The effects of surface diameter and incline on the hindlimb kinematics of an arboreal lizard (Anolis sagrei)
Department of Biological Sciences, University of Cincinnati, PO Box 210006, Cincinnati, OH 45221-0006, USA
* Author for correspondence at present address: Department of Zoology, Miami University, 212 Pearson Hall, Oxford, OH 45056 (e-mail: spezzalc{at}muohio.edu)
Accepted 22 March 2004
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Summary |
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Key words: arboreal, locomotion, kinematics, lizard, Anolis sagrei, incline, perch diameter, limb posture
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Introduction |
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Although the limb function of primates is well studied (reviewed in
Jenkins, 1974;
Strasser et al., 1998
), limb
function and movement is poorly understood for most other lineages of
vertebrates with well-documented arboreal specializations. For example, the
adaptive radiation of nearly 400 species within the lizard genus
Anolis forms a diverse clade of arboreal vertebrates that has been a
model system for correlating morphology to habitat partitioning and locomotor
speed. Anoles have morphologically and behaviorally distinct forms, or
ecomorphs, which have evolved convergently
(Williams, 1983
). The
morphology of anoles is correlated to both habitat selection and locomotor
performance. For example, species of Anolis with short limbs, such as
the twig ecomorphs, generally use narrow perches and have slow maximal running
speeds (Moermond, 1979
;
Williams, 1983
;
Losos, 1990
). Consequently,
limb length, combined with locomotor behavior, may directly influence the
ability to traverse a given habitat
(Losos, 1990
;
Higham et al., 2001
). However,
little is known of how the limbs move and are used by any species of
Anolis, much less how diameter or incline affect limb function.
Hence, we quantified the limb movements during arboreal locomotion with
varying perch conditions using Anolis sagrei, which naturally occurs
on perches with a wide range in diameter and inclines
(Mattingly and Jayne,
2004
).
Phylogenetically diverse animals moving on inclines often stay nearer to
the surface by reducing hip height and vertical oscillation of the hip
(Vilensky et al., 1994;
Carlson-Kuhta et al., 1998
;
Jayne and Irschick, 1999
). By
having a more crouched limb posture with greater flexion at the hip (= femur
elevation in sprawling limb vertebrates), knee and ankle joints can contribute
to decreasing hip height of animals with either upright or sprawling limbs.
Furthermore, a terrestrial species of lizard has greater long-axis femur
rotation associated with decreased hip height on inclined surfaces
(Jayne and Irschick, 1999
).
Thus, for locomotion of Anolis lizards on inclined surfaces, we
expected decreased hip height as a result of increased femur rotation and
increased flexion of the joints within the limb. Decreased hip height should
reflect a decreased distance between the center of mass and the locomotor
surface, which would decrease the tendency to topple backwards when climbing a
steep surface.
Variation in perch diameter may also affect limb posture in several ways.
On perches with large diameters, a lizard could have either an overall
sprawling limb posture, with the knees lateral to the hip
(Fig. 1A), or a more upright
posture with both the knees and ankles located more medially
(Fig. 1B). On narrow perches,
if the limbs were sprawled and the ankles were directly below the knees, the
foot would be too lateral to touch a perch with a diameter less than the
inter-knee distance (Fig.
1A,D). When the feet must be placed more medially to fit onto a
narrow perch, hip height might decrease to lower the center of mass and reduce
the torques that tend to topple the animal sideways
(Cartmill, 1985). Thus, we
expected anoles moving on narrow perches to use some combination of femur
depression and knee flexion to facilitate placing the feet more medially, as
well as reducing hip height with the same mechanisms expected for locomotion
on inclined surfaces.
Many aspects of the geometry of placing the limbs on a round perch do not have simple linear increases with increased perch diameter. For example, for a constant lateral distance between the two feet within a girdle, the slope of clearance between the ventral surface of the body and the top of the perch versus perch diameter decreases with increased perch diameter (Fig. 1D). Similarly, for a given distance between contralateral feet, the steepness of the perch surface making contact with the feet declines with increased perch diameter as the values for large diameter perches asymptotically approach those of a horizontal flat surface. Thus, for those kinematic variables changing significantly with perch diameter, a non-linear pattern of change similar to that in Fig. 1D would seem likely. Non-linear changes in kinematics with increased perch diameter may also be likely because variation in perch diameters less than the inter-knee distance may pose a greater need to modify kinematics than variation in perch diameters that exceed the inter-knee distance of lizards with an overall sprawling limb posture.
We focused on the hind limb function of anoles for the following reasons.
First, previous studies of anoles correlating morphology, locomotor speed and
perch diameter have dealt primarily with the dimensions of the hind limb
(Losos and Sinervo, 1989;
Losos and Irschick, 1996
).
Second, more comparative data are available for the hind limbs of lizards
because kinematic studies of terrestrial species have concentrated on the hind
limb since it is used during all speeds of locomotion
(Irschick and Jayne, 1999
;
Jayne and Irschick, 1999
;
Reilly and Delancey, 1997
).
