Department of Neuroscience, University of Minnesota, Minneapolis,
Minnesota 55455
 |
INTRODUCTION |
In recent years, it has become evident that the
study of movement in two- and three-dimensional space introduces
questions that are not apparent in the study of one-dimensional
movement. With respect to arm movements, this has been demonstrated by
various investigators who have recorded from motor and premotor
cortical areas during movements to stationary targets and have shown
movement direction to be prominently represented in the
activity of these neurons (e.g., Fu et al. 1995
;
Georgopoulos et al. 1986
; Kalaska et al.
1997
; Schwartz et al. 1988
). Much less is known
about the control of arm movements for tasks in which the target itself is moving in space, such as tracking or intercepting a target moving in
two dimensions (Johnson et al. 1999
; Port et al.
1997
; Viviani et al. 1987
).
Sensory reception, neural computation, and motor output all require a
finite amount of time. Therefore time delays are inherent in the task
of manually tracking a moving target. However, during the normal
tracking of a predictable target moving along one dimension, the
tracking error can be very small (Poulton 1974
),
implying that predictive algorithms are employed by the nervous system. Studies of tracking in one dimension have shown that this predictive behavior is generated by a velocity error signal in combination with a
positional error signal (Poulton 1974
; Viviani et
al. 1987
; see also Lisberger et al. 1987
). The
question then can be posed: what is the form of the error signal for
tracking in two dimensions?
The current study was undertaken to determine how speed and directional
error signals are used in two-dimensional tracking. To this end, we
asked subjects to track a target that moved initially in a straight
line and then changed direction (and sometimes speed) abruptly. We
identified a rather unexpected strategy. A conceptual model based on a
constant time to intercept could predict the new direction of the
finger motion as well as its maximum speed. This conceptual model
provided the basis for a formal quantitative model in which direction
and speed are the controlled variables.
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METHODS |
Motor task
The manual tracking of targets moving in two dimensions was
assessed in six different experimental conditions. Before describing each of the experimental conditions in detail, we will describe those
aspects which were common to all experiments.
Subjects sat in front of a touch-sensitive computer video monitor. Seat
height was adjusted such that each subject was comfortable and could
easily reach all areas of the video screen. Room lighting was dimmed to
increase the contrast of the display. No restrictions were imposed on
head or eye movements. Each experiment typically consisted of 300-360
trials and lasted from 45 min to 1 h. The subjects gave their
informed consent to the experimental procedures, which were approved by
the Institutional Review Board of the University of Minnesota.
All subjects were right handed and were asked to track, with their
right index finger, the motion of a target presented on the video
monitor. In most experiments, a box 1.6 cm per side initially appeared
1.6 cm from the top edge of the screen to indicate the starting
position for the subject's finger. When the subject placed his or her
finger in the box, a round target 1.6 cm in diameter appeared at the
same edge of the screen and began to move at a constant downward
velocity toward the box (see Fig. 1).
Subjects were to begin tracking the target as soon as it entered the
box. In all cases, the target initially moved at a constant speed and
in a direction that was constant from trial to trial. After the target
had traveled a random distance of from 10.9 to 17.4 cm, it made a
single abrupt change in direction. On average, the target motion
changed direction when the target was in the middle of the screen
~1-2 s after the start of the trial.

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Fig. 1.
An example of tracking performance during a directional change in
target motion. Top: results from a single trial. The
thin line denotes the path of the target with the arrows indicating the
direction of target motion. The open arrow (slightly below the start of
the target's trajectory) marks the starting position of the finger.
After the change in target direction, the position of the finger and
position of the target are connected every 100 ms by a thin straight
(isochronic) line. Inset: description of how angular
changes, both of the target and of the finger, are defined with
counterclockwise rotations from the vertical defined positive.
Bottom: all 10 trials from this subject.
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Experiment 1: tracking a target moving at a constant speed
In this experiment, the target appeared at the middle of the top
edge of the screen, and moved straight downward at a speed of 10.8 cm/s. Then after the target had traveled a random distance, it made an
abrupt change in direction to 1 of 24 equally spaced directions. These
directions were varied randomly from trial to trial. The speed of the
target remained constant throughout the experiment. Four subjects
participated in this experiment.
Experiment 2: tracking an obliquely moving target
To determine whether the results from experiment
1 could be generalized to any initial direction, the experiment
was repeated, with one modification: the initial direction of finger
tracking was rotated counter-clockwise through 135°. Therefore the
start box for the subject appeared in the lower left-hand corner of the
video screen rather than at the top middle. The initial target motion
was upward and rightward, rather than straight downward. As in
experiment 1, target motion changed unpredictably to 1 of 24 equally spaced directions. Four subjects participated in this experiment.
Experiment 3: the effect of target speed on tracking
In this experiment, the target again appeared at the top, middle
section of the screen and initially moved straight downward. At a
random point in time, the target then changed to one of six equally
spaced directions. The speed of the target remained constant throughout
any particular trial but was varied randomly across trials. Four speeds
were used: 5.4, 10.8, 16.2, and 21.7 cm/s. Five subjects participated
in this experiment.
