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- import sympy.physics.mechanics as _me
- import sympy as _sm
- import math as m
- import numpy as _np
- q1, q2, u1, u2 = _me.dynamicsymbols('q1 q2 u1 u2')
- q1_d, q2_d, u1_d, u2_d = _me.dynamicsymbols('q1_ q2_ u1_ u2_', 1)
- l, m, g = _sm.symbols('l m g', real=True)
- frame_n = _me.ReferenceFrame('n')
- frame_a = _me.ReferenceFrame('a')
- frame_b = _me.ReferenceFrame('b')
- frame_a.orient(frame_n, 'Axis', [q1, frame_n.z])
- frame_b.orient(frame_n, 'Axis', [q2, frame_n.z])
- frame_a.set_ang_vel(frame_n, u1*frame_n.z)
- frame_b.set_ang_vel(frame_n, u2*frame_n.z)
- point_o = _me.Point('o')
- particle_p = _me.Particle('p', _me.Point('p_pt'), _sm.Symbol('m'))
- particle_r = _me.Particle('r', _me.Point('r_pt'), _sm.Symbol('m'))
- particle_p.point.set_pos(point_o, l*frame_a.x)
- particle_r.point.set_pos(particle_p.point, l*frame_b.x)
- point_o.set_vel(frame_n, 0)
- particle_p.point.v2pt_theory(point_o,frame_n,frame_a)
- particle_r.point.v2pt_theory(particle_p.point,frame_n,frame_b)
- particle_p.mass = m
- particle_r.mass = m
- force_p = particle_p.mass*(g*frame_n.x)
- force_r = particle_r.mass*(g*frame_n.x)
- kd_eqs = [q1_d - u1, q2_d - u2]
- forceList = [(particle_p.point,particle_p.mass*(g*frame_n.x)), (particle_r.point,particle_r.mass*(g*frame_n.x))]
- kane = _me.KanesMethod(frame_n, q_ind=[q1,q2], u_ind=[u1, u2], kd_eqs = kd_eqs)
- fr, frstar = kane.kanes_equations([particle_p, particle_r], forceList)
- zero = fr+frstar
- from pydy.system import System
- sys = System(kane, constants = {l:1, m:1, g:9.81},
- specifieds={},
- initial_conditions={q1:.1, q2:.2, u1:0, u2:0},
- times = _np.linspace(0.0, 10, 10/.01))
- y=sys.integrate()
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