Finally, the shoulders of lizards have some translational movements that
complicate kinematic analyses (Goslow and
Jenkins, 1983
; Peterson,
1984
).
This study had the following four main objectives. First, we manipulated
perch diameter and incline to determine their effects on hind limb posture and
kinematics during steady-speed locomotion. Second, we used a large range of
perch diameters to determine whether kinematics changed more for a change in
diameter among narrower perches than for a change in diameter among wider
perches. Third, we tested whether the effects of perch diameter depended on
incline (had interactive effects). Finally, we compared the effects of surface
and incline on hind limb kinematics between A. sagrei and other
tetrapod vertebrates including the specialized arboreal lizard Chamaeleo
calyptratus (Higham and Jayne,
2004) and the more generalized terrestrial lizard, Dipsosaurus
dorsalis (Jayne and Irschick,
1999
).
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Materials and methods |
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All lizards used in the study were obtained from a commercial supplier in Florida and shipped to the University of Cincinnati for experiments. Lizards were caged individually and maintained on a diet of crickets with a vitamin supplement and given water ad libitum. Incandescent bulbs provided light and heat for 14 h per day and adequate conditions for the lizards to thermoregulate to their active field temperature range (2931°C).
To obtain dorso-ventral view radiographs, we anesthetized the lizards with Halothane following a protocol approved by the Institutional Animal Care and Use Committee of the University of Cincinnati. We measured skeletal dimensions from radiographs for all four A. sagrei and the measurements and mean values (± S.E.M.) were as follows: tail length (97±0.9 mm), longitudinal distance between the shoulder and hip joints (32.3±0.2 mm), width between the two hip joints (6.4±0.1 mm), and the lengths of the femur (13.3±0.3 mm), tibia (11.6±0.5 mm), hind foot (8.1±0.2 mm) and fourth toe (12.2±0.2 mm) of the right hind limb. Hence, the average distances from the hip to the tip of the fourth toe and between outstretched knees were 45.0±1.2 and 33.0±0.7 mm, respectively.
Experimental protocol
We obtained simultaneous dorsal and lateral views of steady speed
locomotion using a two-camera NAC (Tokyo, Japan) HSV-500 high-speed video
system operating at 250 images s1. Lizards were placed in a
thermally insulated container at a temperature similar to the active field
body temperature of this species (2931°C) for at least 30 min prior
to eliciting locomotion. We determined body temperature immediately before
trials using a thermocouple and a Tegam model 871A digital thermometer
(Geneva, Ohio, USA). We covered all perch and treadmill surfaces with 1.5 mm
mesh fiberglass screen to enhance the traction of the lizards, as in Irschick
and Losos (1998) and Higham et
al. (2001
). All of the round
perches were 122 cm long with diameters of 1 cm (wooden dowel), 3, 6 or 10 cm
(polyvinylchloride pipe). For each round perch, we obtained locomotion on a
level, 45° and 90° uphill incline. The flat surface trials, which used
a rubberized belt of a stationary treadmill, as in Fieler and Jayne
(1998
) and Higham and Jayne
(2004
), were either level or
uphill at 45°. We could not obtain data for the flat, vertical surface
because the lizards would not move reliably under this condition. Thus, a
total of 14 combinations of surface and incline were used for each of the four
individuals in our experimental design.
To facilitate frame-by-frame motion analysis, we painted landmarks on a
prominent protuberance of the pelvis and several joints of the right hind limb
(Fig. 2). The pelvic landmark
coordinates were transformed to approximate the coordinates of the hip as in
Fieler and Jayne (1998) and
Jayne and Irschick (1999
). All
lizards ran no more than four times in rapid succession within each testing
session, and were allowed to recover for more than 2 h between sessions. Over
the course of several weeks, we randomized the order of perch conditions and
we always provided at least one day of rest between successive days of
testing.
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Each stride analyzed was from a different trial. As a result of using a stationary surface and because A. sagrei often moves in short bursts rather than steadily, we had to conduct a large number of trials to obtain adequate samples of reasonably steady locomotion with similar speeds. The strides selected for analysis were in the middle of a bout of locomotion with three or more strides that subjectively appeared to be of similar speed. Hence, we selected strides with little if any acceleration.
Rather than selecting a random sample of all strides videotaped on the different perches, we selected a subset of data to avoid speed confounding the potential effects of diameter and incline. Although our experimental protocol was not designed to elicit maximal locomotor speed, we did observe some regular patterns of variation in the speeds of locomotion. Speeds greater than 60 cm s1 were rare on the on the 1 cm perch regardless of incline. Speeds greater than 100 cm s1 were fairly common for horizontal and 45° perches with diameter >3 cm, and some individuals obtained speeds between 120 and 130 cm s1 under these conditions. For a given perch diameter, speeds were usually slowest on the vertical surface compared to the other inclines.
