0,0 +1,79 @@
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import matplotlib.pyplot as plt
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from math import sqrt
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import sys, os
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if __name__ == "__main__":
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BUILD = "../build"
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postProcessing = "postProcessing/flowRatePatch(name=outlet)/0/surfaceFieldValue.dat"
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#structures = [
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# "simple",
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# #"bodyCentered",
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# #"faceCentered"
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#]
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theta = [c * 0.01 for c in range(1, 28 + 1)]
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directions = [
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[1, 0, 0],
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[0, 0, 1],
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[1, 1, 1]
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]
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flowrate = [ [] for n in range(3) ]
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#nu = 1e-06
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#p = [1e-03, 0]
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for num, d in enumerate(directions):
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for t in theta:
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path = os.path.join(
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BUILD,
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"simple",
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"direction-{}{}{}".format(*d),
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"theta-{}".format(t),
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postProcessing
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)
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with open(path, "r") as io:
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lastLine = io.readlines()[-1]
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value = lastLine.replace(" ", "").replace("\n", "").split("\t")[1]
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flowrate[num].append(float(value))
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k2, k3 = [], []
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for n, _ in enumerate(flowrate[0]):
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k2.append(2 * flowrate[1][n] / flowrate[0][n])
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k3.append(2 * flowrate[2][n] / flowrate[0][n])
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plt.figure(1)
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ax = plt.subplot(211)
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line, = ax.plot(theta, flowrate[0], "o")
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line.set_label("[1, 0, 0]")
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line, = ax.plot(theta, flowrate[1], "o")
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line.set_label("[0, 0, 1]")
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line, = plt.plot(theta, flowrate[2], "o")
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line.set_label("[1, 1, 1]")
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ax.set_yscale("log")
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plt.legend()
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plt.grid(True)
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plt.xlabel("theta")
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plt.ylabel("flowRate")
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ax = plt.subplot(212)
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line, = ax.plot(theta, k2, "o")
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line.set_label("k2")
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line, = ax.plot(theta, k3, "o")
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line.set_label("k3")
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plt.legend()
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plt.grid(True)
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plt.xlabel("theta")
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plt.ylabel("k")
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plt.show()
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@ -29,7 +29,8 @@ def simpleCubic(theta = 0.01, fillet = False, direction = [1, 0, 0]):
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C1, C2 = 0.8, 0.5 #0.8, 0.05
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theta1, theta2 = 0.01, 0.28
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Cf = C1 + (C2 - C1) / (theta2 - theta1) * (theta - theta1)
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filletradius = 0.2 - Cf * (radius - r0)
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delta = 0.2
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filletradius = delta - Cf * (radius - r0)
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scale = 100
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oo = geompy.MakeVertex(0, 0, 0)
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@ -168,7 +169,8 @@ def simpleHexagonalPrism(theta = 0.01, fillet = False, direction = [1, 1, 1]):
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C1, C2 = 0.8, 0.5 # 0.8, 0.05
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theta1, theta2 = 0.01, 0.28
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Cf = C1 + (C2 - C1) / (theta2 - theta1) * (theta - theta1)
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filletradius = 0.2 - Cf * (radius - r0)
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delta = 0.2
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filletradius = delta - Cf * (radius - r0)
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scale = 100
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oo = geompy.MakeVertex(0, 0, 0)
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