Experiment 4: tracking during an abrupt change in speed
In experiments 1-3, during any particular trial,
only the direction of the target's motion varied. Experiment
4 was conducted to determine whether the results from these three
experiments generalize when target speed also changes unpredictably. In
experiment 4, the target again appeared at the middle of the
top edge of the screen, moved straight downward at a constant velocity
of 10.8 cm/s, and then changed to 1 of 12 equally spaced directions. However, the target sometimes also changed speed (unpredictably) at the
same time it changed direction. In one third of the trials, the target
abruptly slowed from its initial speed of 10.8 cm/s to a speed of 5.4 cm/s. In another third, it abruptly increased speed to 16.2 cm/s. In
the last third, it maintained its original speed of 10.8 cm/s. Six
subjects participated in this experiment.
Experiment 5: constant vertical velocity/variable horizontal
velocity
As in experiment 1, the target initially moved
downward at a speed of 10.8 cm/s. The motion of the target then changed
unpredictably to 1 of 12 directions. For 7 of these 12 directions,
target speed also underwent a step change. In these instances, the
vertical component of velocity was held constant throughout the entire trial and the horizontal velocity underwent a stepwise change from 0 to
some new constant value. Seven values of horizontal velocity were used
such that the resulting directional change of the target was 0, ±22.5,
±45, or ±67.5°. Consequently, the speed and direction of the
target's motion changed simultaneously as in experiment 4. For the remaining five directions, the target's motion changed to one
of five upward directions (180, ±150, and ±120° with respect to the
downward direction); the target's speed being held constant throughout
the trial (as in experiment 1). Four subjects participated
in this experiment.
Experiment 6: the effect of target acceleration on tracking
The parameters for experiment 6 were nearly identical
to those for experiment 4 except that acceleration was
changed instead of speed. In experiment 6, the target either
accelerated or decelerated at a rate of 5.4 cm/s2
or maintained its original speed of 10.8 cm/s, at the time when its
direction of motion changed. Five subjects participated in this experiment.
Recording system
The experiments were performed using a touch screen (Elo Touch
Systems, TN) mounted over a standard 20-in computer monitor (Mitsubishi
Diamond Scan 20 M). The touch screen has a spatial resolution of 0.08 mm. The target motion and recording of finger position were controlled
by a laboratory computer using custom software. The position of the
finger was recorded at a rate of 100 Hz. Target location was updated at
a rate of 60 Hz, equal to the refresh rate of the video monitor. The
output of the touch screen was scaled and aligned with the video image
through the use of cubic polynomials and a rectangular reference grid
of target positions (see Flanders and Soechting 1992
).
Data analysis
Data were averaged by aligning the trials on the point at which
the target changed direction. All subsequent analysis was performed on
averaged data. Velocity was calculated by numerically differentiating
the position data and digitally smoothed using a two-sided exponential
filter with a cutoff frequency of 12 Hz. As will be shown in
RESULTS, after the target changed direction, the finger
maintained the original target direction for a reaction time period,
changed direction, initially headed in a nearly straight line to
intercept the target, and then finally curved to merge with the new
target direction. This heading to intercept the target was defined by
computing the inverse tangent of the ratio of the horizontal and
vertical velocities at 350 ms after the change in target direction.
This point in time was chosen because it is generally in the middle of
the straight interception period, at a time when tracking speed was
increasing (see Figs. 4B, 8, and 11).
To determine when two averages of either speed or direction began to
differ from each other, we performed a t-test at each point
in time. The averages were said to diverge once the 0.05% confidence
level was reached and the two series remained separated by at least
this level of confidence for the next 70 ms. To determine reaction time
(defined as the interval between the time at which target motion
changed direction and the first observable change in the finger's
trajectory), a baseline period was defined by averaging both direction
and speed data over the interval from 150 ms before the target changed
direction to 100 ms after the target changed direction. The standard
deviation of direction and speed was also computed for this same 250-ms
interval. The subject's reaction time was then defined as the point in
time beyond this baseline interval when either finger speed or
direction exceeded the 2 standard-deviation limit and continued to
exceed it for at least 30 ms.
 |
RESULTS |
Response to a change in target direction (experiment 1)
To study manual tracking in two dimensions, we began with the
simplest experiment, that of a target moving downward at a constant speed and making a single change in direction. Figure 1,
top, shows the result for one trial of tracking. The path of
the target is shown by the thin line. The direction of target motion is
indicated by arrows. In this example, the target changed direction to
= 135°. The path of the finger is shown by the thick line.
(During the vertical segment of the target's motion, the path of the
finger obscures the path of the target.) To demonstrate how the motion of the finger with respect to the target evolved over time, the position of the finger and the position of the target were joined by a
thin (isochronic) line, every 100 ms, starting at the point where the
target changed direction. After this point in time, the finger
maintained its original downward trajectory for a period of time,
slowed in speed to change direction, then accelerated to reacquire the
target (see Fig. 4B). For this example, the reaction time
was found to be 230 ms using directional data and 210 ms using speed.
For this subject, for all directions, the average reaction time was
239 ± 25 (SD) ms for direction and 235 ± 26 ms for speed.
Averaging across all directions for all subjects, the reaction time was
229 ± 24 ms for direction and 227 ± 28 ms for speed. There
was a statistically significant effect of target direction on reaction
time (ANOVA, P < 0.05). However, a post hoc comparison
(Tukey HSD) showed that the reaction times did not depend significantly
on the amount by which the target changed direction for changes
exceeding 30°. For smaller changes in target direction, the estimated
reaction times were about 30 ms longer, but these estimates are not as
reliable because the signal to noise ratio is much smaller in these
cases (see Fig. 4). These reaction times are in general agreement with
previous findings (Hanneton et al. 1997
; Poulton
1974
).