For our frame-by-frame motion analysis, we selected 24 strides of
similar-speed, steady locomotion for each individual on each combination of
surface and incline. An analysis of variance (ANOVA) of speed for the strides
on round perches confirmed the lack of significant main effects of diameter
(F3,9=1.12, P=0.39) and incline
(F2,6=2.87, P=0.13) effects on speed, and none of
the two-way interaction terms involving individual, diameter and incline was
significant. The ANOVA of strides including the flat surface but excluding
data from vertical inclines also confirmed a lack of diameter
(F4,12=1.91, P=0.30) and incline
(F1,3=0.66, P=0.48) effects on speed. This lack
of significant variation in speed with variation in locomotor surface is
important since speed often has significant effects on kinematics
(Jayne and Irschick, 1999).
The grand means (N=185) for speed and duty factor (±
S.E.M.) were 54±0.5 cm
s1 and 54±0.6%, respectively.
Kinematics
We used custom-designed video-analysis software (Stereo Measurement TV,
written by Garr Updegraff, San Clemente, CA, USA;
garr{at}uci.edu)
to digitize all of the two- and three-dimensional coordinates. We calculated
all of the kinematic quantities from these coordinates using macros for
Microsoft Excel version 7.0 (written by G. Updegraff and B. Jayne). We sampled
images every 4 ms, which provided 20 or more images per stride. Two
two-dimensional coordinates digitized from a dorsal perspective were the right
and left pelvic landmarks. Three-dimensional coordinates digitized from both a
dorsal and lateral view included the right pelvic landmark, knee, ankle,
distal end of the fourth metatarsal and both the middle (joint) and tip of the
fourth toe. For our fixed frame of reference, the x-axis was parallel
to the overall direction of travel, which was parallel to the long axis of the
locomotor surface. The y-axis was within a vertical plane containing
the x-axis. The z-axis was perpendicular to the
xy plane.
The following seven variables described attributes of the entire locomotor cycle or orientation of the pelvis. Stride length was the difference between x-axis positions of successive right hind footfalls, and step length was the x-distance traveled by the body during stance of one limb. Stride duration was the elapsed time between successive right hind limb footfalls, and stride frequency was the inverse of stride duration (Hz). Duty factor was the percentage of the total stride cycle when the right hind foot contacted the perch, and mean forward velocity was stride length (cm) divided by stride duration (s). A two-dimensional (x, z) angle indicated the angle between the line passing through both hips and the x-axis, and the difference of the maximum and minimum values of these angles was pelvic rotation.
Five linear variables described positions and displacements relative to the
locomotor surface or the hip. Hip height relative to the top of the path
surface (location of the greatest value of Y in a yz
section through the perch) was described with three linear variables,
standardized so that the top of the path surface was y=0: hip height
at the moment of footfall (Yhipfootfall), hip height at
footfall minus minimum hip height or the change in hip height during stance
(Yhipstance), and the maximum hip height minus the
minimum hip height (total vertical oscillation of the hip) for the entire
stride cycle (
Yhiptotal). Effective limb lengths
were also measured as the straight-line distance between the hip and the ankle
in both two (x, y) and three dimensions.
Thirty-six linear variables used relative coordinates so that the hip was
located at (0, 0, 0) and positive x, y and z values
indicated anterior, dorsal and lateral, respectively. For the relative
coordinates of each dimension, we determined minimum
(Xmin, Ymin, Zmin)
and maximum (Xmax, Ymax,
Zmax) positions and the difference (excursion) between the
two (X,
Y,
Z) for the knee,
ankle, distal end of the fourth metatarsal and the tip of the fourth toe
during each entire stride cycle.
Six variables described three-dimensional angles of knee, ankle and the joint between the metatarsal and fourth toe within the right hind limb at footfall and the end of stance. Smaller values of the knee angle (between 0° and 180°) indicated greater flexion of the joint. The ankle angle was measured between the tibia and the metatarsal on the dorsal surface of the foot so that decreasing values (between 0° and 180°) indicated greater dorsiflexion of the foot. Toe angle, measured at both footfall and end of stance, was the angle between the fourth metatarsal and a straight line extending from the base to the tip of the fourth toe, such that values greater than 180° indicated plantar flexion.
For each of three angles describing the orientation of the right femur, we determined the maximum, minimum and excursion (maximumminimum), during an entire stride cycle. Femur retraction was the two-dimensional (x, z) angle, between the femur and a line connecting the hips such that a value of 0° indicated the femur was perpendicular to the long axis of the pelvis, and greater magnitude positive and negative values indicated greater retraction and protraction, respectively. Long-axis femur rotation was determined from a three-dimensional angle between the plane containing the femur and the tibia and a vertical reference plane passing through the femur. Greater clockwise long-axis rotation of the right femur, as seen in right lateral view, is indicated by greater positive values, and a value of zero indicates that the plane containing the femur and tibia is within the vertical reference plane passing through the femur. Lastly, femur depression was a three-dimensional angle between the femur and a horizontal plane passing through the right hip where greater positive and negative values equalled greater amounts of depression (knee below the hip) and elevation (knee above the hip), respectively.
