''' 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 MainBody(): def __init__(self, htc_filename, modelpath, body_name): self.htcfile = htcfile = HTCFile(htc_filename, modelpath) s = htcfile.new_htc_structure main_bodies = {s[k].name[0]:s[k] for k in s.keys() if s[k].name_ == "main_body"} self.main_body = main_bodies[body_name] self.stFile = StFile(os.path.join(htcfile.modelpath, self.main_body.timoschenko_input.filename[0])) self.c2def = np.array([v.values[1:5] for v in self.main_body.c2_def if v.name_ == "sec"]) self.concentrated_mass = [cm.values for cm in self.main_body if cm.name_.startswith('concentrated_mass')] def plot_xz_geometry(self, plt=None): if plt is None: import matplotlib.pyplot as plt plt.figure() plt.xlabel("z") plt.ylabel("x") z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100) plt.plot(self.c2def[:, 2], self.c2def[:, 0],'.-', label='Center line') 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') for cm in self.concentrated_mass: plt.plot(self.c2def[cm[0]-1,2]+cm[3],self.c2def[cm[0]-1,0]+cm[1],'x', label='Concentrated mass') plt.legend() def plot_yz_geometry(self, plt=None): if plt is None: import matplotlib.pyplot as plt plt.figure() plt.xlabel("z") plt.ylabel("y") z = np.linspace(self.c2def[0, 2], self.c2def[-1, 2], 100) plt.plot(self.c2def[:, 2], self.c2def[:, 1], label='Center line') 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') for cm in self.concentrated_mass: plt.plot(self.c2def[cm[0]-1,2]+cm[3],self.c2def[cm[0]-1,1]+cm[2],'x', label='Concentrated mass') plt.legend() 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 Blade(MainBody, BladeData): def __init__(self, htc_filename, modelpath=None, blade_number=1): self.htcfile = htcfile = HTCFile(htc_filename, modelpath) blade_name = [link[2] for link in htcfile.aero if link.name_.startswith('link') and link[0]==blade_number][0] MainBody.__init__(self, htc_filename, modelpath, blade_name) self.pcFile = PCFile(os.path.join(htcfile.modelpath, htcfile.aero.pc_filename[0]), os.path.join(htcfile.modelpath, htcfile.aero.ae_filename[0])) def plot_xz_geometry(self, plt=None): if plt is None: import matplotlib.pyplot as plt plt.figure() MainBody.plot_xz_geometry(self, plt) BladeData.plot_xz_geometry(self, plt=plt) plt.legend() def plot_geometry_yz(self, plt=None): if plt is None: import matplotlib.pyplot as plt plt.figure() BladeData.plot_yz_geometry(self, plt=plt) MainBody.plot_yz_geometry(self, plt)