Figure 1 illustrates a general aspect of our results: after the
finger's motion changed direction, the hand initially headed in a
nearly straight line before curving to merge with the path of the
target. It is clear that this new heading is not directed toward the
current location of the target. (The target's location can be noted by
considering the isochronic line that most closely connects finger and
target location at the time of the directional change.) Rather, the
finger heads in a direction anticipating the future location of the target.
In Fig. 1, bottom, all trials from this subject for this
direction are shown with the trials aligned on the point at which the
target changed direction. The consistency in the handpaths illustrated
was typical of the results we obtained in this and the other subjects.
We computed the deviation of finger position (the square root of the
sum of the variances in X and in Y). For this
example, the average deviation of the finger position after the change
in target direction was 0.56 cm. This deviation was not significantly
related to target direction (slope not significantly different from 0, P > 0.36). Across all subjects and directions the
average deviation was 0.63 ± 0.1 cm. Since this value was fairly
small, we restricted our analysis to averaged data.
Figure 1 shows the results from one out of 24 target directions tested
in this experiment. Figure 2 summarizes
the results that were obtained from one subject for 8 of the 24 directions, the dotted lines denoting the paths of the target. The
finger trajectories begin to diverge from a common point, and during the reacquisition of the target, the path of the finger appears to be
reasonably straight for a considerable period of time. Finally, once
most of the positional error has been eliminated, the path of the
finger curves to merge with the path of the target. Therefore while the
movement is continuous, for the purpose of discussion, we may consider
it as occurring in four steps: a "reaction phase," in which the
subject continued on the original target heading, a change in
direction, a "reacquisition phase," in which the subject moved in a
relatively straight, anticipatory path to reduce the error between the
target and the finger, and a gradual "merging" of finger velocity
with target velocity.

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Fig. 2.
Tracking paths for 8 of 24 target directions. Dotted lines represent
the path of the target and the thick lines represent the average
trajectories of the finger. Inset: approximation to the
behavior: the finger trajectory is represented by 2 straight lines.
With this approximation, the finger appears to intercept the target at
a constant time, represented by the circle centered on the point where
the target changes direction. Thin lines emanate from the finger
position at the end of a constant reaction time (250 ms) and intersect
the target paths on the perimeter of the circle. Note that these lines
generally parallel the straight line portion of the finger path
following the reaction time. (The fit between the model and
experimental data are better for target changes to the right, as the
finger position on the touch screen deviates slightly for right-handed
subjects moving toward the left hand of the screen.)
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Simple model for tracking directional changes in target motion
In an attempt to gain some understanding as to how the
reacquisition of the target is controlled by the nervous system, we developed a simple geometrical model of the subjects' behavior. In
particular, we approximated the finger path by two straight lines, one
representing the movement of the finger during the reaction phase, the
other representing the movement of the finger during the reacquisition
phase (see Fig. 2, inset). We also assumed that the reaction
time did not depend on the amount by which target motion changed
direction (see preceding text). These are clearly oversimplifications
because the finger does not change direction instantaneously, because
there is some curvature in the path of the finger, and because there
may be some slight variability in the reaction time. However, this
conceptual model allowed us to test a hypothesis that was suggested by
the data: the path of the finger merges with the path of the target at
a constant time after the target changes in direction, independent of
the amount of the directional change. (In this experiment, the target
moved a constant distance in a constant time. Accordingly, the
predicted point of interception can be represented by a circle centered on the time of the target's change in direction, as in Fig. 2.)
Because the path of the hand merged gradually with the path of the
target, we could not measure this time with any confidence. However,
using the simple model we could test a corollary of the hypothesis: the
motion of the finger during the "reacquisition phase" is in a
direction such as to intercept the target at a constant time. For the
reacquisition phase of the finger, we predicted the direction of travel
(
) such that the points of interception were a constant distance
(dt) away from the point in space at which the target changed direction, assuming a constant distance of
travel (dr) during the reaction time.
Therefore by trigonometry, for each target direction the distance the
finger must travel to intercept the target is simply
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(1)
|
Furthermore, the direction to intercept the target is given by
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(2)
|
The straight lines in Fig. 2 represent the idealized finger paths
of the model, from the point representing the reaction distance
(dr) to the point where the path of
the target intercepts the circle. The model fits the data reasonably
well. In this example, the fit appears better for counterclockwise
changes in target direction. The larger error for clockwise rotations
may be due to a slight rotation of finger position on the touch screen.
This typically occurred during leftward movements of the right-handed subjects.
To evaluate the extent to which this model fit the experimental data,
we used an error minimization algorithm (Nelder and Mead
1964
) to compute and compare the predicted heading of the finger (Eq. 2) with the heading measured experimentally.