Statistical analyses
We used SAS version 8.0 for all of the statistical analyses, and a 3-way
mixed model ANOVA, for which incline and diameter were fixed factors and
individual was a random factor. Thus, according Scheffe
(1959) the denominators for
the F-tests of the main effects were the mean squares of the two-way
interaction terms involving the fixed effect and individual, and the
denominator for the F-test of the diameter x incline
interaction term was the incline x diameter x individual
interaction mean square. Although we used P<0.05 as the primary
criterion for statistical significance, we provide tables with degrees of
freedom (d.f.) and F-values to clarify potential effects of making
multiple comparisons. Unless stated otherwise, all mean values are presented
± S.E.M., where N equals the
total number of strides observed for each combination of surface and
incline.
We performed principle component analyses, primarily to clarify the
relative importance of kinematic variables when considered simultaneously for
explaining the total variance associated with different locomotor surfaces
rather than for testing for the effects of different inclines and perches.
Thus, we were most interested in the factor loadings for providing insights
that were not evident in the univariate analyses. We used 15 kinematic
variables used previously to analyze terrestrial lizard locomotion in
Dipsosaurus dorsalis (Jayne and
Irschick, 1999). For our multivariate analysis of A.
sagrei, each stride (N=185) was a data point.
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Results |
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During most of stance, the knee extended, and the femur retracted and rotated in a clockwise direction, and all of these angles usually attained maximum values near the end of stance (Figs 2, 5). At midstance the tibia was often nearly horizontal (Fig. 3) as values of long-axis femur rotation often approximated 90° (Fig. 5). During the first half of stance femur depression often increased slightly to a maximum value and then femur depression usually decreased gradually during the later half of stance (Figs 3, 4). Despite considerable variation in femur depression associated with variation in the locomotor surfaces, values of femur depression during stance were rarely less that zero (Fig. 5), indicating that the knee usually remained ventral to the hip throughout stance (Figs 3, 4). The ankle usually flexed during the first half of stance and extended during the latter half of stance (Fig. 5). All portions of the limb were usually most posterior relative to the hip at the end of stance (Fig. 4).
Femur protraction usually started and continued for the first two-thirds of the swing phase of the stride (Fig. 5). Consequently, the arc traveled by the knee relative to the hip during swing had its most lateral position near mid swing (Figs 2D,H, 4). In contrast to the early lateral movements of the knee relative to the hip, the more distal portions of the limb often moved medially relative to the hip during early stance (Fig. 4). Counter-clockwise long-axis rotation of the femur usually started and continued throughout the swing phase, and the femur was usually elevated slightly during the first half of swing and depressed slightly during the latter half of swing (Fig. 5). The knee and ankle usually began to flex near the beginning of swing and continued to flex until mid-swing (Fig. 5). During the latter one-half to one-third of swing, the angles of the knee, ankle and femur retraction often changed little or increased slightly (Fig. 5).
Effects of diameter and incline
Variation in the locomotor surfaces had profound effects on the hindlimb
kinematics of A. sagrei (Tables
1,
2,
3,
4). For example, of 45 linear
and timing variables, 38 variables for the round perch data (Tables
1,
2) and 36 variables for the
data including the flat surface (Tables
1,
3) had significant effects of
either diameter, incline or the diameter x incline interaction term. Of
14 angular variables (Table 4)
for the round and flat surface data, 8 and 12 variables had either a
significant main or interaction effect of diameter and incline,
respectively.
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Diameter had more widespread effects on kinematics than incline. For example, the main effect of diameter was significant for 26 variables, whereas the main effect of incline was significant for only 17 of the 45 linear and timing variables for the round perch data (Tables 1, 2). For the ANOVA results summarized in Tables 2 and 3, only seven diameter x incline interactions were significant, and five of these seven interaction terms were only marginally significant (0.01<P<0.05).
Stride length and step length increased significantly with increased diameter, whereas stride frequency decreased significantly with increased diameter (Table 1, Fig. 6A,B). Of the four whole-stride characteristics, incline only had significant main effects on stride length (Table 1). For a particular perch diameter, mean values of stride length were consistently the smallest on vertical inclines (Fig. 6A), and the smallest mean value of stride length was for the 1 cm perch inclined at 90°.
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Hip height at footfall and effective limb length indicate the extent to which the limb is directly beneath the hip and straight. Diameter and incline had significant interactive effects on hip height at footfall (Table 1) such that values were nearly constant on the 90° incline, but usually increased with increased perch diameter on the other inclines (Fig. 6C). Values of hip height at footfall on the flat surface were nearly twice as large as those for the 1 cm perch (Fig. 6C). The three-dimensional effective limb length had highly significant increases with increased diameter (Table 1), but it increased less with increased diameters beyond an intermediate diameter (Fig. 6D). The three-dimensional effective limb length also differed significantly among inclines, and the 45° incline consistently had the lowest values for each diameter (Fig. 6D).
