Drake

The Acrobot  a canonical underactuated system as described in Chapter 3 of Underactuated Robotics. More...
#include <drake/multibody/benchmarks/acrobot/acrobot.h>
Public Member Functions  
Acrobot (const Vector3< T > &normal, const Vector3< T > &up, double m1=1.0, double m2=1.0, double l1=1.0, double l2=1.0, double lc1=0.5, double lc2=0.5, double Ic1=.083, double Ic2=.33, double b1=0.1, double b2=0.1, double g=9.81)  
Creates an acrobot model in a plane passing through the world's origin and normal to normal . More...  
Matrix2< T >  CalcMassMatrix (const T &theta2) const 
Computes the mass matrix H(q) for the double pendulum system. More...  
Vector2< T >  CalcCoriolisVector (const T &theta1, const T &theta2, const T &theta1dot, const T &theta2dot) const 
Computes the bias term C(q, v) * v containing Coriolis and gyroscopic effects as a function of the state of the pendulum. More...  
Vector2< T >  CalcGravityVector (const T &theta1, const T &theta2) const 
Computes the effective jointspace torques induced by gravity tau_g(q) containing the effect of gravity as a function of the configuration of the pendulum. More...  
math::RigidTransform< T >  CalcLink1PoseInWorldFrame (const T &theta1) const 
Computes the pose of the center of mass of link 1 measured and expressed in the world frame. More...  
math::RigidTransform< T >  CalcLink2PoseInWorldFrame (const T &theta1, const T &theta2) const 
Computes the pose of the center of mass of link 2 measured and expressed in the world frame. More...  
math::RigidTransform< T >  CalcElbowOutboardFramePoseInWorldFrame (const T &theta1, const T &theta2) const 
Computes the pose of the elbow outboard frame Eo in the world frame W. More...  
Vector6< T >  CalcLink1SpatialVelocityInWorldFrame (const T &theta1, const T &theta1dot) const 
Computes the spatial velocity of the center of mass of link 1 expressed in the world frame. More...  
Vector6< T >  CalcLink2SpatialVelocityInWorldFrame (const T &theta1, const T &theta2, const T &theta1dot, const T &theta2dot) const 
Computes the spatial velocity of the center of mass of link 2 expressed in the world frame. More...  
Vector6< T >  CalcLink1SpatialAccelerationInWorldFrame (const T &theta1, const T &theta1dot, const T &theta1dotdot) const 
Computes the spatial acceleration of the center of mass of link 1 expressed in the world frame. More...  
Vector6< T >  CalcLink2SpatialAccelerationInWorldFrame (const T &theta1, const T &theta2, const T &theta1dot, const T &theta2dot, const T &theta1dotdot, const T &theta2dotdot) const 
Computes the spatial acceleration of the center of mass of link 2 expressed in the world frame. More...  
T  CalcPotentialEnergy (const T &theta1, const T &theta2) const 
Computes the total potential energy due to gravity of the acrobot system for the state given by angles theta1 and theta2 . More...  
The Acrobot  a canonical underactuated system as described in Chapter 3 of Underactuated Robotics.
This system essentially is a double pendulum consisting of two links. Link 1 is connected to the world by a "shoulder" revolute joint parameterized by angle theta1 and Link 2 is connected to Link 1 by an "elbow" revolute joint parameterized by angle theta2.
T  The vector element type, which must be a valid Eigen scalar. 
Instantiated templates for the following kinds of T's are provided:
Acrobot  (  const Vector3< T > &  normal, 
const Vector3< T > &  up,  
double  m1 = 1.0 , 

