## Abstract

A new method for analyzing kinematic patterns during smooth movements is proposed. Subjects are asked to move the end of a two-joint manipulandum to copy a smooth initial target path. On subsequent trials the target path is the subject's actual movement from the preceding trial. Using Principal Components Analysis, it is shown that the trajectories have very low dimension and that they converge toward a linear superposition of the first few principal components. We show similar results for handwriting on an electronic pen tablet. We hypothesize that the low dimensionality and convergence are attributable to combined properties of the internal controller and the musculoskeletal system. The low dimensionality may allow for efficient descriptions of a large class of arm movements.

For unconstrained human hand movements, there is a very large set of possible trajectories determined both by the path as well as by the time at which each point on the path is reached. Accessing or computing such trajectories would require significant motor memory storage and computational power. This consideration leads to the question of whether the human motor system might use a simplified strategy that restricts the set of possible movement trajectories (Bernstein, 1967). Several properties of human movement patterns are well known, including smoothness (Hogan, 1984; Flash and Hogan, 1985; Uno et al., 1989), interjoint torque constraints (Gottlieb et al., 1996), and the “2/3-power law” relating speed to curvature (Viviani and Terzuolo, 1982; Lacquaniti et al., 1983). It is not evident how these observed properties of movement might lead to computational simplifications.

Using Principal Components Analysis (PCA), recent studies of human kinematics have suggested that in several different cases movements can be described as a linear combination of a small number of components. Eighty percent of the variance of grasping hand movements is captured using only two principal components (Santello and Soechting, 1997;Santello et al., 1998), and similar results have been found for typing (Soechting and Flanders, 1997). PCA has also been used to analyze lip motion during speech (Ramsay et al., 1996), trunk bending (Alexandrov et al., 1998), and gait (Loslever et al., 1994; Borghese et al., 1996;Olney et al., 1998), and in all cases the number of components needed to describe the movements was significantly fewer than the total number of possible degrees of freedom. Recent results suggest that 94% of the variance in the pattern of forces generated in the frog hindlimb in response to vestibular stimulation can be explained using only five components (d'Avella and Bizzi, 1998), and 75–90% of the variance of rabbit jaw muscle EMG during voluntary chewing can be explained using only three components (Weijs et al., 1999). This data, along with earlier results on superposition of fields of forces with spinal cord microstimulation (Bizzi et al., 1991; Mussa-Ivaldi et al., 1994; Sergio and Ostry, 1995), provides a physiological correlate to the psychophysical results.

We hypothesize that the trajectory followed by the hand during planar curved movements can be approximated as a linear combination of a small number of principal components. Because human movement has great flexibility and may change depending on the specified task, we developed a new practice methodology to investigate the unconstrained behavior of the human arm. As a subject attempts to copy a curved figure, each movement that he or she makes is used as the target figure for the next trial. We refer to this technique as “iterated practice.” Although an initial target is provided, subsequent movements can modify this target toward a class of preferred movements. The trajectory followed on successive movements becomes progressively smoother with an increasing fraction of the variance accounted for by a decreasing number of principal components. We show that this behavior is a property of smooth linear low-dimensional systems, and we suggest that it arises as a combined effect of an internal human movement controller and mechanical properties of the arm.

## MATERIALS AND METHODS

Experimental techniques were approved in accordance with MIT's policy statement on the use of humans in experiments, and informed consent was obtained from eight right-handed subjects. Subjects grasped the end of a two-joint horizontal planar manipulandum (Fayé, 1986) with their dominant hand while seated in a chair aligned with the center of the workspace. A point on a 14 inch video screen placed slightly above eye level tracks the movement of the end of the manipulandum. To start a trial, the subject must move the manipulandum so that the point on the screen lies within a small box corresponding to a 2 cm square in the center of the manipulandum workspace. As soon as the point comes to rest within this box, a smooth target curve is displayed in the lower left-hand corner of the screen. Subjects are asked to copy the approximate shape of the figure smoothly and rapidly within 0.5 sec. There are no other timing constraints, and in particular, subjects are free to choose movement velocities at each point on the curve. The subjects perform their copy in the center of the screen at a distance of several inches from the displayed target curve so that tracing is not possible. The trial starts when the manipulandum leaves the start box and ends when the manipulandum is again brought to rest, at which time the full path of the subject's movement is displayed. Trials lasting >0.5 sec sound a warning buzzer and are discarded. After the first few minutes of practice, subjects had no difficulty in accomplishing movements in <0.5 sec. The horizontal (tangential) and vertical (radial) positions of the manipulandum endpoint were sampled at 100 Hz by a 66 MHz Intel Pentium computer. In some cases, the x, y, and z components of elbow position were also sampled using a Polhemus position sensor. The elbow movement was not constrained. In a related experiment, four subjects moved a pen on the surface of a smooth tablet (Calcomp), and pen tip positions were recorded at 30 Hz. The experiment was otherwise similar.

