pinocchio  2.6.3 A fast and flexible implementation of Rigid Body Dynamics algorithms and their analytical derivatives
2) Grasp an object (aka inverse Geometry)

## Objectives

The main objective of the first tutorial is to compute a configuration of the robot minimizing a cost (maximizing a reward) and respecting some given constraints. Additionally, the objective is to have a first hands on the difficulties of working outside of real vector spaces and to consider what are the guesses that are taken by an optimal solver.

## 2.0) Technical prerequisites

### Python SciPy and MatplotLib

You will need the two Python libraries: SciPy (scientific Python) and MatPlotLib (plot mathematical data).

SciPy can be installed by sudo apt-get install python-scipy. Examples of calls of these two functions are given below. We will use both solvers with numerical (finite-differencing) differentiation, to avoid the extra work of differencing the cost and constraint functions by hand. In general, it is strongly advice to first test a numerical program with finite differencing, before implementing the true derivatives only if needed. In any case, the true derivatives must always be checked by comparing the results with the finite differentiation.

Additionally, the provided implementation of BFGS allows the user to provide a callback function and track the path taken by the solver, but does not provide the possibility to specify constraints (constraints can be added as penalty functions in the cost, but this requires additional work). The constrained least-square implementation allows the user to specify equality and inequality constraints, but not the callback. In the following, start to use BFGS before moving to the constrained least-square only when constraints are really needed.

# Example of use a the optimization toolbox of SciPy.
import numpy as np
from scipy.optimize import fmin_bfgs, fmin_slsqp
def cost(x):
'''Cost f(x, y) = x² + 2y² - 2xy - 2x '''
x0, x1 = x
return -(2 * x0 * x1 + 2 * x0 - x0 ** 2 - 2 * x1 ** 2)
def constraint_eq(x):
''' Constraint x³ = y '''
return np.array([ x[0] ** 3 - x[1] ])
def constraint_ineq(x):
'''Constraint x >= 2, y >= 2'''
return np.array([ x[0] - 2, x[1] - 2 ])
class CallbackLogger:
def __init__(self):
self.nfeval = 1
def __call__(self,x):
print('===CBK=== {0:4d} {1: 3.6f} {2: 3.6f} {3: 3.6f}'.format(self.nfeval, x[0], x[1], cost(x)))
self.nfeval += 1
x0 = np.array([0.0, 0.0]) # Optimize cost without any constraints in BFGS, with traces.
xopt_bfgs = fmin_bfgs(cost, x0, callback=CallbackLogger())
print('*** Xopt in BFGS =', xopt_bfgs)
# Optimize cost without any constraints in CLSQ
xopt_lsq = fmin_slsqp(cost, [-1.0, 1.0], iprint=2, full_output=1)
print('*** Xopt in LSQ =', xopt_lsq)
# Optimize cost with equality and inequality constraints in CLSQ
xopt_clsq = fmin_slsqp(cost, [-1.0, 1.0], f_eqcons=constraint_eq, f_ieqcons=constraint_ineq, iprint=2, full_output=1)
print('*** Xopt in c-lsq =', xopt_clsq)

Take care that all SciPy always works with vectors represented as 1-dimensional array, while Pinocchio works with vectors represented as matrices (which are in fact two-dimensional arrays, with the second dimension being 1). You can pass from a SciPy-like vector to a Pinocchio-like vector using:

import numpy as np
x = np.array([1.0, 2.0, 3.0])
q = np.matrix(x).T
x = q.getA()[:, 0]

The second library MatPlotLib plots values on a 2D graph. A tutorial is available here. An example is provided below.

import numpy as np
import matplotlib.pyplot as plt
# In plt, the following functions are the most useful:
# ion, plot, draw, show, subplot, figure, title, savefig
# For use in interactive python mode (ipthyon -i)
interactivePlot = False
if interactivePlot:
plt.ion() # Plot functions now instantaneously display, shell is not blocked
# Build numpy array for x axis
x = 1e-3 * np.array(range(100))
# Build numpy array for y axis
y = x ** 2
fig = plt.figure()
ax.plot(x, y)
ax.legend(("x^2", ))
if not interactivePlot:
# Display all the plots and block the shell.
# The script will only ends when all windows are closed.
plt.show()

### Robots

We mostly use here the model UR5, used in the first lab. Refer to the instructions of Lab 1 to load it.

Optionally, we might want to use a more complex robot model. Romeo is a humanoid robot developed by the French-Japanese company Aldebaran Robotics. It has two legs, two arms and a head, for a total of 31 joints (plus 6DOF on the free flyer). The description of Romeo can be obtained with:

sudo apt install robotpkg-romeo-description

from os.path import join
import pinocchio as se3
from pinocchio.romeo_wrapper import RomeoWrapper
PKG = '/opt/openrobots/share'
URDF = join(PKG, 'romeo_description/urdf/romeo.urdf')
robot = RomeoWrapper(URDF, [PKG]) # Load urdf model

Additionally, the index of right and left hands and feet are stored in robot.rh, robot.lh, robot.rf and robot.lf.

## 2.1) Position the end effector

The first tutorial is to position (i.e. translation only) the end effector of a manipulator robot to a given position. For this first part, we will use the fixed serial-chain robot model.