As diameter increased the most anterior positions of the ankle, metatarsal
and toe tip relative to the hip (Xmax) increased
significantly, whereas the most posterior positions (Xmin)
of these distal limb locations had less regular or significant change with
increased diameter (Tables 2,
3;
Fig. 7A). Consequently, the
longitudinal excursions (X) of the ankle, metatarsal and toe
tip increased significantly with increased diameter, and the distal limb was
positioned progressively more anterior to the hip as diameter increased.
Average values of the ankle at footfall were posterior to the hip for the 1 cm
diameter perches on all inclines and some of the 3 cm diameter perches,
whereas for broader surfaces the ankle was well anterior to the hip at the
beginning of stance (Fig. 3). Incline significantly affected Xmin of both the metatarsal
and the toe tip such that the greatest magnitude of the values was uniformly
observed for the 45° incline for each perch diameter
(Fig. 7A). For all combinations
of diameter and incline, the magnitude of Xmin exceeded
that of Xmax for the ankle and more distal locations of
the limb (Fig. 7A). Thus, the
extreme longitudinal positions of the limb relative to the hip are not
symmetric, and positions posterior to the hip dominate the stride cycle
(Fig. 4).
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For most portions of the limb, the most ventral position relative to the hip (Ymin) changed significantly, whereas the most dorsal position (Ymax) changed little with the diameter of round perches (Table 2). For the knee, Ymin had decreased magnitude with increased diameter, whereas Ymin of the toe tip often had the greatest magnitude on the narrowest perch as a result of the foot and the toe pointing downward and wrapping around the narrow perches (Fig. 2). The height of the ankle at footfall often approximated that of the knee on the 1 cmdiameter perches, but with increasing surface diameter the height of the knee relative to the ankle at footfall generally increased (Fig. 3).
Both the most medial (Zmin) and the most lateral
(Zmax) positions of the ankle, metatarsal and toe tip
increased significantly with increased diameter (Tables
2,
3), and the most conspicuous
increases were from the smallest to intermediate diameter
(Fig. 7C). On the 1 cm diameter
perches, the ankle was consistently located medial to the knee at footfall,
but for larger perch diameters the ankle was commonly slightly lateral to the
knee at footfall (Fig. 3). In
contrast to Zmin and Zmax, the lateral
excursion (Z) was unaffected by diameter (Tables
2,
3). Thus, although the amounts
of lateral limb movement were similar for different diameters, the overall
location of the limb throughout the entire stride cycle shifted laterally as
diameter increased (Figs 4A,B,
8).
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Knee angle at footfall increased significantly with diameter and the largest increases were from the smallest to intermediate diameter (Table 4; Fig. 9A). For each perch diameter, the values of both knee and ankle angle at footfall were uniformly the smallest for the 45° incline (Fig. 9A,B). Pelvic rotation was not affected significantly by either diameter or incline alone (Table 4). However, the mean values of pelvic rotation on the level surfaces were usually the lowest for each perch diameter (Fig. 9C).
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Maximum (most posterior) femur retraction decreased significantly with increased diameter, and the most conspicuous decrease was from the 1 cm to the 3 cm diameter (Table 4; Fig. 10A). However, minimum femur retraction was nearly equal for all surfaces (Fig. 10A). Consequently, the mean values of protractionretraction excursion decreased significantly with increased perch diameter in a manner similar to that of maximum femur retraction (Table 4; Fig. 11A). Both minimum and maximum femur depression had highly significant decreases with increased diameter (Table 4; Fig. 10B), but the excursion of femur depression was nearly constant for increases in perch diameter greater than 3 cm (Fig. 11B). For each perch diameter, the maximum (most clockwise) long-axis rotation of the femur was less for the level surface compared to the other two inclines, and this variable generally decreased with increased surface diameter (Fig. 10C). The amount of femur rotation decreased considerably from the 1 cm to the 3 cm diameter surface, but changed little with further increases in diameter (Fig. 11C).
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Non-linear changes in kinematics with increased diameter were very common. The most common pattern of non-linear change was that the magnitude of change in the kinematic variable decreased with increased diameter for a similar incremental increase in perch diameter (Figs 6D, 7C, 9A, 11C). For example, 22 of the 32 kinematic variables with a significant main effect of diameter (round perch data in Tables 1, 2, 4) had a greater difference between the mean values (pooled across all inclines) of 3 cm and 1 cm than those of the 10 cm and 6 cm diameter.
In the principle components (PC) analysis (performed without rotation of the axes), values of the first PC generally increased with increased surface diameter (Fig. 12). In multivariate space, locomotion on different inclines was not kinematically very distinct (Fig. 12). A more extended knee at footfall, smaller values of maximum femur retraction and smaller values of femur depression all contributed to the high scores of PC1 (Table 5). The first three principle components accounted for 28%, 21% and 9.6% of the total variance in kinematics, respectively.