For each block of trials, the first 2 target paths are identical, and they are generated automatically using: Equation 1 Equation 2where x˙(t) and y˙(t) are the path velocities in centimeters per second, the amplitudes α are chosen randomly between 0 and 1, and the phases φ are chosen randomly between −π and π. The dynamic trajectory information is arbitrary, and the display does not include timing or velocity information. Note that although the static shape of the target is described by only 12 variables, the set of possible trajectories that accomplish this path has very high dimensionality because the subjects are free to choose from an infinite number of possible sets of hand velocities.

On trials beyond the second, the target hand path is the average of the recorded hand trajectories on the previous two movements, where the average x and y coordinates are computed point-by-point at each time during the movements. Averaging of two previous paths reduces the effect of small hand tremors or unintentional movements. Points are aligned in time by scaling pairs of movements with linear interpolation to have the same total time from movement onset to return to a stationary position. The size of the displayed target path is normalized so that the larger of the x or y deviation is constant.

Data was collected in blocks of 20 trials, with each block initiated by a new random target path. An example set of hand paths from a single experiment is shown in Figure1*A*. Experimental sessions lasted 1 hr, during which time 60–80 movement blocks (1200–1600 movements) were performed. Subjects were seen once or twice weekly over a period of 3 months.

PCA was used to analyze the variability in trajectory shape. For each movement, 50 points spaced equally in time from the start to the end of the trajectory were extracted. Thus, all movements are effectively scaled to the same duration. A 100 element column vectorm⃗ was constructed for each movement by joining the x and y coordinates m_{x}(t) and m_{y}(t) of the 50 points so thatm⃗ = < m_{x}(1), … , m_{x}(50), m_{y} (1), … , m_{y}(50) >. (If elbow motion is recorded, then 50 x, y, and z components of elbow position are appended to the hand movement vectorm⃗.) To compute the principal components, the mean vector is subtracted from each of a set of K movement vectors m⃗_{j}, and the covariance matrix is formed:
Equation 3The eigenvectors c⃗_{i} (principal components) are then calculated using Matlab (version 5.0, MathWorks). To allow comparison across movement trials, all 1200–1600 movements made by a subject on a given day are used to calculate a single set of eigenvectors. The x and y components of the eigenvectors are then separated to yield c_{ix}(t) and c_{iy}(t), and example components are shown in Figure 1*B*. Note that the components themselves represent smoothly curved trajectories. They also satisfy an approximate power law relating velocity to curvature (Viviani and Terzuolo, 1982; Lacquaniti et al., 1983), as shown in Figure1*C*. There is a high baseline correlation between principal components from different subjects because most movements are smooth, and the early components are thus dominated by low-frequency smooth movement terms.

Any movement vector can be exactly reconstructed as a superposition of the full set of principal components c⃗_{i}according to:
Equation 4where the number of dimensions is 100 (250 if elbow motion is included). If the movements are approximated with a smaller number of components n < 100, then we can write:
Equation 5so that:
Equation 6
Equation 7where n is the number of necessary components and is much less than the maximum possible N (100). For any given number of components n, the approximation error is:
Equation 8and the error e_{n} decreases as the number of components n increases.

## RESULTS

Figure 2*A* shows histograms over all subjects and all days of the approximation error e_{n}^{2} for one to five components. The principal components are calculated from the entire set of trajectories on each day. The results are not significantly different if components are calculated from only the final movement of each block, but this leads to increased variability caused by the decreased number of samples. The first five components account for an average of 90% of the hand movement variance. Figure 3shows the decrease in component variance (eigenvalue) with increasing component number for one subject on a typical day. Note the rapid decrease after the first few components, with two orders of magnitude decrease after the first 10 components and 10 orders of magnitude after the first 20.

Because of the high dimensionality of the space of possible movements, there is no single measure that describes the similarity between components from different subjects. In fact, we are most interested in the similarity between the space of components from each subject. To investigate this, we can examine the ability for the components from one subject to describe movements from a different subject. Low error for a small number of components indicates similar approximation abilities and a similar space of components. Figure2*B* approximates the movement error for all subjects using the components from subject 1, thereby demonstrating the similarity between component spaces from different subjects and at different times. The actual components may be very different, because there may be shuffling or varying linear combinations of the first few components.

