Underactuated Robotics

Algorithms for Walking, Running, Swimming, Flying, and Manipulation

Russ Tedrake

© Russ Tedrake, 2022
Last modified .
How to cite these notes, use annotations, and give feedback.

Note: These are working notes used for a course being taught at MIT. They will be updated throughout the Spring 2022 semester. Lecture videos are available on YouTube.

Table of contents Next Chapter

Fully-actuated vs Underactuated Systems

Robots today move far too conservatively, and accomplish only a fraction of the tasks and achieve a fraction of the performance that they are mechanically capable of. In many cases, we are still fundamentally limited by control technology which matured on rigid robotic arms in structured factory environments. The study of underactuated robotics focuses on building control systems which use the natural dynamics of the machines in an attempt to achieve extraordinary performance in terms of speed, efficiency, or robustness.


Let's start with some examples, and some videos.

Honda's ASIMO vs. passive dynamic walkers

The world of robotics changed when, in late 1996, Honda Motor Co. announced that they had been working for nearly 15 years (behind closed doors) on walking robot technology. Their designs have continued to evolve, resulting in a humanoid robot they call ASIMO (Advanced Step in Innovative MObility). For nearly 20 years, Honda's robots were widely considered to represent the state of the art in walking robots, although there are now many robots with designs and performance very similar to ASIMO's. We will dedicate effort to understanding a few of the details of ASIMO when we discuss algorithms for walking... for now I just want you to become familiar with the look and feel of ASIMO's movements [watch the asimo video below now].

Honda's ASIMO (from http://world.honda.com/ASIMO/video/)

I hope that your first reaction is to be incredibly impressed with the quality and versatility of ASIMO's movements. Now take a second look. Although the motions are very smooth, there is something a little unnatural about ASIMO's gait. It feels a little like an astronaut encumbered by a heavy space suit. In fact this is a reasonable analogy... ASIMO is walking a bit like somebody that is unfamiliar with his/her dynamics. Its control system is using high-gain feedback, and therefore considerable joint torque, to cancel out the natural dynamics of the machine and strictly follow a desired trajectory. This control approach comes with a stiff penalty. ASIMO uses roughly 20 times the energy (scaled) that a human uses to walk on the flat (measured by cost of transport)Collins05. Also, control stabilization in this approach only works in a relatively small portion of the state space (when the stance foot is flat on the ground), so ASIMO can't move nearly as quickly as a human, and cannot walk on unmodelled or uneven terrain.

replace these when Andy fixes the link

A 3D passive dynamic walker by Steve Collins and Andy RuinaCollins01.

For contrast, let's now consider a very different type of walking robot, called a passive dynamic walker (PDW). This "robot" has no motors, no controllers, no computer, but is still capable of walking stably down a small ramp, powered only by gravity [watch videos above now]. Most people will agree that the passive gait of this machine is more natural than ASIMO's; it is certainly more efficient. Passive walking machines have a long history - there are patents for passively walking toys dating back to the mid 1800's. We will discuss, in detail, what people know about the dynamics of these machines and what has been accomplished experimentally. This most impressive passive dynamic walker to date was built by Steve Collins in Andy Ruina's lab at CornellCollins01.

Passive walkers demonstrate that the high-gain, dynamics-cancelling feedback approach taken on ASIMO is not a necessary one. In fact, the dynamics of walking is beautiful, and should be exploited - not cancelled out.

The world is just starting to see what this vision could look like. This video from Boston Dynamics is one of my favorites of all time:

Boston Dynamics' Atlas robot does a backflip. Make sure you've seen the dancing video, too.

This result is a marvel of engineering (the mechanical design alone is amazing...). In this class, we'll teach you the computational tools required to make robots perform this way. We'll also try to reason about how robust these types of maneuvers are and can be. Don't worry, if you do not have a super lightweight, super capable, and super durable humanoid, then a simulation will be provided for you.