Recall first that the position (3D) of the joint with index i at position q can be access by the following two lines of code:

# Compute all joint placements and put the position of joint "i" in variable "p".
import pinocchio as se3
se3.forwardKinematics(robot.model, robot.data, q)
p = robot.data.oMi[i].translation

#### Question 1

Using this, build a cost function to be the norm of the difference between the end-effector position p and a desired position pdes. The cost function is a function that accepts as input an 1-dimensional array and return a float.

#### Question 2

Then use fmin_bfgs to find a configuration q with the end effector at position pdes.

#### Question 3

Finally, implements a callback function that display in Gepetto-Viewer every candidate configuration tried by the solver.

## 2.2) Approaching the redundancy (optionnal)

The manipulator arm has 6 DOF, while the cost function only constraints 3 of them (the position of the end effector). A continuum of solutions then exists. The two next questions are aiming at giving an intuition of this continuum.

#### Question 4

Sample several configurations respecting pdes by giving various initial guesses to the solver. Store this sampling of solutions in a list, then display this list in Gepetto-Viewer, each configuration begin displayed during 1 second (pause of 1 seconds can be obtained using: import time; time.sleep(1)).

A configurations in this continuum can then be selected with particular properties, like for example being the closest to a reference configuration, or using some joints more than the others, or any other criterion that you can imagine.

#### Question 5

Sum a secondary cost term to the first positioning cost, to select the posture that maximizes the similarity (minimizes the norm of the difference) to a reference posture. The relative importance of the two cost terms can be adjusted by weighting the sum: find the weight so that the reference position is obtained with a negligible error (below millimeter) while the posture is properly taken into account.

## 2.3) Placing the end-effector

The next step is to find a configuration of the robot so that the end effector respects a reference placement, i.e. position and orientation. The stake is to find a metric in $$SE(3)$$ to continuously quantify the distance between two placements. There is no canonical metric in $$SE(3)$$, i.e. no absolute way of weighting the position with respect to the orientation. Two metrics can be considered, namely the log in $$SE(3)$$ or in $$R^3 \times SO(3)$$. The tutorial will guide you through the first choice.

The $$SE(3)$$ and $$SO(3)$$ logarithm are implemented in Pinocchio in the explog module.

from pinocchio.explog import log
from pinocchio import SE3
nu = log(SE3.Random())
nu_vec = nu.vector

#### Question 6

Solve for the configuration that minimizes the norm of the logarithm of the difference between the end effector placement and the desired placement.

Optionally, try other metrics, like the log metric of $$R^3 \times SO(3)$$, or the Froebenius norm of the homogeneous matrix.

## 2.4) Working with a mobile robot (optionnal)

Until now, the tutorial only worked with a simple manipulator robot, i.e. whose configuration space is a real vector space. Consider now the humanoid robot, whose first joint is a free joint: it has 6 degrees of freedom (3 rotations, 3 translations) but its configuration vector is dimension 7. You can check it with robot.model.nq, that stores the dimension of the configuration, and robot.model.nv, that stores the dimension of the configuration velocity, i.e. the number of degrees of freedom. For the humanoid, nq = nv + 1.

Indeed, the configuration coefficients 3 to 7 are indeed representing a quaternion. The additional constraint is that these 4 coefficients must be normalize.

#### Question 7

Display a configuration of the robot for which the norm of the quaternion is bigger than one (e.g. 2.0). What happens?

During the search, the solver must respect this constraint. A solution is to make this constraint explicit in the numerical program. However, we will start by an easier quick-and-dirty trick. With quaternions, the trick is simply to normalize any invalid quaternions. In the cost function, first normalize the quaternion before computing the cost due to the end-effector placement. An additional term should also be added to the cost function to avoid excessive drift of the quaternion norm, in particular with the norm going to 0.

#### Question 8

Use fmin_bfgs to compute a configuration respecting a given placement with the humanoid model, by normalizing the quaternion at each step.

#### Question 9 (harder)

Do the same with the solver C-LSQ fmin_slsqp, with the explicit constraint that the norm of the quaternion must be 1.

## 2.5) Configuration of a parallel robot

A parallel robot is composed of several kinematic chains (called the robot legs) that are all attached to the same end effector. This imposes strict constraints in the configuration space of the robot: a configuration is valide iff all the legs meets the same end-effector placement. We consider here only the geometry aspect of parallel robots (additionnally, some joints are not actuated, which causes additional problems).

The kinematic structure of a paralel robot indeed induces loops in the joint connection graph. In Pinocchio, we can only represents (one of) the underlying kinematic tree. The loop constraints have to be handled separately. An example that loads 4 manipulator arms is available here. Each leg i (for i=0,1,2,3) of the robot is loaded in the list robots[i]. The loop constraints are that the relative placement of every leg end-effector must stay the same that in the initial configuration given as example in the above file.

#### Question 10

Consider now that the orientation of the tool plate is given by the quaternion Quaternion(0.7, 0.2, 0.2, 0.6), with the translation that you like. Find using the above optimization routines the configuration of each robot leg so that the loop constraints are all met.