Figure 2*C* shows that inclusion of three additional dimensions of elbow position at each time point does not significantly increase the required dimensionality. This implies that the same small set of components can be used to describe both hand and elbow movement, and that the hand and elbow trajectories are correlated for this task. Figure 2*D* shows similar results for the approximation error using a pen tablet instead of the manipulandum to record movements.

Figure 4 shows a typical trial block from subject 5, as well as approximations of each trial movement using from one to five components. As the iterated practice progresses, the actual subject movements change to shapes that are better approximated by a smaller number of components. Note that the first component does not contribute significantly to this particular block of trial movements.

On average, the approximation error e_{n}^{2} for the first few components decreases with iterated practice, indicating that these components represent progressively more of the data variance and that the movement converges toward a superposition of fewer and fewer components. The effect is shown for all subjects in Figure5*A*. The figure shows the percentage of variance accounted for, averaged over blocks of 20 trials (400 movements) on multiple days for each subject. Here, principal components are computed separately within each block of 400 movements to allow comparison of the average errors. In all cases, the combination of the first few components accounts for progressively more of the variance. In some cases, although the percentage accounted for by the first five components does not change significantly, the movements converge so that the first 3–4 components contain a larger proportion of the variance than initially. Also note that the first component may actually lose power in some series, but that this power is recovered in the second component as the set of movements “rotates” in the high-dimensional space toward the low-dimensional projection.

Convergence is not simply an effect of practice, because Figure5*B* shows that repeated presentation of the same target does not lead to this phenomenon. Figure 6shows the average convergence behavior for all subjects for 2 and 3 components, with error bars indicating 1 SD from the between-subject mean. Although the slope of the average curve is not significant, the average downward trend is significant (p < 0.01). Figure 7 shows the distance from each movement in an iterated sequence to the final movement in the block. Although the progression toward this final movement is steady, it does not stabilize at any time. If movements progressed toward a particular set of movements, we would expect that at least in some cases this curve would approach zero at a low iteration number and then remain near zero. This pattern is not seen. Figures 6 and 7 show that although iterated practice converges toward a linear subspace, it does not converge to a fixed set of preferred trajectories such as those in a memory-based controller (Atkeson, 1989, 1990).

## DISCUSSION

We have shown that the trajectories followed by the hand while performing smooth planar movements can be described by a small number of principal components. These components satisfy an approximate power law relating speed and curvature. The approximation by a small number of components is accentuated with iterated practice, for which an increasing fraction of the variance of the movements can be described by a decreasing number of components. These results therefore show that arm movement trajectories provide a further example of low dimensionality in human motor behavior.

The methods used here operate within the Cartesian coordinate system. Although there is some evidence to suggest that visual–motor tasks are in fact planned in Cartesian coordinates (Morasso, 1981; Wolpert et al., 1995), our results do not address this question, and the same type of analysis could have been performed in joint or body-centered polar coordinates.

Trajectories with a small number of components are a property of certain classes of very smooth movements. For example, trajectories that are generated by splines, Fourier series, or from linearly filtered noise will all have low dimensionality. In particular, a second-order mechanical system with mass, stiffness, and damping may generate low-dimensional trajectories when driven by white noise. We now provide a mathematical analysis of iterated practice for linear systems, followed by a simulation of iterated practice for a two-joint planar arm with a smooth equilibrium point controller (Feldman, 1974;Bizzi et al., 1984).

Consider a system in which the mapping from one movement to the next can be described by a linear system A: m⃗_{k} →m⃗_{k+1}. A represents the entire process of seeing the target path generated from the previous movement, planning the next trajectory, sending motor commands to the muscles to execute the trajectory, and then performing the next movement. If the initial target movement is m⃗_{0}, the k th movement in the iterated practice series ism⃗_{k} = A^{k}m⃗_{0}. (There is an additional effect from rescaling of the movements to be at approximately the same size. We will ignore this because it does not affect the conclusions.) This process is known to converge toward the first eigenvector of the matrix A (Golub and Van Loan, 1983). If we perform a principal components decomposition m⃗_{k} = ∑_{i}a_{i}(k)c⃗_{i} at each step, then the change in each component for step k is given by:
Equation 9where λ_{i} is the i th eigenvalue of A, and c_{i} is its i th eigenvector. This means that if we order the components from largest to smallest with λ_{1} > λ_{2} > … , then during iterated practice the higher-numbered components will decrease fastest so that the lower components a_{1}, a_{2}, and so on account for an increasing percentage of the data variance. This effect is greatest for low-dimensional A with rapidly decreasing eigenvalues λ_{i}. Therefore, the property of convergence toward a low-dimensional representation can be explained if the combination of movement controller and musculoskeletal mechanics behaves as a low-dimensional linear system.

