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Various Symbolic calculation for Physical Consistency
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from sympy import * | |
from sympy.matrices import * | |
x1, y1, x2, y2, x3, y3, x4, y4 = symbols('x1 y1 x2 y2 x3 y3 x4 y4'); | |
r1 = x1*x1+y1*y1; | |
r2 = x2*x2+y2*y2; | |
r3 = x3*x3+y3*y3; | |
r4 = x4*x4+y4*y4; | |
#A = Matrix([1,1,1,1],[x1,x2,x3,x4],[y1,y2,y3,y4],[r1,r2,r3,r4]); | |
A = eye(4); | |
A[0,0] = A[0,1] = A[0,2] = A[0,3] = 1; | |
A[1,0] = x1; | |
A[1,1] = x2; | |
A[1,2] = x3; | |
A[1,3] = x4; | |
A[2,0] = y1; | |
A[2,1] = y2; | |
A[2,2] = y3; | |
A[2,3] = y4; | |
A[3,0] = r1; | |
A[3,1] = r2; | |
A[3,2] = r3; | |
A[3,3] = r4; | |
I = eye(3); | |
Ixx, Iyy, Izz = symbols('Ixx Iyy Izz') | |
r, p, y = symbols('r p y') | |
R = rot_axis1(r)*rot_axis2(p)*rot_axis3(y); | |
I[0,0] = Ixx | |
I[1,1] = Iyy | |
I[2,2] = Izz | |
rI = R*I*R.transpose(); | |
Ixy, Ixz, Iyz = symbols('Ixy Ixz Iyz') | |
I[1,0] = I[0,1] = Ixy; | |
I[2,0] = I[0,2] = Ixz; | |
I[2,1] = I[1,2] = Iyz; | |
#cholesky decomposition | |
l00, l10, l11, l20, l21, l22 = symbols('l00 l10 l11 l20 l21 l22'); | |
L = eye(3); | |
L[0,0] = l00; | |
L[1,0] = l10; | |
L[1,1] = l11; | |
L[2,0] = l20; | |
L[2,1] = l21; | |
L[2,2] = l22; | |
L*L.transpose(); | |
#beyer 1987 | |
Ib = I; | |
Ib[0,0] = I[0,0]-x; | |
Ib[1,1] = I[1,1]-x; | |
Ib[2,2] = I[2,2]-x; | |
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