Birds vs. modern aircraft

The story is surprisingly similar in a very different type of machine. Modern airplanes are extremely effective for steady-level flight in still air. Propellers produce thrust very efficiently, and today's cambered airfoils are highly optimized for speed and/or efficiency. It would be easy to convince yourself that we have nothing left to learn from birds. But, like ASIMO, these machines are mostly confined to a very conservative, low angle-of-attack flight regime where the aerodynamics on the wing are well understood. Birds routinely execute maneuvers outside of this flight envelope (for instance, when they are landing on a perch), and are considerably more effective than our best aircraft at exploiting energy (eg, wind) in the air.

As a consequence, birds are extremely efficient flying machines; some are capable of migrating thousands of kilometers with incredibly small fuel supplies. The wandering albatross can fly for hours, or even days, without flapping its wings - these birds exploit the shear layer formed by the wind over the ocean surface in a technique called dynamic soaring. Remarkably, the metabolic cost of flying for these birds is indistinguishable from the baseline metabolic costArnould96, suggesting that they can travel incredible distances (upwind or downwind) powered almost completely by gradients in the wind. Other birds achieve efficiency through similarly rich interactions with the air - including formation flying, thermal soaring, and ridge soaring. Small birds and large insects, such as butterflies and locusts, use "gust soaring" to migrate hundreds or even thousands of kilometers carried primarily by the wind.

Birds are also incredibly maneuverable. The roll rate of a highly acrobatic aircraft (e.g, the A-4 Skyhawk) is approximately 720 deg/secShyy08; a barn swallow has a roll rate in excess of 5000 deg/secShyy08. Bats can be flying at full-speed in one direction, and completely reverse direction while maintaining forward speed, all in just over 2 wing-beats and in a distance less than half the wingspanTian06. Although quantitative flow visualization data from maneuvering flight is scarce, a dominant theory is that the ability of these animals to produce sudden, large forces for maneuverability can be attributed to unsteady aerodynamics, e.g., the animal creates a large suction vortex to rapidly change directionTriantafyllou95. These astonishing capabilities are called upon routinely in maneuvers like flared perching, prey-catching, and high speed flying through forests and caves. Even at high speeds and high turn rates, these animals are capable of incredible agility - bats sometimes capture prey on their wings, Peregrine falcons can pull 25 G's out of a 240 mph dive to catch a sparrow in mid-flightTucker98, and even the small birds outside our building can be seen diving through a chain-link fence to grab a bite of food.

Although many impressive statistics about avian flight have been recorded, our understanding is partially limited by experimental accessibility - it is quite difficult to carefully measure birds (and the surrounding airflow) during their most impressive maneuvers without disturbing them. The dynamics of a swimming fish are closely related, and can be more convenient to study. Dolphins have been known to swim gracefully through the waves alongside ships moving at 20 knotsTriantafyllou95. Smaller fish, such as the bluegill sunfish, are known to possess an escape response in which they propel themselves to full speed from rest in less than a body length; flow visualizations indeed confirm that this is accomplished by creating a large suction vortex along the side of the bodyTytell08 - similar to how bats change direction in less than a body length. There are even observations of a dead fish swimming upstream by pulling energy out of the wake of a cylinder; this passive propulsion is presumably part of the technique used by rainbow trout to swim upstream at mating seasonBeal06.


Despite a long history of success in industrial applications, and the huge potential for consumer applications, we still don't have robot arms that can perform any meaningful tasks in the home. Admittedly, the perception problem (using sensors to detect/localize objects and understand the scene) for home robotics is incredibly difficult. But even if we were given a perfect perception system, our robots are still a long way from performing basic object manipulation tasks with the dexterity and versatility of a human.

