cartpole_dynamics_solver.cpp
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29 
31 
33 
34 namespace exotica
35 {
36 CartpoleDynamicsSolver::CartpoleDynamicsSolver()
37 {
38  num_positions_ = 2;
39  num_velocities_ = 2;
40  num_controls_ = 1;
41  has_second_order_derivatives_ = true;
42 }
43 
44 void CartpoleDynamicsSolver::AssignScene(ScenePtr scene_in)
45 {
46  const int num_positions_in = scene_in->GetKinematicTree().GetNumControlledJoints();
47  // TODO: This is a terrible check (not against name etc.), but can stop _some_ mismatches between URDF/model and dynamics
48  if (num_positions_in != 2)
49  ThrowPretty("Robot model may not be a Cartpole.");
50 }
51 
52 Eigen::VectorXd CartpoleDynamicsSolver::f(const StateVector& x, const ControlVector& u)
53 {
54  const double& theta = x(1);
55  const double& xdot = x(2);
56  const double& thetadot = x(3);
57 
58  auto sin_theta = std::sin(theta);
59  auto cos_theta = std::cos(theta);
60  auto theta_dot_squared = thetadot * thetadot;
61 
62  auto x_dot = StateVector(4);
63  x_dot << xdot, thetadot,
64  (u(0) + m_p_ * sin_theta * (l_ * theta_dot_squared + g_ * cos_theta)) /
65  (m_c_ + m_p_ * sin_theta * sin_theta),
66  -(l_ * m_p_ * cos_theta * sin_theta * theta_dot_squared + u(0) * cos_theta +
67  (m_c_ + m_p_) * g_ * sin_theta) /
68  (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta);
69 
70  return x_dot;
71 }
72 
73 // NOTE: tested in test/test_cartpole_diff.py in this package
74 Eigen::MatrixXd CartpoleDynamicsSolver::fx(const StateVector& x, const ControlVector& u)
75 {
76  const double& theta = x(1);
77  const double& tdot = x(3);
78 
79  auto sin_theta = std::sin(theta);
80  auto cos_theta = std::cos(theta);
81 
82  Eigen::Matrix4d fx;
83  fx << 0, 0, 1, 0,
84  0, 0, 0, 1,
85  //
86  0,
87  -2 * m_p_ * (m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * sin_theta + u(0)) * sin_theta * cos_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2) + (-g_ * m_p_ * sin_theta * sin_theta + m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * cos_theta) / (m_c_ + m_p_ * sin_theta * sin_theta),
88  0,
89  2 * l_ * m_p_ * tdot * sin_theta / (m_c_ + m_p_ * sin_theta * sin_theta),
90  //
91  0,
92  -2 * l_ * m_p_ * (-g_ * (m_c_ + m_p_) * sin_theta - l_ * m_p_ * tdot * tdot * sin_theta * cos_theta - u(0) * cos_theta) * sin_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) + (-g_ * (m_c_ + m_p_) * cos_theta + l_ * m_p_ * tdot * tdot * sin_theta * sin_theta - l_ * m_p_ * tdot * tdot * cos_theta * cos_theta + u(0) * sin_theta) / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta),
93  0,
94  -2 * l_ * m_p_ * tdot * sin_theta * cos_theta / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta);
95 
96  return fx;
97 }
98 
99 // NOTE: tested in test/test_cartpole_diff.py in this package
100 Eigen::MatrixXd CartpoleDynamicsSolver::fu(const StateVector& x, const ControlVector& u)
101 {
102  const double& theta = x(1);
103 
104  auto sin_theta = std::sin(theta);
105  auto cos_theta = std::cos(theta);
106 
107  Eigen::Vector4d fu;
108  fu << 0, 0, 1 / (m_c_ + m_p_ * sin_theta * sin_theta), -cos_theta / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta);
109  return fu;
110 }
111 
112 // NOTE: Code to generate 2nd order dynamics is in scripts/gen_second_order_dynamics.py
113 // fxx -> NX x NX x NX
114 // middle dimension is always NX
115 // NX = 4
116 // NU = 1
117 Eigen::Tensor<double, 3> CartpoleDynamicsSolver::fxx(const StateVector& x, const ControlVector& u)
118 {
119  const double& theta = x(1);
120  const double& tdot = x(3);
121 
122  auto sin_theta = std::sin(theta);
123  auto cos_theta = std::cos(theta);
124 
125  Eigen::Tensor<double, 3> fxx(num_positions_ + num_velocities_, num_positions_ + num_velocities_, num_positions_ + num_velocities_);
126  fxx.setValues({{{0, 0, 0, 0},
127  {0, 0, 0, 0},
128  {0, 0, 0, 0},
129  {0, 0, 0, 0}},
130  {{0, 0, 0, 0},
131  {0, 0, 0, 0},
132  {0,
133  8 * m_p_ * m_p_ * (m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * sin_theta + u(0)) * sin_theta * sin_theta * cos_theta * cos_theta /
134  std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 3) -
