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Commit 724f70d6 authored by Mads M. Pedersen's avatar Mads M. Pedersen
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Added bladeData.py + test

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'''
Created on 01/08/2016
@author: MMPE
'''
from wetb.hawc2.pc_file import PCFile
from wetb.hawc2.ae_file import AEFile
from wetb.hawc2.htc_file import HTCFile
import os
import numpy as np
from wetb.hawc2.st_file import StFile
class BladeData(object):
def plot_xz_geometry(self, plt):
z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100)
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 0]), label='Center line')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 0]) + self.pcFile.chord(z) / 2, label='Leading edge')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 0]) - self.pcFile.chord(z) / 2, label="Trailing edge")
x, y, z = self.hawc2_splines()
#plt.plot(z, x, label='Hawc2spline')
def plot_yz_geometry(self, plt):
z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100)
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 1]), label='Center line')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 1]) + self.pcFile.thickness(z) / 100 * self.pcFile.chord(z) / 2, label='Suction side')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 1]) - self.pcFile.thickness(z) / 100 * self.pcFile.chord(z) / 2, label="Pressure side")
x, y, z = self.hawc2_splines()
#plt.plot(z, y, label='Hawc2spline')
def hawc2_splines(self):
curve_z = np.r_[0, np.cumsum(np.sqrt(np.sum(np.diff(self.c2def[:, :3], 1, 0) ** 2, 1)))]
curve_z_nd = curve_z / curve_z[-1]
def akima(x, y):
n = len(x)
var = np.zeros((n + 3))
z = np.zeros((n))
co = np.zeros((n, 4))
for i in range(n - 1):
var[i + 2] = (y[i + 1] - y[i]) / (x[i + 1] - x[i])
var[n + 1] = 2 * var[n] - var[n - 1]
var[n + 2] = 2 * var[n + 1] - var[n]
var[1] = 2 * var[2] - var[3]
var[0] = 2 * var[1] - var[2]
for i in range(n):
wi1 = abs(var[i + 3] - var[i + 2])
wi = abs(var[i + 1] - var[i])
if (wi1 + wi) == 0:
z[i] = (var[i + 2] + var[i + 1]) / 2
else:
z[i] = (wi1 * var[i + 1] + wi * var[i + 2]) / (wi1 + wi)
for i in range(n - 1):
dx = x[i + 1] - x[i]
a = (z[i + 1] - z[i]) * dx
b = y[i + 1] - y[i] - z[i] * dx
co[i, 0] = y[i]
co[i, 1] = z[i]
co[i, 2] = (3 * var[i + 2] - 2 * z[i] - z[i + 1]) / dx
co[i, 3] = (z[i] + z[i + 1] - 2 * var[i + 2]) / dx ** 2
co[n - 1, 0] = y[n - 1]
co[n - 1, 1] = z[n - 1]
co[n - 1, 2] = 0
co[n - 1, 3] = 0
return co
def coef2spline(s, co):
x, y = [], []
for i, c in enumerate(co.tolist()[:-1]):
p = np.poly1d(c[::-1])
z = np.linspace(0, s[i + 1] - s[i ], 10)
x.extend(s[i] + z)
y.extend(p(z))
return y
x, y, z = [coef2spline(curve_z_nd, akima(curve_z_nd, self.c2def[:, i])) for i in range(3)]
return x, y, z
class H2BladeData(BladeData):
def __init__(self, htc_filename, modelpath):
self.htcfile = htcfile = HTCFile(htc_filename, modelpath)
self.pcFile = PCFile(os.path.join(htcfile.modelpath, htcfile.aero.pc_filename[0]),
os.path.join(htcfile.modelpath, htcfile.aero.ae_filename[0]))
s = htcfile.new_htc_structure
blade_name = htcfile.aero.link[2]
mainbodies = [s[k] for k in s.keys() if s[k].name_ == "main_body"]
blade_main_body = [mb for mb in mainbodies if mb.name[0] == blade_name][0]
self.stFile = StFile(os.path.join(htcfile.modelpath, blade_main_body.timoschenko_input.filename[0]))
self.c2def = np.array([v.values[1:5] for v in blade_main_body.c2_def if v.name_ == "sec"])
def plot_geometry(self, plt=None):
if plt is None:
import matplotlib.pyplot as plt
BladeData.plot_xz_geometry(self, plt=plt)
z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100)
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 0]) + self.stFile.x_e(z), label='Elastic center')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 0]) + self.stFile.x_cg(z), label='Mass center')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 0]) + self.stFile.x_sh(z), label='Shear center')
plt.legend()
plt.figure()
BladeData.plot_yz_geometry(self, plt=plt)
z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100)
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 1]) + self.stFile.y_e(z), label='Elastic center')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 1]) + self.stFile.y_cg(z), label='Mass center')
plt.plot(z, np.interp(z, self.c2def[:, 2], self.c2def[:, 1]) + self.stFile.y_sh(z), label='Shear center')
plt.legend()
plt.show()
class H2AeroBladeData(BladeData):
def __init__(self, htc_filename, modelpath):
self.htcfile = htcfile = HTCFile(htc_filename, modelpath)
self.pcFile = PCFile(os.path.join(htcfile.modelpath, htcfile.aero.pc_filename[0]),
os.path.join(htcfile.modelpath, htcfile.aero.ae_filename[0]))
self.c2def = np.array([v.values[1:5] for v in htcfile.blade_c2_def if v.name_ == "sec"])
def plot_geometry(self, plt=None):
if plt is None:
import matplotlib.pyplot as plt
BladeData.plot_xz_geometry(self, plt=plt)
z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100)
plt.legend()
plt.figure()
BladeData.plot_yz_geometry(self, plt=plt)
z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100)
plt.legend()
plt.show()
'''
Created on 01/08/2016
@author: MMPE
'''
import unittest
import os
from wetb.hawc2.bladeData import H2AeroBladeData, H2BladeData
tfp = os.path.join(os.path.dirname(__file__), 'test_files/') # test file path
class TestBladeData(unittest.TestCase):
def testBladedata(self):
#bd = H2AeroBladeData(tfp + "h2aero_tb/htc/h2aero.htc", '../')
#bd = H2AeroBladeData(r'C:\mmpe\programming\python\Phd\pitot_tube\tests\test_files\swt36_107\h2a\htc\templates/swt3.6_107.htc', "../../")
#print (bd.pcFile.chord(36))
#bd = H2BladeData(r"C:\mmpe\HAWC2\models\SWT3.6-107\original_data\SWT4.0-130\dlc12_wsp06_wdir010_s18002.htc", ".")
bd = H2BladeData(r"C:\mmpe\HAWC2\models\SWT3.6-107\htc/stat6/stat6_10.0_0.htc", "../../")
#bd = H2BladeData(r"C:\mmpe\HAWC2\models\NREL 5MW reference wind turbine_play/htc/NREL_5MW_reference_wind_turbine_heli_step.htc", "../")
if 1:
bd.plot_geometry()
if __name__ == "__main__":
#import sys;sys.argv = ['', 'Test.testBladedata']
unittest.main()
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