Figure 3A shows how well the
model was able to predict the heading of the finger. The plot
illustrates the angular difference between the initial heading of the
finger and the heading of the target during the reacquisition phase
plotted as a function of target direction. The crosses represent the
average angular differences recorded for the 24 target directions for
one subject. The smooth curve represents the angular differences
calculated by the model. For this subject, a ratio of target
reacquisition distance (dt) to
reaction distance (dr) of 3.63 provided the best fit. [Assuming a reaction time of 250 ms, this would
imply a time to reacquire the target (reaction time + interception
time) of 900 ms.] The model accounted for 94% of the variance in
angular differences across directions for this subject. For the four
subjects, the ratio of
dt/dr
ranged from 2.51 to 3.63 (see Table 1),
and the variance accounted for by the model was above 0.85 in each
case.

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Fig. 3.
A comparison between the model and experimental performance.
Experimental data (+) for 1 subject and the model's prediction are
shown for the direction (A) and maximum velocity
(B) of the finger's trajectory. In A,
angular difference is defined as the difference between the angular
change of the finger and the angular change of the target. Finger
heading was determined by taking the inverse tangent of the ratio of
horizontal and vertical velocities at 350 ms after the target changed
direction. In B, the straight line represents the speed
of the target.
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The simple conceptual model also makes clear predictions about the
maximum speed of the finger during the reacquisition phase. If one is
to intercept a target moving at a constant speed at a constant time,
the average speed of the finger must scale proportionally to the
distance traveled (di). If the speed
profile is similar for each direction (e.g., is bell-shaped), then the
maximum speed should be proportional to
di. Therefore the variation in maximum finger speed with direction should be predicted by Eq. 1.
Figure 3B displays the average peak speed reached by the
finger for another subject as a function of target direction (crosses).
The smooth curve represents the prediction of the model. Finally, the
horizontal line indicates the target speed (10.8 cm/s). For this
subject, the scaling factor relating interception distance to peak
velocity was 2.73, while the variance in peak speed accounted for by
the scaled distance was 0.93. For the four subjects, the scaling factor relating interception distance to peak velocity ranged from 2.70 to
4.54 (Table 1), and the variance in peak speed during the reacquisition
period accounted for by the distance to the reacquisition circle ranged
from 0.89 to 0.94.
To better demonstrate the modulation of the speed profile as a function
of interception distance, finger speed was plotted in two different
formats in Fig. 4. Figure 4A
shows how speed varied with time for one subject for 12 of the 24 target directions. The traces all begin at the time the target changed
direction; the baseline indicates the speed of the target. In each
case, initially the speed of the finger was slightly slower than the target's speed, indicating that this subject was slowly starting to
fall behind the target (perhaps anticipating the change in target
direction). Then after a nearly uniform period of time (the subject's
reaction time), the finger's speed changed, first slowing to allow for
the change in direction of the finger, then accelerating to reacquire
the target. (For 0°, there was no change in target direction and the
finger maintained its original velocity throughout.) As the amount by
which target motion changed direction became greater, the amount of
deceleration as well as acceleration also increased such that the time
to reacquire the target remained constant.

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Fig. 4.
The temporal profile of finger speed during target reacquisition.
A: the finger speed for 12 of the 24 target directions
for 1 subject. In each case, the baseline indicates the speed of the
target. The horizontal and vertical scales are identical for each
trace. Each trace begins at the point when the target changed
direction. The variations in speed have been superimposed for 13 of the
24 total target directions (half of the circle) in B.
Line thickness increases with increasing angular changes of the
target.
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Figure 4B, where the traces for the 13 directions ranging
from 0 to 180° (the right hemisphere) have been superimposed,
provides further support for our hypothesis. One can observe that there are only minor variations in the reaction time. Furthermore the duration of the reacquisition phase does not depend on target direction; after ~750 ms the finger has re-assumed the velocity of
the target. In summary, since the distance to intercept the target is
not constant, it appears that both the direction and speed of the
finger's motion are coordinated in such a manner that the time to
intercept, or possibly the distance the target travels before
interception, is held constant.
Obliquely moving targets (experiment 2)
The initial path of the finger in the first experiment was always
straight downward. It is possible that the tracking of a downward
moving target is somehow unique or that gravity might have an effect on
tracking performance. To determine whether the results from
experiment 1 can be generalized to other tracking directions, the experiment was repeated with the target initially moving obliquely at an angle of 135°. Figure
5 shows the paths of the target and of
the finger to 8 of the 24 directions (left). As was the case
in experiment 1, the hand generally headed in a straight
line to intercept the target. Also as was true for initial downward
target motion, the simple model was able to account for the angular
differences between finger heading and target heading as well as
modulation in the finger's peak speed (right).

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Fig. 5.
Tracking obliquely moving targets. Left: path of the
target, which always started in the lower-left corner of the screen and
the average path of the finger during tracking to 8 of the 24 directions tested. Right: comparison between the model
and tracking performance of the obliquely moving targets. The
conventions are the same as those used in Fig. 3.
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For the four subjects, the ratio of target interception distance
(dt) to reaction distance
(dr) varied from 2.84 to 3.77. In this
experiment, the variance accounted for by the model ranged from 0.92 to
0.97. There was one subject who participated in this experiment as well
as in experiment 1. The results for this subject were almost
identical, with ratios of 3.71 and 3.63 respectively. Again, in this
second experiment, the peak speed for all subjects was well correlated
to the target interception distance. For the four subjects in this
experiment, the factor relating distance to peak speed ranged from 3.17 to 4.44 with the variance in peak speed accounted for by the distance
to reacquisition ranging from 0.86 to 0.95.