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Discussion |
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The nearly horizontal femur (femur depression=0°) of A. sagrei at footfall on the flat level surface conforms to one key attribute of sprawling limb posture. For femur rotation, femur retraction and knee angle, the minimum values approximate the values at footfall and the mean values of these variables were 36°, 60° and 82°, respectively (Figs 9A, 10A,C). Near midstance, femur retraction of A. sagrei approximated zero as is the case for nearly all vertebrates with sprawled limbs, and values of femur depression, femur rotation and knee angle approximated 16°, 62° and 90°, respectively. Thus, on the flat level surface, at both footfall and midstance, femur depression and knee angles conformed closely to typical sprawling posture. However, the rotated femur results in the foot being considerably posterior to the knee rather than below it (Fig. 3).
Of the previously studied species of lizards, the limb posture of A.
sagrei most closely resembles that of Sceloperus clarkii, which
commonly traverses steep rock faces. For locomotion of S. clarkii on
a flat surface and with duty factors similar to those of A. sagrei, S.
clarkii has a nearly horizontal femur and the foot is markedly posterior
to the knee (Reilly and Delancy, 1997) as a result of long-axis femur
rotation. Thus, the hind limbs of both A. sagrei and S.
clarkii have an overall dorsal-ventrally flattened appearance as a result
of this limb posture. In contrast, for a more generalized terrestrial lizard,
Dipsosaurus dorsalis, on a flat level surface with slightly higher
duty factors (63%) and similar speeds (50 cm s1), compared
to A. sagrei and S. clarkii at footfall the ankle is more
nearly beneath the knee and the tibia is more nearly perpendicular to the
ground as a result of less femur rotation
(Jayne and Irschick, 1999).
Similar to A. sagrei on the flat surface, the knee angle at midstance
of S. clarkii (Reilly and Delancy, 1997), D. dorsalis
(Jayne and Irschick, 1999
),
several terrestrial lizard species
(Irschick and Jayne, 1999
) and
an arboreal specialist, Chamaeleo calyptratus
(Higham and Jayne, 2004
) all
approximate 90°. However, unlike A. sagrei and terrestrial
species of lizards at low speeds, the knee of C. calyptratus is much
more extended at footfall (125°). Hence, A. sagrei, S. clarkii
and C. calyptratus all have morphological and behavioral
specializations for climbing, but only the former two species have similar
limb posture.
As expected, with decreased perch diameter the femur of A. sagrei became more depressed throughout stance (Fig. 10B), and femur depression is one mechanism for locating the foot more medially. Although increased femur protraction is another potential mechanism for locating the foot more medially, this angle at footfall did not change significantly with decreased perch diameter (Fig. 10A). Increasing the amount of knee flexion is perhaps the most important mechanism used by A. sagrei for locating the foot more medially when moving on narrow perches, and the most conspicuous difference in knee flexion of A. sagrei was between the 3 cm and 1 cm diameter perches.
If A. sagrei had a typical sprawling posture (Fig. 1A), then the ankles could not contact the 1 cm diameter perch because it is considerably narrower than the distance between outstretched knees of the lizard (33 mm). The midline of the pelvis of A. sagrei is approximately centered over the perch at footfall, which facilitates the following calculations for the level 1 cm diameter perch. If the knee angle were 90° and femur depression and femur rotation were 0°, then for the observed mean values of pelvic rotation (25°) and femur protraction (55°) the ankle would be more than 4 mm lateral to the perch. Accounting for the observed value of femur depression (34°) only decreases this distance by approximately 1 mm. For the observed value of knee angle (40°) while holding other angles constant, the lateral distance from the middle of the pelvis to the ankle is only 2.6 mm and hence fits well within a 1 cm diameter perch.
For perches with diameters larger than 1 cm, all of the above mechanisms
are used to varying degrees to locate the feet more medially. After meeting
the requirements to make contact with the perch, further medial locations of
the foot on a round perch will change the orientation of the locomotor surface
that contacts the foot. On a perch of a given diameter, a foot located more
medially will be on a surface that is more nearly horizontal, similar to the
manner in which the feet on larger diameter perches are located on more nearly
horizontal surfaces (Fig. 8).
Unlike A. sagrei, the values of knee angle and femur depression for
C. calyptratus did not change significantly for locomotion on a
narrow round perch compared to a flat surface
(Higham and Jayne, 2004).
Although many kinematic variables of A. sagrei changed
significantly with increased incline, fewer variables changed than with perch
diameter. With increased incline, hip height decreases in many diverse groups
of vertebrates to minimize the risk of falling backwards
(Cartmill, 1985;
Vilensky et al., 1994
;
Carlson-Kuhta et al., 1998
;
Jayne and Irschick, 1999
). For
A. sagrei, incline and perch diameter had significant interactive
effects such that hip height was lowest on the steepest incline for most perch
diameters and hip height did not change conspicuously with perch diameters for
the steepest incline (Fig. 6C).