Most robots that perform object manipulation today use a stereotypical pipeline. First, we enumerate a handful of contact locations on the hand (these points, and only these points, are allowed to contact the world). Then, given a localized object in the environment, we plan a collision-free trajectory for the arm that will move the hand into a "pre-grasp" location. At this point the robot closes it's eyes (figuratively) and closes the hand, hoping that the pre-grasp location was good enough that the object will be successfully grasped using e.g. only current feedback in the fingers to know when to stop closing. "Underactuated hands" make this approach more successful, but the entire approach really only works well for enveloping grasps.

The enveloping grasps approach may actually be sufficient for a number of simple pick-and-place tasks, but it is a very poor representation of how humans do manipulation. When humans manipulate objects, the contact interactions with the object and the world are very rich -- we often use pieces of the environment as fixtures to reduce uncertainty, we commonly exploit slipping behaviors (e.g. for picking things up, or reorienting it in the hand), and our brains don't throw NaNs if we use the entire surface of our arms to e.g. manipulate a large object.

In the last few years, I've began to focus my own research to problems in the manipulation domain. In this space, the interaction between dynamics and perception is incredibly rich. As a result, I've started an entirely separate set of notes (and a second course) on manipulation.

By the way, in most cases, if the robots fail to make contact at the anticipated contact times/locations, bad things can happen. The results are hilarious and depressing at the same time. (Let's fix that!)

The common theme

Classical control techniques for robotics are based on the idea that feedback control can be used to override the dynamics of our machines. In contrast, the examples I've given above suggest that to achieve outstanding dynamic performance (efficiency, agility, and robustness) from our robots, we need to understand how to design control systems which take advantage of the dynamics, not cancel them out. That is the topic of this course.

Surprisingly, many formal control ideas do not support the idea of "exploiting" the dynamics. Optimal control formulations (which we will study in depth) allow it in principle, but optimal control of nonlinear systems is still a relatively ad hoc discipline. Sometimes I joke that in order to convince a control theorist to consider the dynamics, you have to do something drastic, like taking away her control authority - remove a motor, or enforce a torque-limit. These issues have created a formal class of systems, the underactuated systems, for which people have begun to more carefully consider the dynamics of their machines in the context of control.


According to Newton, the dynamics of mechanical systems are second order ($F = ma$). Their state is given by a vector of positions, $\bq$ (also known as the configuration vector), and a vector of velocities, $\dot{\bq}$, and (possibly) time. The general form for a second-order control dynamical system is: $$\ddot{\bq} = {\bf f}(\bq,\dot{\bq},\bu,t),$$ where $\bu$ is the control vector.

Underactuated Control Differential Equations

A second-order control differential equationThis definition can also be extended to discrete-time systems and/or differential inclusions. described by the equations \begin{equation} \ddot\bq = {\bf f}(\bq, \dot\bq, \bu, t) \label{eq:underactuated_def}\end{equation} is fully actuated in state $\bx = (\bq, \dot\bq)$ and time $t$ if the resulting map ${\bf f}$ is surjective: for every $\ddot\bq$ there exists a $\bu$ which produces the desired response. Otherwise it is underactuated (in $\bx$ at time $t$).

As we will see, the dynamics for many of the robots that we care about turn out to be affine in commanded torque, so let's consider a slightly constrained form: \begin{equation}\ddot{\bq} = {\bf f}_1(\bq,\dot{\bq},t) + {\bf f}_2(\bq,\dot{\bq},t)\bu \label{eq:f1_plus_f2}.\end{equation} For a control dynamical system described by equation \eqref{eq:f1_plus_f2}, if we have \begin{equation} \textrm{rank}\left[{\bf f}_2 (\bq,\dot{\bq},t)\right] < \dim\left[\bq\right],\label{eq:underactuated_low_rank}\end{equation} then the system is underactuated. Be careful, though -- sometimes we will write equations that look like \eqref{eq:f1_plus_f2} but tack on additional constraints like $|\bu|\le 1$; as we will discuss below, input limits and other constraints can also make a system underactuated.