Effect of target speed on tracking performance (experiment 3)
In the first two experiments, the speed of the target was the same
for all trials. We observed that the initial heading of the hand (
)
was such as to reacquire the target at a constant time. Since the
target moved at a constant speed, a constant distance to intercept
(dt, Eqs. 1 and 2) is
equally consistent with the data. By examining manual tracking at
different target speeds, it was possible to differentiate these two
possibilities. To accomplish this, we repeated experiment 1 varying the speed of the target randomly from trial to trial over a
fourfold range. As will be demonstrated in the following
text, if the goal is to keep time to intercept constant, the
initial heading of the finger (
) should not depend on target speed.
However, if the goal is to keep distance (dt) constant,
should depend in a
predictable manner on target speed, becoming larger for faster speeds
(to make up for the extra distance traveled during the reaction time).
Figure 6, A and B,
shows the results from one subject for two different target directions.
The thin line represents the path of the target, which was the same
independent of target speed. The bold lines represent the average
finger paths for each of the different target speeds. There was a small
but statistically significant (ANOVA, averaged data for all subjects
and all directions, P < 0.01) effect of speed on
reaction time. A post hoc pairwise comparison showed that the reaction
time for the slowest speed was longer (13%) than for the other three
speeds. This difference in time was small (33 ms) compared with the
mean reaction time of ~250 ms. Since the reaction time is
approximately constant, the distance traveled during the reaction time
is approximately a linear function of the target speed.

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Fig. 6.
The effect of target speed on tracking performance. Thin lines indicate
the path of the target traveling at 4 speeds (5.4, 10.8, 16.2, and 21.6 cm/s), changing by 135° (left) and 60°
(right). Bold lines demonstrate the average path of the
finger for each of the 4 speeds. After the reaction time, finger paths
are parallel to each other, intercepting the target at a constant
time.
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After the finger changed direction, the four traces of the finger
position during the reacquisition phase were parallel with each other.
An ANOVA showed that for four of the five subjects, there was no effect
of speed on reacquisition direction (P > 0.05). For
the one remaining subject, linear regression showed that for only one
of six target directions was the relation between speed and
reacquisition direction significantly different from zero (with a slope
of 0.44°/cm/s, corresponding to a 7° difference in heading between
the slowest and fastest target speeds). In conclusion, the distance
traveled by the finger during the reaction time scaled with target
speed and the directions of the finger paths during the reacquisition
phase were parallel to each other at the four speeds. Therefore from
the law of similar triangles, the finger intercepted the path of the
target at a distance that also scaled with target speed. Accordingly,
since the target traveled at a constant speed throughout each trial,
the time not the distance to reacquisition
remained constant, irrespective of the speed of the target.
Response to an abrupt change in target speed (experiment 4)
In all of the experiments described so far the speed of the target
was constant and thus predictable throughout any given trial. The
question can then be posed, do the results generalize when speed as
well as direction changes unpredictably during the trial? We explored
this question by introducing, in some trials, a step change in the
speed of the target at the same time its direction changed. Since the
speed during the initial downward tracking segment was constant, the
reaction distance remained relatively constant as well. This is evident
in Fig. 7A where the traces
for all three averages overshoot the change in target direction by
nearly the same amount.

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Fig. 7.
The effect of changing target direction and target speed
simultaneously. The thin line in A represents the path
of the target. Target speed was constant (10.8 cm/s) during the
downward phase. When the target changed direction, target speed either
decreased (5.4 cm/s), increased (16.2 cm/s), or remained constant. Bold
lines show the average path of the finger during tracking. The scale
along the target path demonstrates the position of the target at a
constant time for the 3 speed levels. B: a comparison of
the direction of finger motion with that predicted by the constant time
to intercept model. The angular difference between target and finger
heading is shown for each target speed. Smooth curves represent the
angular difference predicted by the model assuming the same time to
intercept for all 3 speeds.
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The direction of the finger motion during the reacquisition phase
depended on the new speed of the target. Figure 7B shows the
results of fitting Eq. 2 to these data. The three curves of the model were calculated such that the time to intercept was the same
for all three speeds (i.e., dt was
proportional to target speed). For this subject, the model explained
89% of the variance for those trials where the target abruptly slowed,
95% of the variance for those trials where speed did not change, and
99% of the variance for those trials where the target abruptly
increased speed.
Therefore it appears that the subject was able to detect the change in
speed of the target and scale the speed of the interception trajectory
such that time to contact remained constant. This can also be
appreciated in Fig. 7A. The three tick marks are equally spaced and represent the position of the target at the modeled interception time for the three speeds. The location of these ticks
correspond well to where the extrapolated linear motion of the finger
intercepts the path of the target. The results in Fig. 7 are
representative of the results for the five subjects who participated in
this experiment. For all subjects, the constant time to intercept model
was able to fit the data at all three speeds with a considerable amount
of fidelity (Table 2).