Reducing the height of the hip and the center of mass reduces some of the
adverse effects of torques that tend to make the animal fall off of the
locomotor surface (Cartmill,
1985
). For a vertical uphill perch, falling by tipping from side
to side is not a problem, but the tendency to fall backwards is greatest and
constant regardless of perch diameter. The tendency to tip from side to side
increases with decreased perch diameter, but for both the level and 45°
inclines the tendency to fall backwards is absent or constant. Thus, the
interactive effects of incline and diameter on hip height correspond well with
the different functional problems associated with the three inclines in our
study of A. sagrei.
A more crouched limb posture will decrease hip height, and diverse groups
of vertebrates commonly use increased amounts of flexion at the knee and ankle
as mechanisms for increasing the extent to which the limb is crouched on
uphill surfaces compared to level surfaces
(Vilensky et al., 1994;
Carlson-Kuhta et al., 1998
;
Jayne and Irschick, 1999
).
Unexpectedly, the angles of the knee and ankle at footfall of A.
sagrei on 45° uphill were lower than those of both the level and
90° uphill (Fig. 9). Additional mechanisms of decreasing hip height include orienting the femur
more nearly parallel to the locomotor surface and increasing long-axis femur
rotation in animals with sprawling limbs. Femur depression of A.
sagrei did not change significantly with incline. In contrast, the values
of femur rotation of A. sagrei were significantly less on the level
surface compared to the uphill inclines
(Fig. 10), which is similar to
the manner in which a generalized terrestrial lizard decreases hip height with
increased femur rotation on downhill inclines
(Jayne and Irschick,
1999
).
Responses to incline and diameter of specialized and generalized lizards
The three lizard taxa for which the most detailed comparisons are possible
regarding the effects of incline are Anolis, Chamaleo calyptratus and
Dipsosaurus dorsalis. Both Anolis lizards
(Losos, 1990;
Irschick and Losos, 1996
) and
chameleons (Peterson, 1984
;
Russell and Bels, 2001
) have
several divergent morphological and behavioral specializations for moving in
arboreal habitats. For example, chameleons have prehensile feet and tails,
move very slowly and have unusually high proportions of slow muscle fibers in
their limbs (Abu-Ghalyun et al.,
1988
). Anolis lizards have toe pads that adhere to
surfaces (Williams and Peterson,
1982
; Irschick et al.,
1996
). The low endurance and rapid running speeds of many
Anolis species suggest they have a preponderance of fast glycolytic
fibers, as seen in most other lizards
(Bonine et al., 2001
). Anoles
commonly jump to bridge gaps between perches. Chameleons do not jump, but do
have several features of forelimb and hindlimb movement that appear to
facilitate reaching forward (Peterson,
1984
; Higham and Jayne,
2004
). In contrast to A. sagrei and C.
calyptratus, the desert iguana D. dorsalis lacks feet with
specializations for either adhesion or prehension, and most of its locomotion
is on the ground rather than on perches. Consequently, D. dorsalis is
a good model for a morphologically and behaviorally generalized lizard
(Fieler and Jayne, 1998
).
In A. sagrei, the percentage of kinematic variables that had
significant main effects of incline (incline factor significant regardless of
interaction term significance) was 40%. This value is intermediate between the
low percentage (11%) of variables affected in C. calyptratus
(Higham and Jayne, 2004) and
the high percentage (73%) of kinematic differences reported by Jayne and
Irschick (1999
) for D.
dorsalis. Unlike our study of A. sagrei, the data for D.
dorsalis and C. calyptratus included both uphill and downhill
inclines. The downhill locomotion of D. dorsalis is kinematically
most distinct and hence, was likely responsible for many of the significant
main effects of incline (Jayne and
Irschick, 1999
). The only other study to quantify diameter effects
on hind limb kinematics of lizards was for C. calyptratus on 2.4 cm
diameter round perches versus flat surfaces
(Higham and Jayne, 2004
).
Diameter had significant main effects for approximately twice the percentage
of variables for A. sagrei (67%) compared to C. calyptratus
(32%) (Higham and Jayne,
2004
). C. calyptratus is striking for its uniformly small
changes in limb kinematics with changes in incline and perch diameter compared
to the former two species of lizards, and the tokay gecko Gekko gecko
is another arboreal specialist that may have only minimal changes in limb
kinematics with variable incline (Zaaf et
al., 2001b
). Perhaps, the greater modulation of limb kinematics in
A. sagrei and D. dorsalis facilitates their ability to move
with a wider range of speeds on different locomotor surfaces than some
climbing specialists.
A very general feature of the hind limb kinematics of lizards and other
vertebrates is that the knee flexes briefly during early stance
(Higham and Jayne, 2004), as
would be expected if the limb was functioning according to the `mass-spring'
model (Blickhan, 1989
).