Note also that we are using the word system here to describe the mathematical model (potentially of a physical robot). When we way that the system is underactuated, we are talking about the mathematical model. Imagine a two-link robot with two actuators, a typical model with rigid links could be fully actuated, but if we add extra degrees of freedom to model small amounts of flexibility in the links then that system model could be underactuated.

Notice that whether or not a control system is underactuated may depend on the state of the system or even on time, although for most systems (including all of the systems in this book) underactuation is a global property of the model. We will refer to a model as underactuated if it is underactuated in all states and times. In practice, we often refer informally to systems as fully actuated as long as they are fully actuated in most states (e.g., a "fully-actuated" system might still have joint limits or lose rank at a kinematic singularity). Admittedly, this permits the existence of a gray area, where it might feel awkward to describe the model as either fully- or underactuated (we should instead only describe its states); even powerful robot arms on factory floors do have actuator limits, but we can typically design controllers for them as though they were fully actuated. The primary interest of this text is in models for which the underactuation is useful/necessary for developing a control strategy.

Robot Manipulators

make this image spring to life with a python movie<
Simple double pendulum. Click here for an animation.

Consider the simple robot manipulator illustrated above. As described in the Appendix, the equations of motion for this system are quite simple to derive, and take the form of the standard "manipulator equations": $${\bf M}(\bq)\ddot\bq + \bC(\bq,\dot\bq)\dot\bq = \btau_g(\bq) + {\bf B}\bu.$$ It is well known that the inertia matrix, ${\bf M}(\bq)$ is (always) uniformly symmetric and positive definite, and is therefore invertible. Putting the system into the form of equation \ref{eq:f1_plus_f2} yields: \begin{align*}\ddot{\bq} =& {\bf M}^{-1}(\bq)\left[ \btau_g(\bq) + \bB\bu - \bC(\bq,\dot\bq)\dot\bq \right].\end{align*} Because ${\bf M}^{-1}(\bq)$ is always full rank, we find that a system described by the manipulator equations is fully-actuated if and only if $\bB$ is full row rank. For this particular example, $\bq = [\theta_1,\theta_2]^T$ and $\bu = [\tau_1,\tau_2]^T$ (motor torques at the joints), and $\bB = {\bf I}_{2 \times 2}$. The system is fully actuated.

Python Example

I personally learn best when I can experiment and get some physical intuition. Most chapters in these notes have an associated Jupyter notebook that can run on Deepnote; this chapter's notebook makes it easy for you to see this system in action.

Try it out! You'll see how to simulate the double pendulum, and even how to inspect the dynamics symbolically.

Note: You can also run the code on your own machines (see the Appendix for details).

While the basic double pendulum is fully actuated, imagine the somewhat bizarre case that we have a motor to provide torque at the elbow, but no motor at the shoulder. In this case, we have $\bu = \tau_2$, and $\bB(\bq) = [0,1]^T$. This system is clearly underactuated. While it may sound like a contrived example, it turns out that it is almost exactly the dynamics we will use to study as our simplest model of walking later in the class.

The matrix ${\bf f}_2$ in equation \ref{eq:f1_plus_f2} always has dim$[\bq]$ rows, and dim$[\bu]$ columns. Therefore, as in the example, one of the most common cases for underactuation, which trivially implies that ${\bf f}_2$ is not full row rank, is dim$[\bu] < $ dim$[\bq]$. This is the case when a robot has joints with no motors. But this is not the only case. The human body, for instance, has an incredible number of actuators (muscles), and in many cases has multiple muscles per joint; despite having more actuators than position variables, when I jump through the air, there is no combination of muscle inputs that can change the ballistic trajectory of my center of mass (barring aerodynamic effects). My control system is underactuated.

A quick note about notation. When describing the dynamics of rigid-body systems in this class, I will use $\bq$ for configurations (positions), $\dot{\bq}$ for velocities, and use $\bx$ for the full state ($\bx = [\bq^T,\dot{\bq}^T]^T$). There is an important limitation to this convention (3D angular velocity should not be represented as the derivative of 3D pose) described in the Appendix, but it will keep the notes cleaner. Unless otherwise noted, vectors are always treated as column vectors. Vectors and matrices are bold (scalars are not).