Figure 8 demonstrates that the reaction
time for a change in target speed is similar to the reaction time to a
change in target direction. The plots provide a comparison of the two
instances in which the target either increased or decreased in speed at the time of the directional change. The dashed line indicates the time
at which the target changed both direction and speed. The top
panel describes the speed of the target, while the bottom panels show the speed and direction of the finger for both
conditions. We performed a statistical comparison between the finger
data for the two target speeds to determine the time at which the two curves first diverged (P < 0.05, see
METHODS). In Fig. 8, this time is denoted (
). For this
subject, the speed traces were found to diverge 250 ms after the target
changed speed. Note that finger speed decreases at about the same time
(~175 ms) for both target speeds, but that the finger begins to
accelerate earlier when the target speed is increased. Across all
subjects and directions the average time at which the speed of the
finger first differed significantly (P < 0.05) for
slow and fast target speeds was 270 ± 40 ms after the change in
target speed, slightly larger than the reaction time found for finger
speed to change in response to a change in target direction.

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Fig. 8.
Reaction time to a change in target speed. - - -, point in time at
which target speed and direction were varied. The target either
increased to 16.2 cm/s or decreased to 5.4 cm/s (top).
Bottom traces: time profiles of finger speed and
direction. , time at which the 2 movements diverged from each
other.
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Direction of finger motion also depended on target speed, with a
reaction time that was again comparable to that found for a change in
target direction. In this instance (Fig. 8), the direction of the
finger diverged 180 ms after the target changed speed. Across all
subjects and directions, finger direction for the two target speeds
diverged on average 280 ± 80 ms after the target changed speed.
This value is comparable with the reaction time for the finger
direction to change in response to a change in target direction.
Tracking a constant downward velocity (experiment 5)
There has been considerable work, both in terms of experimentation
and modeling, attempting to understand manual tracking performance in
one dimension (cf. Poulton 1974
; Viviani et al. 1987
). One might conjecture that tracking in two dimension
(2-D) is equivalent to two simultaneous cases of one dimensional
tracking occurring in the X and Y directions. To
ascertain whether this viewpoint was viable, we conducted the following
experiment. As in previous experiments, target direction changed
randomly through angles encompassing all 360°. However, for those
cases in which the change in direction was <90°, (maintaining a
downward directional component), the speed of the target was modified
such that the vertical (Y) velocity remained constant, and
the horizontal (X) velocity underwent a step change. If
manual tracking can be decomposed into two cases of independent
tracking along orthogonal axes, then one would expect that the addition
of an X component should not perturb the tracking in the
vertical dimension.
Figure 9, left, shows the path
of the target as well as the average path of the finger for one of
these downward trajectories. Figure 9, right, displays the
X and Y components of the target and finger
velocity. - - - indicates the time at which the target changed
direction. For the X component of finger motion, after ~200 ms the finger accelerated, exceeded, and eventually matched the
velocity of the target. At a comparable latency (~200 ms), the
Y velocity of the finger first decreased, then increased to reacquire the target, even though the Y velocity of the
target did not change. The same general pattern was seen in
all four subjects for all angles. It is therefore clear that tracking
behavior in two dimensions cannot adequately be expressed as two
independent cases of one-dimensional tracking occurring simultaneously
along orthogonal axes.

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Fig. 9.
Tracking a target with a constant downward velocity.
Left: the average target and finger paths for 1 direction for trials in which the vertical velocity was constant.
Right: horizontal and vertical motion of the finger and
the target vs. time. - - -, time at which the target changed
direction.
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Response to target acceleration (experiment 6)
In the preceding (experiment 4), we showed that target
speed influenced the direction of finger motion. Can target
acceleration also influence the direction of the reacquisition
movement? To address this question, in a final experiment, the target
either maintained its original speed or accelerated or decelerated,
coincident with the change in target direction. For the two examples
shown in Fig. 10, A and
B, there is no discernable effect of target acceleration on
the direction of finger motion. Figure 10, C-E, shows how
the movement described in the left-hand panels evolved over
time for the cases of accelerating and decelerating targets. The speed of the finger for the two movements did not begin to diverge until 590 ms after the target changed direction (arrow in Fig. 10D). For all subjects and all directions, target acceleration did not begin
to have an effect on finger speed until 490 ± 80 ms after the
target changed direction. The direction of finger motion was nearly
identical for both the accelerating and decelerating targets (Fig.
10E). For this subject, target acceleration had no
significant effect on the direction of finger motion. In only 11 of 50 cases was there a statistically significant divergence in finger
direction at any point in the movement, at an average time of 450 ± 120 ms.

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Fig. 10.
The effect of target acceleration on tracking performance.
A and B: 2 examples of tracking an
accelerating target. Thin lines indicate the path of the target for 3 acceleration profiles. During the downward phase of target motion, the
target maintained a constant speed of 10.8 cm/s. At the point at which
the target changed direction, the target speed either accelerated or
decelerated at a rate of 5.4 cm/s2 or remained constant.
The thick lines represent the finger paths for each of these
acceleration profiles. C-E: increasing and decreasing
target accelerations. The dotted line indicates the time at which the
target changed direction and accelerated. The arrow indicates the time
at which the finger speed profiles for accelerating and decelerating
targets diverged. For this subject, finger direction did not differ for
the 2 target motions.
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Quantitative modeling of manual tracking in two dimensions
A simple conceptual model in which the direction of finger motion
changes abruptly in response to a change in the direction of target
motion so as to intercept the target at a constant time was able to
account for a large body of experimental data. This model is compatible
with the idea of intermittent control during tracking (Miall et
al. 1986
; Young and Stark 1963
). Specifically, our results might be interpreted to imply that there is one major correction in the finger's trajectory, secondary corrections perhaps occurring as the finger's trajectory eventually merges with that of
the target. However, tracking behavior is more commonly modeled to be
under continuous control (Krauzlis and Lisberger 1994
;
Lisberger et al. 1987
; Viviani et al.
