Пример #1
0
    def setBackgroundField(self, Inc, Dec, Btot):

        Bx = Btot*np.cos(Inc/180.*np.pi)*np.sin(Dec/180.*np.pi)
        By = Btot*np.cos(Inc/180.*np.pi)*np.cos(Dec/180.*np.pi)
        Bz = -Btot*np.sin(Inc/180.*np.pi)

        self.B0 = np.r_[Bx, By, Bz]
Пример #2
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    def setBackgroundField(self, Inc, Dec, Btot):

        Bx = Btot * np.cos(Inc / 180. * np.pi) * np.sin(Dec / 180. * np.pi)
        By = Btot * np.cos(Inc / 180. * np.pi) * np.cos(Dec / 180. * np.pi)
        Bz = -Btot * np.sin(Inc / 180. * np.pi)

        self.B0 = np.r_[Bx, By, Bz]
Пример #3
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 def simpleFail(x):
     return np.sin(x), -sdiag(np.cos(x))
Пример #4
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 def simpleFunction(x):
     return np.sin(x), lambda xi: sdiag(np.cos(x)) * xi
Пример #5
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 def simplePass(x):
     return np.sin(x), sdiag(np.cos(x))
Пример #6
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 #%% Create a 2D mesh along axis of Tx end points and keep z-discretization    
 dx = np.min( [ np.min(mesh.hx), np.min(mesh.hy) ])
 nc = np.ceil(dl_len/dx)+3
 
 padx = dx*np.power(1.4,range(1,15))
 
 # Creating padding cells
 h1 = np.r_[padx[::-1], np.ones(nc)*dx , padx]
 
 # Create mesh with 0 coordinate centerer on the ginput points in cell center
 mesh2d = Mesh.TensorMesh([h1, mesh.hz], x0=(-np.sum(padx)-dx/2,mesh.x0[2]))
 
 # Create array of points for interpolating from 3D to 2D mesh
 xx = Tx[0][0,0] + mesh2d.vectorCCx * np.cos(azm)
 yy = Tx[0][1,0] + mesh2d.vectorCCx * np.sin(azm)
 zz = mesh2d.vectorCCy
 
 [XX,ZZ] = np.meshgrid(xx,zz)
 [YY,ZZ] = np.meshgrid(yy,zz)
 
 xyz2d = np.c_[mkvc(XX),mkvc(YY),mkvc(ZZ)]
 
 #plt.scatter(xx,yy,s=20,c='y')
 
 
 F = interpolation.NearestNDInterpolator(mesh.gridCC,model)
 m2D = np.reshape(F(xyz2d),[mesh2d.nCx,mesh2d.nCy]).T
 
  
 #==============================================================================
Пример #7
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 def simpleFail(x):
     return np.sin(x), -sdiag(np.cos(x))
Пример #8
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 def simpleFunction(x):
     return np.sin(x), lambda xi: sdiag(np.cos(x))*xi
Пример #9
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 def simplePass(x):
     return np.sin(x), sdiag(np.cos(x))