Feedback Equivalence

Fully-actuated systems are dramatically easier to control than underactuated systems. The key observation is that, for fully-actuated systems with known dynamics (e.g., ${\bf f}_1$ and ${\bf f}_2$ are known for a second-order control-affine system), it is possible to use feedback to effectively change an arbitrary control problem into the problem of controlling a trivial linear system.

When ${\bf f}_2$ is full row rank, it is invertibleIf ${\bf f}_2$ is not square, for instance you have multiple actuators per joint, then this inverse may not be unique.. Consider the potentially nonlinear feedback control: $$\bu = {\bf \pi}(\bq,\dot\bq,t) = {\bf f}_2^{-1}(\bq,\dot\bq,t) \left[ \bu' - {\bf f}_1(\bq,\dot\bq,t) \right],$$ where $\bu'$ is the new control input (an input to your controller). Applying this feedback controller to equation \ref{eq:f1_plus_f2} results in the linear, decoupled, second-order system: $$\ddot{\bq} = \bu'.$$ In other words, if ${\bf f}_1$ and ${\bf f}_2$ are known and ${\bf f}_2$ is invertible, then we say that the system is "feedback equivalent" to $\ddot{\bq} = \bu'$. There are a number of strong results which generalize this idea to the case where ${\bf f}_1$ and ${\bf f}_2$ are estimated, rather than known (e.g, Slotine90).

Feedback Cancellation on the Double Pendulum

Let's say that we would like our simple double pendulum to act like a simple single pendulum (with damping), whose dynamics are given by: \begin{align*} \ddot \theta_1 &= -\frac{g}{l}\sin\theta_1 -b\dot\theta_1 \\ \ddot\theta_2 &= 0. \end{align*} This is easily achieved using Note that our chosen dynamics do not actually stabilize $\theta_2$ - this detail was left out for clarity, but would be necessary for any real implementation. $$\bu = \bB^{-1}\left[ \bC\dot{\bq} - \btau_g + {\bf M}\begin{bmatrix} -\frac{g}{l}s_1 - b\dot{q}_1 \\ 0 \end{bmatrix} \right].$$

Since we are embedding a nonlinear dynamics (not a linear one), we refer to this as "feedback cancellation", or "dynamic inversion". This idea reveals why I say control is easy -- for the special case of a fully-actuated deterministic system with known dynamics. For example, it would have been just as easy for me to invert gravity. Observe that the control derivations here would not have been any more difficult if the robot had 100 joints.

You can run these examples in the notebook:

As always, I highly recommend that you take a few minutes to read through the source code.

Fully-actuated systems are feedback equivalent to $\ddot\bq = \bu$, whereas underactuated systems are not feedback equivalent to $\ddot\bq = \bu$. Therefore, unlike fully-actuated systems, the control designer has no choice but to reason about the more complex dynamics of the plant in the control design. When these dynamics are nonlinear, this can dramatically complicate feedback controller design.

A related concept is feedback linearization. The feedback-cancellation controller in the example above is an example of feedback linearization -- using feedback to convert a nonlinear system into a controllable linear system. Asking whether or not a system is "feedback linearizable" is not the same as asking whether it is underactuated; even a controllable linear system can be underactuated, as we will discuss soon.

Input and State Constraints

Although the dynamic constraints due to missing actuators certainly embody the spirit of this course, many of the systems we care about could be subject to other dynamic constraints as well. For example, the actuators on our machines may only be mechanically capable of producing some limited amount of torque, or there may be a physical obstacle in the free space with which we cannot permit our robot to come into contact with.