1987
). The question then arises: can the observed behavior be a
consequence of the workings of continuous feedback control? We will
show that this is indeed the case.
A CARTESIAN MODEL.
We begin with analytical models of tracking similar to models for
tracking in one dimension that have been used previously to account for
two-dimensional manual tracking (Viviani et al. 1987
).
In this form of model, the acceleration of the finger
(
F) is related to a positional
(ep) and a velocity
(ev) error signal
|
(3)
|
where
The subscripts T and F
denote the target and the finger, respectively and p is a
vectorial representation of the position {px,
py}. The coefficients
a1 and
a2 are constants, as are the two time
delays
p and
v. This
model leads to two uncoupled equations, one in x and one in
y
|
(4)
|
where epx and
epy are the x and
y components of the position error vector and
Fx and
Fy are the x and
y components of the finger acceleration.
This model is incompatible with the results presented in Fig. 9. In
experiment 5, there was no perturbation along the
y axis and therefore the positional and velocity error terms
on the left side of Eq. 4
(epy and
evy) are zero. Accordingly, the
y component of finger acceleration is predicted to be zero
by this model. Nevertheless it is instructive to consider its other
predictions in more detail.
Figure 11, left, shows the
finger trajectory and the time course of speed and direction predicted
by this model (model 1) for one subject for experiment
1. Equation 3 was solved using a Runge-Kutta scheme
(Press et al. 1992
) and an iterative error minimization algorithm to identify the four parameters
(a1,
a2,
p and
v) that gave the best fit to data. We used the
11 directions in which target motion deviated to the right and
minimized the mean square difference between finger and model speeds
and directions (directional error being weighted 1/10th as much as
speed, to give comparable weight to both). We began the model using as
initial conditions, finger speed and direction 800 ms after the onset
of target motion (i.e., at about
300 ms in the examples in Fig. 11).
As noted, the subjects' tracking speed (before the target changed
direction) was generally less than the speed of the target. The
analytical model attempted to bring tracking speed back up to the
target's value and accordingly there is an initial acceleration in the model's response (at the time the dotted and solid curves diverge in
Fig. 11).

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Fig. 11.
Comparison of the behavior of 2 analytical models in capturing tracking
behavior in trials in which the target changed direction
(experiment 1). In model 1, the finger
acceleration vector is related to vectorial error signals of position
and velocity. In model 2, acceleration is defined by its
normal and tangential component. The tangential component is related to
a vectorial error signal in position and velocity (as in model
1), but the normal component is related to a directional error
signal. Results of the modeling for 3 directions are shown for
subject 2. For each direction, the paths of the finger
and the target are shown to the left and the temporal
variation in speed and direction is shown to the right.
The dotted traces represent the performance of the models. Note that
model 2 provides a better fit to the time course of the
change in direction of finger motion as well as the time course of the
variations in speed.
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From Fig. 11, it is clear that this model gave a reasonable fit to the
data. It does predict the heading of the finger after the target
changed direction (see the left-most plots in Fig. 11 which
show the finger paths). The discrepancy in finger paths between
experimental data and the model arises because, as noted previously,
subjects lagged behind the target prior to the time at which the target
changed direction, whereas the model attempted to match finger speed to
the target speed. Model 1 accounted for 96.8% of the
variance in speed and direction for this subject, averaged over the 11 directions. (Parameter values and the goodness of fit of model
1 are reported in Table 3.)
Despite the apparent success of model 1, there are
consistent discrepancies between this model and the experimental data
for this subject as well as for the others. First, the model failed to
predict the maximum speed of the finger; maximum speed of the model
generally being substantially lower than the actual data. Second, the
model failed to match the time course of the directional change of
finger motion. It did provide a good match to data in the bottom-most
example, but it anticipated the change in direction for the other two
examples. Furthermore, in the top two cases, the rate of change in
direction was much slower than the experimental data. The results shown
in Fig. 11 are representative of the results obtained for the other
subjects as well. In all cases, the time course of the change in
direction was well matched when the directional change was large (as in
Fig. 11, bottom), but the model's response was in advance
of the experimental data when the directional change in target motion
was more modest.
EXTENSIONS TO THE CARTESIAN MODEL.
The errors in matching finger speed suggest that a nonlinear model
might give an improved fit, i.e., that finger acceleration would depend
on the square and/or the cube of the error terms (ep and ev) in
Eq. 3. We can rule out a quadratic nonlinearity since it
would violate the mirror symmetry that was obtained for targets moving
to the right or to the left (Fig. 2). We did try a model including a
cubic nonlinearity (which does not violate mirror symmetry) for the
data for one subject. This nonlinear model gave a negligible
improvement in the fit (<1% reduction in error).
Another modification to the model in Eq. 3 would be to
replace the scalar coefficients a1 and
a2 with matrices
|
(5)
|
and similarly for a2. Such a
model was proposed by Viviani and Monoud (1990)
, and it
would be compatible with the x-y interaction presented in Fig. 9. However, we found in experiment 2 that
the behavior was invariant under a rotation, i.e., that the response did not depend on the initial direction of the target motion (Fig. 5).