135  4 * m_p_ * (-g_ * m_p_ * sin_theta * sin_theta + m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * cos_theta) * sin_theta * cos_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2) +
136  2 * m_p_ * (m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * sin_theta + u(0)) * sin_theta * sin_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2) - 2 * m_p_ * (m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * sin_theta + u(0)) * cos_theta * cos_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2) + (-3 * g_ * m_p_ * sin_theta * cos_theta - m_p_ * (g_ * cos_theta + l_ * tdot * tdot) * sin_theta) / (m_c_ + m_p_ * sin_theta * sin_theta),
137  0,
138  -4 * l_ * m_p_ * m_p_ * tdot * sin_theta * sin_theta * cos_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2) + 2 * l_ * m_p_ * tdot * cos_theta / (m_c_ + m_p_ * sin_theta * sin_theta)},
139  {0,
140  8 * l_ * l_ * m_p_ * m_p_ * (-g_ * (m_c_ + m_p_) * sin_theta - l_ * m_p_ * tdot * tdot * sin_theta * cos_theta - u(0) * cos_theta) * sin_theta * sin_theta * cos_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 3) + 2 * l_ * m_p_ * (-g_ * (m_c_ + m_p_) * sin_theta - l_ * m_p_ * tdot * tdot * sin_theta * cos_theta - u(0) * cos_theta) * sin_theta * sin_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) - 2 * l_ * m_p_ * (-g_ * (m_c_ + m_p_) * sin_theta - l_ * m_p_ * tdot * tdot * sin_theta * cos_theta - u(0) * cos_theta) * cos_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) - 4 * l_ * m_p_ * (-g_ * (m_c_ + m_p_) * cos_theta + l_ * m_p_ * tdot * tdot * sin_theta * sin_theta - l_ * m_p_ * tdot * tdot * cos_theta * cos_theta + u(0) * sin_theta) * sin_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) + (g_ * (m_c_ + m_p_) * sin_theta + 4 * l_ * m_p_ * tdot * tdot * sin_theta * cos_theta + u(0) * cos_theta) / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta),
141  0,
142  4 * l_ * l_ * m_p_ * m_p_ * tdot * sin_theta * sin_theta * cos_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) + 2 * l_ * m_p_ * tdot * sin_theta * sin_theta / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta) - 2 * l_ * m_p_ * tdot * cos_theta * cos_theta / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta)}},
143  {{0, 0, 0, 0},
144  {0, 0, 0, 0},
145  {0, 0, 0, 0},
146  {0, 0, 0, 0}},
147  {{0, 0, 0, 0},
148  {0, 0, 0, 0},
149  {0,
150  -4 * l_ * m_p_ * m_p_ * tdot * sin_theta * sin_theta * cos_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2) + 2 * l_ * m_p_ * tdot * cos_theta / (m_c_ + m_p_ * sin_theta * sin_theta),
151  0, 2 * l_ * m_p_ * sin_theta / (m_c_ + m_p_ * sin_theta * sin_theta)},
152  {0,
153  4 * l_ * l_ * m_p_ * m_p_ * tdot * sin_theta * sin_theta * cos_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) +
154  (2 * l_ * m_p_ * tdot * sin_theta * sin_theta - 2 * l_ * m_p_ * tdot * cos_theta * cos_theta) / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta),
155  0, -2 * l_ * m_p_ * sin_theta * cos_theta / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta)}}});
156  return fxx;
157 }
158 
159 Eigen::Tensor<double, 3> CartpoleDynamicsSolver::fxu(const StateVector& x, const ControlVector& u)
160 {
161  const double& theta = x(1);
162 
163  auto sin_theta = std::sin(theta);
164  auto cos_theta = std::cos(theta);
165 
166  Eigen::Tensor<double, 3> fxu(num_positions_ + num_velocities_, num_positions_ + num_velocities_, num_controls_);
167  fxu.setValues({{{0, 0, 0, 0},
168  {0, 0, 0, 0},
169  {0, -2 * m_p_ * sin_theta * cos_theta / std::pow(m_c_ + m_p_ * sin_theta * sin_theta, 2), 0, 0},
170  {0, 2 * l_ * m_p_ * sin_theta * cos_theta * cos_theta / std::pow(l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta, 2) + sin_theta / (l_ * m_c_ + l_ * m_p_ * sin_theta * sin_theta),
171  0, 0}}});
172  return fxu;
173 }
174 
175 } // namespace exotica
#define REGISTER_DYNAMICS_SOLVER_TYPE(TYPE, DERIV)
#define ThrowPretty(m)
std::shared_ptr< Scene > ScenePtr
Eigen::Matrix< T, NU, 1 > ControlVector
Eigen::Matrix< T, NX, 1 > StateVector


exotica_cartpole_dynamics_solver
Author(s): Traiko Dinev
autogenerated on Sat Apr 10 2021 02:36:04