Input and State Constraints

A dynamical system described by $\dot{\bx} = {\bf f}(\bx,\bu,t)$ may be subject to one or more constraints described by $\bphi(\bx,\bu,t)\ge0$.

In practice it can be useful to separate out constraints which depend only on the input, e.g. $\phi(\bu)\ge0$, such as actuator limits, as they can often be easier to handle than state constraints. An obstacle in the environment might manifest itself as one or more constraints that depend only on position, e.g. $\phi(\bq)\ge0$.

By our generalized definition of underactuation, we can see that input constraints can certainly cause a system to be underactuated. State (only) constraints are more subtle -- in general these actually reduce the dimensionality of the state space, therefore requiring less dimensions of actuation to achieve "full" control, but we only reap the benefits if we are able to perform the control design in the "minimal coordinates" (which is often difficult).

Input limits

Consider the constrained second-order linear system \[ \ddot{x} = u, \quad |u| \le 1. \] By our definition, this system is underactuated. For example, there is no $u$ which can produce the acceleration $\ddot{x} = 2$.

Input and state constraints can complicate control design in similar ways to having an insufficient number of actuators, (i.e., further limiting the set of the feasible trajectories), and often require similar tools to find a control solution.

Nonholonomic constraints

You might have heard of the term "nonholonomic system" (see e.g. Bloch03), and be thinking about how nonholonomy relates to underactuation. Briefly, a nonholonomic constraint is a constraint of the form $\phi(\bq, {\bf \dot{q}}, t) = 0$, which cannot be integrated into a constraint of the form $\phi(\bq, t) = 0$ (a holonomic constraint). A nonholonomic constraint does not restrain the possible configurations of the system, but rather the manner in which those configurations can be reached. While a holonomic constraint reduces the number of degrees of freedom of a system by one, a nonholonomic constraint does not. An automobile or traditional wheeled robot provides a canonical example:

Wheeled robot

Consider a simple model of a wheeled robot whose configuration is described by its Cartesian position $x,y$ and its orientation, $\theta$, so $\bq = \begin{bmatrix} x, y, \theta \end{bmatrix}^T$. The system is subject to a differential constraint that prevents side-slip, \begin{gather*} \dot{x} = v \cos\theta \\ \dot{y} = v \sin\theta \\ v = \sqrt{\dot{x}^2 + \dot{y}^2} \end{gather*} or equivalently, \[\dot{y} \cos \theta - \dot x \sin \theta = 0.\] This constraint cannot be integrated into a constraint on configuration—the car can get to any configuration $(x,y,\theta)$, it just can't move directly sideways—so this is a nonholonomic constraint.

Contrast the wheeled robot example with a robot on train tracks. The train tracks correspond to a holonomic constraint: the track constraint can be written directly in terms of the configuration $\bq$ of the system, without using the velocity ${\bf \dot{q}}$. Even though the track constraint could also be written as a differential constraint on the velocity, it would be possible to integrate this constraint to obtain a constraint on configuration. The track restrains the possible configurations of the system.

A nonholonomic constraint like the no-side-slip constraint on the wheeled vehicle certainly results in an underactuated system. The converse is not necessarily true—the double pendulum system which is missing an actuator is underactuated but would not typically be called a nonholonomic system. Note that the Lagrangian equations of motion are a constraint of the form \[\bphi(\bq,{\bf \dot{q}},{\bf \ddot{q}},t) = 0,\] so do not qualify as a nonholonomic constraint.

Underactuated robotics

The control of underactuated systems is an open and interesting problem in controls. Although there are a number of special cases where underactuated systems have been controlled, there are relatively few general principles. Now here's the rub... most of the interesting problems in robotics are underactuated:

Even control systems for fully-actuated and otherwise unconstrained systems can be improved using the lessons from underactuated systems, particularly if there is a need to increase the efficiency of their motions or reduce the complexity of their designs.