Together with the mirror symmetry in the response (Fig. 2), these
observations require that
Therefore there does not appear to be a simple way to improve the
Cartesian model represented by Eq. 3.
MODELING TRACKING BEHAVIOR IN CURVILINEAR COORDINATES.
As an alternative to the Cartesian model, we investigated models in
which the error signals are described in a curvilinear coordinate
system fixed to the hand (Flanders et al. 1992
).
Specifically, we defined feedback error signals in directions
tangential and perpendicular to the finger's trajectory at each point
in time. In such a description, acceleration is defined by the rate of change of speed and direction
|
(6)
|
where
is the speed,
is the direction of motion, and
and
are unit vectors in the
tangential and normal directions, respectively (see Fig.
12A). (The normal component of the acceleration can also be written as
2/R, where R is the
radius of curvature.) We chose this frame of reference because it makes
speed and direction explicit parameters in the model and because the
experimental data suggested these two parameters were important
controlled variables.

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Fig. 12.
Schematic defining the error signals in model 2.
A: the path of the finger, where and
denote the tangential and normal directions and denotes the direction of finger movement. B: how the
directional target signal is defined.
pT and
pF denote the position of the target
and of the finger, and T indicates
the target velocity. The angle is defined by a vector from the
finger to target positions (pT pF) plus the target velocity vector.
|
|
We began with a model in which the tangential and normal accelerations
were proportional to the components of the positional (ep) and velocity
(ev) error terms (Eq. 3) along these two directions
|
(7)
|
If a1 is equal to
a3 and
a2 is equal to
a4, this model will give the same
results as the Cartesian model in Eq. 3. (As a test of the
simulations, we verified that this was the case.) We next let the four
coefficients
a1-a4
vary independently and found that this gave only a modest improvement
in the fit. Furthermore, a1 and
a3 differed by <15%, as did
a2 and
a4.
We then proceeded to test different error signals, beginning with the
equation for the normal acceleration. We chose the difference between
the present direction
(t) and a desired direction
(t) to be the directional error signal. We defined this
desired direction based on the observation that the initial direction
of motion appeared to be such as to intercept the target at a constant
time. This could come about if the desired direction were defined by the vector sum of a positional error signal and the target velocity signal
|
(8)
|
where the
denotes the angle that the vector in
brackets makes with a reference direction (see Fig. 12B).
The coefficient b5 is a constant, as
are the time delays
dv and
dp.
Then, the simplest model for the finger acceleration in the normal
direction is
|
(9)
|
According to Eq. 9, the rate of change in direction of
finger motion (
) will be zero when
is equal to
, i.e.,
the finger will move in a straight trajectory in the direction given by
. Thus qualitatively, it appears that Eq. 9 could account
for the experimental data.
For the acceleration in the tangential direction, we used an error term
that was similar to the one we used in the Cartesian model (see
Eq. 7). This choice was motivated by the observation that
model 1 gave a reasonable fit to the speed of the finger, with a suggestion of a nonlinearity. We defined the error signal for
speed to be
|
(10)
|
where es represents the
components of the positional and velocity errors terms, defined as
before, in the tangential direction. The tangential acceleration of the
finger is then given by
|
(11)
|
As was the case for the first model, Eqs. 9 and 11 were integrated, using an iterative search over the five
coefficients
b1-b5, and the three time delays
v,
dv, and
dp to obtain
the best fit to the data.
The results of this procedure, for one subject for experiment
1, are shown in the right column of Fig. 11. Note that this second model gave a much improved fit, matching the time course of the direction of finger motion and the variations in finger speed much
better than did the first model. For this subject, the second model
gave a 47% decrease in the error of the fit. This was typical for all
subjects, as can be appreciated in Table
4. Furthermore the model was also able to
fit the results of experiments 4 and 6, in which
target speed underwent a step change or accelerated at a constant rate,
as can be seen in Figs. 13 and
14. For all three experiments,
model 2 consistently gave an improved fit, with an average
decrease of 46% in the error over model 1.

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Fig. 13.
Performance of model 2 in matching tracking behavior in
trials in which target speed underwent a step change. The data are the
same as in Fig. 8 and are from subject 7.
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Fig. 14.
Performance of model 2 in matching tracking behavior in
trials in which target speed accelerated or decelerated. The data are
the same as in Fig. 10 and are from subject 10.
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It might be argued that such an improvement in fit should not be
unexpected since the second model has eight parameters, whereas the
first model only has four. However, even a simple version of the model,
in which the quadratic nonlinearity was omitted and
dv was set equal to
v, gave a significant improvement in fit (by
21% for subject 1 in experiment 1) in the
instance in which this model was tested. To the contrary, adding more
free parameters to the first model (by including nonlinear terms) did not improve the fit. As we have noted, extending the first model to a
matrix formulation is precluded by our experimental results.
As can be appreciated in Table 4, the parameter values that gave the
best fit to the data were highly consistent from subject to subject and
for all three experiments. This is especially true for the three time
delays. The time delay for the error signal for speed
(
v) was consistently the lowest, with an
average value of 115 ms, whereas the time delay for the velocity
component of the directional error signal (
dv)
was consistently the largest, with an average value of 258 ms.
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DISCUSSION |
When targets made an abrupt change