本文整理汇总了Python中pydrake.multibody.plant.MultibodyPlant.mutable_gravity_field方法的典型用法代码示例。如果您正苦于以下问题:Python MultibodyPlant.mutable_gravity_field方法的具体用法?Python MultibodyPlant.mutable_gravity_field怎么用?Python MultibodyPlant.mutable_gravity_field使用的例子?那么恭喜您, 这里精选的方法代码示例或许可以为您提供帮助。您也可以进一步了解该方法所在类pydrake.multibody.plant.MultibodyPlant
的用法示例。
在下文中一共展示了MultibodyPlant.mutable_gravity_field方法的2个代码示例,这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞,您的评价将有助于系统推荐出更棒的Python代码示例。
示例1: test_multibody_dynamics
# 需要导入模块: from pydrake.multibody.plant import MultibodyPlant [as 别名]
# 或者: from pydrake.multibody.plant.MultibodyPlant import mutable_gravity_field [as 别名]
def test_multibody_dynamics(self):
file_name = FindResourceOrThrow(
"drake/multibody/benchmarks/acrobot/acrobot.sdf")
plant = MultibodyPlant()
Parser(plant).AddModelFromFile(file_name)
# Getting ready for when we set foot on Mars :-).
gravity_vector = np.array([0.0, 0.0, -3.71])
plant.mutable_gravity_field().set_gravity_vector(gravity_vector)
np.testing.assert_equal(plant.gravity_field().gravity_vector(),
gravity_vector)
plant.Finalize()
context = plant.CreateDefaultContext()
# Set an arbitrary configuration away from the model's fixed point.
plant.SetPositions(context, [0.1, 0.2])
M = plant.CalcMassMatrixViaInverseDynamics(context)
Cv = plant.CalcBiasTerm(context)
self.assertTrue(M.shape == (2, 2))
self.assert_sane(M)
self.assertTrue(Cv.shape == (2, ))
self.assert_sane(Cv, nonzero=False)
nv = plant.num_velocities()
vd_d = np.zeros(nv)
tau = plant.CalcInverseDynamics(
context, vd_d, MultibodyForces(plant))
self.assertEqual(tau.shape, (2,))
self.assert_sane(tau, nonzero=False)
# - Existence checks.
# Gravity leads to non-zero potential energy.
self.assertNotEqual(plant.CalcPotentialEnergy(context), 0)
plant.CalcConservativePower(context)
tau_g = plant.CalcGravityGeneralizedForces(context)
self.assertEqual(tau_g.shape, (nv,))
self.assert_sane(tau_g, nonzero=True)
B = plant.MakeActuationMatrix()
np.testing.assert_equal(B, np.array([[0.], [1.]]))
forces = MultibodyForces(plant=plant)
plant.CalcForceElementsContribution(context=context, forces=forces)
# Test generalized forces.
forces.mutable_generalized_forces()[:] = 1
np.testing.assert_equal(forces.generalized_forces(), 1)
forces.SetZero()
np.testing.assert_equal(forces.generalized_forces(), 0)
# Test body force accessors and mutators.
link2 = plant.GetBodyByName("Link2")
self.assertIsInstance(
link2.GetForceInWorld(context, forces), SpatialForce)
forces.SetZero()
F_expected = np.array([1, 2, 3, 4, 5, 6])
link2.AddInForceInWorld(
context, F_Bo_W=SpatialForce(F=F_expected), forces=forces)
np.testing.assert_equal(
link2.GetForceInWorld(context, forces).get_coeffs(), F_expected)
link2.AddInForce(
context, p_BP_E=[0, 0, 0], F_Bp_E=SpatialForce(F=F_expected),
frame_E=plant.world_frame(), forces=forces)
# Also check accumulation.
np.testing.assert_equal(
link2.GetForceInWorld(context, forces).get_coeffs(),
2 * F_expected)
示例2: test_inverse_dynamics_controller
# 需要导入模块: from pydrake.multibody.plant import MultibodyPlant [as 别名]
# 或者: from pydrake.multibody.plant.MultibodyPlant import mutable_gravity_field [as 别名]
def test_inverse_dynamics_controller(self):
sdf_path = FindResourceOrThrow(
"drake/manipulation/models/" +
"iiwa_description/sdf/iiwa14_no_collision.sdf")
plant = MultibodyPlant(time_step=0.01)
Parser(plant).AddModelFromFile(sdf_path)
plant.WeldFrames(plant.world_frame(),
plant.GetFrameByName("iiwa_link_0"))
plant.mutable_gravity_field().set_gravity_vector([0.0, 0.0, 0.0])
plant.Finalize()
# We verify the (known) size of the model.
kNumPositions = 7
kNumVelocities = 7
kNumActuators = 7
kStateSize = kNumPositions + kNumVelocities
self.assertEqual(plant.num_positions(), kNumPositions)
self.assertEqual(plant.num_velocities(), kNumVelocities)
self.assertEqual(plant.num_actuators(), kNumActuators)
kp = np.array([1., 2., 3., 4., 5., 6., 7.])
ki = np.array([0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7])
kd = np.array([.5, 1., 1.5, 2., 2.5, 3., 3.5])
controller = InverseDynamicsController(robot=plant,
kp=kp,
ki=ki,
kd=kd,
has_reference_acceleration=True)
context = controller.CreateDefaultContext()
output = controller.AllocateOutput()
estimated_state_port = 0
desired_state_port = 1
desired_acceleration_port = 2
control_port = 0
self.assertEqual(
controller.get_input_port(desired_acceleration_port).size(),
kNumVelocities)
self.assertEqual(
controller.get_input_port(estimated_state_port).size(), kStateSize)
self.assertEqual(
controller.get_input_port(desired_state_port).size(), kStateSize)
self.assertEqual(
controller.get_output_port(control_port).size(), kNumVelocities)
# Current state.
q = np.array([-0.3, -0.2, -0.1, 0.0, 0.1, 0.2, 0.3])
v = np.array([-0.9, -0.6, -0.3, 0.0, 0.3, 0.6, 0.9])
x = np.concatenate([q, v])
# Reference state and acceleration.
q_r = q + 0.1*np.ones_like(q)
v_r = v + 0.1*np.ones_like(v)
x_r = np.concatenate([q_r, v_r])
vd_r = np.array([1., 2., 3., 4., 5., 6., 7.])
integral_term = np.array([-1., -2., -3., -4., -5., -6., -7.])
vd_d = vd_r + kp*(q_r-q) + kd*(v_r-v) + ki*integral_term
context.FixInputPort(estimated_state_port, BasicVector(x))
context.FixInputPort(desired_state_port, BasicVector(x_r))
context.FixInputPort(desired_acceleration_port, BasicVector(vd_r))
controller.set_integral_value(context, integral_term)
# Set the plant's context.
plant_context = plant.CreateDefaultContext()
x_plant = plant.GetMutablePositionsAndVelocities(plant_context)
x_plant[:] = x
# Compute the expected value of the generalized forces using
# inverse dynamics.
tau_id = plant.CalcInverseDynamics(
plant_context, vd_d, MultibodyForces(plant))
# Verify the result.
controller.CalcOutput(context, output)
self.assertTrue(np.allclose(output.get_vector_data(0).CopyToVector(),
tau_id))