Goals for the course

This course is based on the observation that there are new computational tools from optimization theory, control theory, motion planning, and even machine learning which can be used to design feedback control for underactuated systems. The goal of this class is to develop these tools in order to design robots that are more dynamic and more agile than the current state-of-the-art.

The target audience for the class includes both computer science and mechanical/aero students pursuing research in robotics. Although I assume a comfort with linear algebra, ODEs, and Python, the course notes aim to provide most of the material and references required for the course.

I have a confession: I actually think that the material we'll cover in these notes is valuable far beyond robotics. I think that systems theory provides a powerful language for organizing computation in exceedingly complex systems -- especially when one is trying to program and/or analyze systems with continuous variables in a feedback loop (which happens throughout computer science and engineering, by the way). I hope you find these tools to be broadly useful, even if you don't have a humanoid robot capable of performing a backflip at your immediate disposal.


Atlas Backflip

Atlas doing a backflip and Atlas standing.
At the beginning of this chapter you have seen the Atlas humanoid doing a backflip. Now consider the robot in the two states captured in the figure above. Assuming that Atlas' actuators can produce unbounded torques $\bu$, establish whether or not each of the following statements is true. Briefly justify your answer.
  1. The state of the humanoid can be represented by the angles and the angular velocities of all its joints.
  2. While doing the backflip (state in the left figure), the humanoid is fully actuated.
  3. While standing (state in the right figure), the humanoid is fully actuated.

Trajectory Tracking in State Space

Take a robot whose dynamics is governed by equation \ref{eq:f1_plus_f2}, and assume it to be fully actuated in all states $\bx = [\bq^T, \dot\bq^T]^T$ at all times $t$.
  1. For any twice-differentiable desired trajectory $\bq_{\text{des}}(t)$, is it always possible to find a control signal $\bu(t)$ such that $\bq(t) = \bq_{\text{des}}(t)$ for all $t \geq 0$, provided that $\bq(0) = \bq_{\text{des}}(0)$ and $\dot \bq(0) = \dot \bq_{\text{des}}(0)$?
  2. Now consider the simplest fully-actuated robot: the double integrator. The dynamics of this system reads $m \ddot q = u$, and you can think of it as a cart of mass $m$ moving on a straight rail, controlled by a force $u$. The figure below depicts its phase portrait when $u=0$. Is it possible to find a control signal $u(t)$ that drives the double integrator from the initial state $\bx(0) = [2, 0.5]^T$ to the origin along a straight line (blue trajectory)? Does the answer change if we set $\bx(0)$ to be $[2, -0.5]^T$ (red trajectory)?
    Phase portrait of the double integrator.
  3. The dynamics \ref{eq:f1_plus_f2} are $n=\dim[\bq]$ second-order differential equations. However, it is always possible (and we'll frequently do it) to describe these equations in terms of $2n$ first-order differential equations $\dot \bx = f(\bx,t)$. To this end, we simply define $$f(\bx,t) = \begin{bmatrix} \dot\bq \\ {\bf f}_1(\bq,\dot\bq,t) + {\bf f}_2(\bq,\dot\bq,t)\bu \end{bmatrix}.$$ For any twice-differentiable trajectory $\bx_{\text{des}}(t)$, is it always possible to find a control $\bu(t)$ such that $\bx(t) = \bx_{\text{des}}(t)$ for all $t \geq 0$, provided that $\bx(0) = \bx_{\text{des}}(0)$?

Task-Space Control of the Double Pendulum

In the example above, we have seen that the double pendulum with one motor per joint is a fully-actuated system. Here we consider a variation of it: instead of controlling the robot with the actuators at the shoulder and the elbow, we directly apply a force on the mass $m_2$ (tip of the second link). Let $\bu = [u_1, u_2]^T$ be this force, with $u_1$ horizontal component (positive to the right) and $u_2$ vertical component (positive upwards). This modification leaves the equations of motion derived in the appendix example almost unchanged; the only difference is that the matrix $\bB$ is now a function of $\bq$. Namely, using the notation from the appendix, $$\bB (\bq) = \begin{bmatrix} l_1 c_1 + l_2 c_{1+2} & l_1 s_1 + l_2 s_{1+2} \\ l_2 c_{1+2} & l_2 s_{1+2} \end{bmatrix}.$$ Is the double pendulum with the new control input still fully-actuated in all states? If not, identify the states in which it is underactuated.