This raises the question of whether the musculoskeletal mechanics alone can account for the data. The mechanics are not able to perform the required translation from the visual representation of a path (which has no timing or velocity information) into the temporal description of a trajectory, but the mechanics can act as a temporal smoothing operator that reduces the apparent dimensionality. However, we now show that simulation of a two-joint mechanical arm with equilibrium point control is not sufficient by itself to explain the convergence results. For the simulation we used standard equations for the dynamics of a two-joint planar robot arm (for example, see McCarthy, 1986) with Euler integration. Mechanical parameters were taken from Amis et al. (1979), and an equilibrium-point controller was used to map from a desired trajectory θ̂ at each joint (in joint coordinates) into torques according to τ = K(θ̂ − θ) − Bθ˙ (Flash, 1987). Stiffness K and damping B coefficients were set as constant at 2 Nm/rad and 0.4 Nm · rad^{−1} · sec^{−1}, respectively, based approximately on human measurements from Katayama and Kawato (1992) and Bennett et al. (1992). Initial target trajectories were generated from Equations 1 and 2, and 20 blocks of iterated trials were simulated. At each iteration, the target for the next movement was the average of the two previous trajectories (including timing information), because the mechanical system could otherwise not make use of the visual representation of a path.

Figure 8 shows the first 10 iteration trials, and Figure 9 shows the decrease in approximation error for 1–5 components as a function of trial number. Although the general features of increasing smoothness and decreasing number of components are present, the simulated trajectories in Figure 8 do not always converge and frequently appear to jump between different alternatives. In particular, note the increase in error on the last two trials in Figure 9. This occurs despite the apparently low variability in the trajectories shown in Figure 8because of the fact that the final trajectories in each block of trials are poorly represented by the set of principal components computed for the entire set of movements. This effect was seen on multiple simulations and suggests that although the movements are converging toward a low-dimensional space, it is not the same low-dimensional space as that computed for the initial movements. This behavior differs from the human data and the analysis of linear systems discussed above, for which convergence is expected to be approximately monotonic, as in Equation 9. The simulation results therefore suggest that the convergence behavior cannot be explained solely on the basis of the mechanical system with an equilibrium point controller. Therefore, the smoothness and low dimensionality may be attributable to the combination of an internal movement controller and the musculoskeletal mechanical system.

In conclusion, the human data shows that the final resulting movements are a set of trajectories of low dimensionality relative to the 100-dimensional complete set of possibilities. Similar results hold for handwriting as for arm movements, and when elbow movements are measured they are found to correlate with the hand movements in such a way that the dimensionality does not significantly increase. Simulation results suggest that the low dimensionality and convergence of the trajectories are attributable to a combination of the movement controller and the musculoskeletal system, but further research will be needed to determine the relative contribution of each.

We emphasize that our results provide only a description of the movements, and therefore they do not indicate how these trajectories are generated. Furthermore, our results do not indicate whether this phenomenon represents an intended behavior of the system or merely a necessary but unintended consequence of the mechanics. Nevertheless, it is possible that the low dimensionality may allow the controller to use a simplified strategy to reduce the storage and computational requirements needed to express variability within the set of curved hand trajectories.

## Footnotes

This research and Dr. Bizzi's laboratory were supported by National Institutes of Health Grant NS09343 and ONR Grant N00014-95-1-0445 to Dr. Emilio Bizzi. I was supported during part of this research by a McDonnell–Pew postdoctoral fellowship. I thank Emilio Bizzi, Simon Giszter, Francesca Gandolfo, Brian Benda, and Margo Cantor for discussions and assistance with these experiments. I also acknowledge the diligence and insight of the anonymous reviewers who contributed significantly to revision of this manuscript.

Correspondence should be addressed to Terence D. Sanger, Department of Movement Disorders, Toronto Western Hospital, MP-11, 399 Bathurst Street, Toronto, Ontario M5T 2S8, Canada. E-mail: tds{at}ai.mit.edu.