double  m2 = 1.0 , 

double  l1 = 1.0 , 

double  l2 = 1.0 , 

double  lc1 = 0.5 , 

double  lc2 = 0.5 , 

double  Ic1 = .083 , 

double  Ic2 = .33 , 

double  b1 = 0.1 , 

double  b2 = 0.1 , 

double  g = 9.81 

) 
Creates an acrobot model in a plane passing through the world's origin and normal to normal
.
Vector up
defines the upwards direction on this plane. Both normal
and up
are expressed in the world's frame. Essentially the two dimensional equations of the acrobot are described in a model frame D within a xy plane with y the vertical direction and gravity pointing downwards. Therefore the axes defining the model frame D are:
z_W = normal_W.normalized() y_W = (up  up.dot(z_W) * z_W).normalized() x_W = y_W.cross(z_W)
The remaining arguments define the properties of the double pendulum system:
Vector2< T > CalcCoriolisVector  (  const T &  theta1, 
const T &  theta2,  
const T &  theta1dot,  
const T &  theta2dot  
)  const 
Computes the bias term C(q, v) * v
containing Coriolis and gyroscopic effects as a function of the state of the pendulum.
RigidTransform< T > CalcElbowOutboardFramePoseInWorldFrame  (  const T &  theta1, 
const T &  theta2  
)  const 
Computes the pose of the elbow outboard frame Eo
in the world frame W.
theta1  The shoulder angle in radians. 
theta2  The elbow angle in radians. 
Computes the effective jointspace torques induced by gravity tau_g(q)
containing the effect of gravity as a function of the configuration of the pendulum.
Unlike http://underactuated.mit.edu/underactuated.html?chapter=3, cited in this class's documentation, we define tau_g(q)
to be on the right hand side of the equations of motion, that is, Mv̇ + C(q, v)v = tau_g(q)
.
math::RigidTransform< T > CalcLink1PoseInWorldFrame  (  const T &  theta1  )  const 
Computes the pose of the center of mass of link 1 measured and expressed in the world frame.
theta1  The shoulder angle in radians. 
theta2  The elbow angle in radians. 
Vector6< T > CalcLink1SpatialAccelerationInWorldFrame  (  const T &  theta1, 
const T &  theta1dot,  
const T &  theta1dotdot  
)  const 
Computes the spatial acceleration of the center of mass of link 1 expressed in the world frame.
theta1  The shoulder angle in radians. 
theta1dot  The shoulder angular velocity in radians per second. 
theta1dotdot  The elbow angular acceleration in radians per second squared. 
A_WL1_W  the spatial acceleration of the center of mass of link 1 with respect to the world and expressed in the world frame. 
Computes the spatial velocity of the center of mass of link 1 expressed in the world frame.
theta1  The shoulder angle in radians. 
theta1dot  The shoulder angular velocity in radians per second. 
RigidTransform< T > CalcLink2PoseInWorldFrame  (  const T &  theta1, 
const T &  theta2  
)  const 
Computes the pose of the center of mass of link 2 measured and expressed in the world frame.
theta1  The shoulder angle in radians. 
theta2  The elbow angle in radians. 
Vector6< T > CalcLink2SpatialAccelerationInWorldFrame  (  const T &  theta1, 
const T &  theta2,  
const T &  theta1dot,  
const T &  theta2dot,  
const T &  theta1dotdot,  
const T &  theta2dotdot  
)  const 
Computes the spatial acceleration of the center of mass of link 2 expressed in the world frame.
theta1  The shoulder angle in radians. 
theta2  The elbow angle in radians. 
theta1dot  The shoulder angular velocity in radians per second. 
theta2dot  The elbow angular velocity in radians per second. 
theta1dotdot  The shoulder angular acceleration in radians per second squared. 
theta2dotdot  The elbow angular acceleration in radians per second squared. 
A_WL2_W  the spatial acceleration of the center of mass of link 2 with respect to the world and expressed in the world frame. 
Vector6< T > CalcLink2SpatialVelocityInWorldFrame  (  const T &  theta1, 
const T &  theta2,  
const T &  theta1dot,  
const T &  theta2dot  
)  const 
Computes the spatial velocity of the center of mass of link 2 expressed in the world frame.
theta1  The shoulder angle in radians. 
theta2  The elbow angle in radians. 
theta1dot  The shoulder angular velocity in radians per second. 
theta2dot  The elbow angular velocity in radians per second. 
Computes the mass matrix H(q)
for the double pendulum system.
It turns out that for this system the mass matrix is independent of the shoulder angle theta1
.
Computes the total potential energy due to gravity of the acrobot system for the state given by angles theta1
and theta2
.
The zero potential energy is defined for y = 0
.