Underactuation of the Planar Quadrotor

Later in the course we will study the dynamics of a quadrotor quite in depth, for the moment just look at the structure of the resulting equations of motion from the planar quadrotor section. The quadrotor is constrained to move in the vertical plane, with the gravity pointing downwards. The configuration vector $\bq = [x, y, \theta]^T$ collects the position of the center of mass and the pitch angle. The control input is the thrust $\bu = [u_1, u_2]^T$ produced by the two rotors. The input $\bu$ can assume both signs and has no bounds.
  1. Identify the set of states $\bx = [\bq^T, \dot \bq^T]^T$ in which the system is underactuated.
  2. For all the states in which the system is underactuated, identify an acceleration $\ddot \bq (\bq, \dot \bq)$ that cannot be instantaneously achieved. Provide a rigorous proof of your claim by using the equations of motion: plug the candidate accelerations in the dynamics, and try to come up with contradictions such as $mg=0$.


  1. Steven H. Collins and Andy Ruina and Russ Tedrake and Martijn Wisse, "Efficient bipedal robots based on passive-dynamic walkers", Science, vol. 307, pp. 1082-1085, February 18, 2005. [ link ]

  2. Steven H. Collins and Martijn Wisse and Andy Ruina, "A Three-Dimensional Passive-Dynamic Walking Robot with Two Legs and Knees", International Journal of Robotics Research, vol. 20, no. 7, pp. 607-615, July, 2001.

  3. J.P.Y. Arnould and D.R. Briggs and J.P. Croxall and P.A. Prince and A.G. Wood, "The foraging behaviour and energetics of wandering albatrosses brooding chicks", Antarctic Science, vol. 8, no. 3, pp. 229-236, 1996.

  4. Wei Shyy and Yongsheng Lian and Jian Teng and Dragos Viieru and Hao Liu, "Aerodynamics of Low Reynolds Number Flyers", Cambridge University Press , 2008.

  5. Xiaodong Tian and Jose Iriarte-Diaz and Kevin Middleton and Ricardo Galvao and Emily Israeli and Abigail Roemer and Allyce Sullivan and Arnold Song and Sharon Swartz and Kenneth Breuer, "Direct measurements of the kinematics and dynamics of bat flight", Bioinspiration \& Biomimetics, vol. 1, pp. S10-S18, 2006.

  6. Michael S. Triantafyllou and George S. Triantafyllou, "An efficient swimming machine", Scientific American, vol. 272, no. 3, pp. 64, March, 1995.

  7. Vance A. Tucker, "Gliding Flight: Speed and Acceleration of Ideal Falcons During Diving and Pull Out", Journal of Experimental Biology, vol. 201, pp. 403-414, Nov, 1998.

  8. Eric D. Tytell and George V. Lauder, "Hydrodynamics of the escape response in bluegill sunfish, Lepomis macrochirus", The Journal of Experimental Biology, vol. 211, pp. 3359-3369, 2008.

  9. D.N. Beal and F.S. Hover and M.S. Triantafyllou and J.C. Liao and G. V. Lauder, "Passive propulsion in vortex wakes", Journal of Fluid Mechanics, vol. 549, pp. 385–402, 2006.

  10. Jean-Jacques E. Slotine and Weiping Li, "Applied Nonlinear Control", Prentice Hall , October, 1990.

  11. Anthony Bloch and P. Crouch and J. Baillieul and J. Marsden, "Nonholonomic Mechanics and Control", Springer , April 8, 2003.

Table of contents Next Chapter