However, for A. sagrei on narrow perches, early stance flexion of the
knee was absent as the knee extended throughout stance
(Fig. 5). Perhaps, the
extremely posterior location of the foot relative to the knee and the nearly
horizontal orientation of the tibia at footfall
(Fig. 2A) make using the limb
as a spring unlikely.
Implications of variable perch diameter for performance
Previous studies of anoles have described linear increases in maximal speed
(Vmax) with increased perch diameter
(Losos and Sinervo, 1989;
Losos and Irschick, 1996
), but
closer examination suggests this relationship for may be nonlinear for some
species. For A. sagrei, running up a 38° incline in the
laboratory, mean values of Vmax are 0.97, 1.44, 1.73 and
1.77 m s1 for perch diameters (D) of 0.6, 1.6, 2.5
and 5.1 cm, respectively (from fig. 1 in
Losos and Irschick, 1996
). We
calculated least-squares regressions for these values of
Vmax of A. sagrei and found that a simple linear
regression predicting Vmax from D was not
statistically significant (F1,2=4.2, P=0.18).
However, a quadratic polynomial of D (not calculated in the previous
study) predicting Vmax was significant overall
(F2,1=7000, P<0.01,
r2=0.99), and the coefficients of both the linear and
quadratic terms of D were both significant (P<0.01) in
the regression model
Vmax=0.60+0.66D0.085D2.
The negative quadratic effect of diameter on Vmax
corresponds well with the non-linear effects of increased diameter that we
found for several kinematic variables. However, we note that our kinematic
data for A. sagrei were for a constant speed (54 cm
s1) that was substantially less than
Vmax, and the data for narrower perches were greater
fractions of Vmax than the data for wider perches.
The hindlimb kinematics of several species of terrestrial lizards have
several general trends with increased speed
(Jayne and Irschick, 1999;
Irshick and Jayne, 1999) that are nearly opposite the changes in kinematics
that we observed for A. sagrei as perch diameter decreased. For
example, stride length and hip height have the greatest values at maximal
speeds of terrestrial lizards, and in some species stride width increases with
speed on level surfaces (Jayne and
Irschick, 1999
). Pelvic rotation during high-speed locomotion of
terrestrial locomotion usually exceeds 45°. At footfall during high speed
running, the knee of most lizards is extended slightly more than 90°.
Furthermore, the minimum values of femur rotation often approximate 0° for
high-speed quadrapedal running, and negative values of femur rotation often
occur during bipedal locomotion (Irshick and Jayne, 1999). As a combined
consequence of knee extension and femur rotation, the foot is generally
anterior to the knee at footfall and the greatest forward reach of the distal
limb usually occurs at highest speeds during terrestrial locomotion. In
addition, the long-axis of the foot is nearly oriented parallel to the overall
direction of travel at high speeds, whereas at low speeds the long-axis of the
foot is often oriented laterally with an angle greater than 30°. At very
high speeds, the effective limb length of terrestrial lizards is often
enhanced as a result of increased plantar flexion resulting in digitigrade
foot posture throughout the stance phase
(Jayne and Irschick, 1999
).
For terrestrial lizards running rapidly, the large amounts of plantar flexion
during late stance and hyperextension of the toe during early swing imply
these movements have an important role for increasing force
(Irschick and Jayne, 1999
) or
increasing the period of time during which force can be applied to the
substrate.
The following examples illustrate some of the changes in hind limb kinematics of A. sagrei with decreased perch diameter that are contrary to those changes observed with increased speeds in terrestrial lizards. With decreased perch diameter on the level surface, stride length decreased, hip height decreased, effective limb length at footfall decreased, pelvic rotation decreased, femur rotation at footfall was considerable (greater than 30°), knee flexion increased and the foot was located more posterior relative to the knee at footfall. The angle between the long-axis of the metatarsals and the perch also increased dramatically from a mean value of 19° on the flat surface to 79° on the 1 cm diameter perch. As perch diameter decreases, the orientation of the surface from which the foot pushes off becomes less horizontal (Fig. 8). Thus, the combination of the lateral orientation of the foot and the surface that it contacts on narrow perches is likely to reduce the ability to use plantar flexion to produce a large forward directed component of the ground reaction force as appears likely for rapidly running terrestrial species.
Although our observations of A. sagrei are for speeds substantially less than maximal speeds, the kinematics that we observed on narrow perches are so contrary to those observed for the high speed locomotion of other lizards, they strongly suggest some of the functional difficulties for obtaining high speeds on narrow perches. Future studies determining ground reaction forces on perches of different diameter would be very useful for further resolving why locomotor performance decreases with decreased perch diameter. Perhaps the orientation of the foot and limb on narrow perches will result in disproportionate increases in the laterally oriented reaction force and decreases in the reaction forces in the y direction relative to the forward-directed forces.
Clearance in arboreal environments
For the arboreal locomotion of lizards, the effects of habitat structure on
locomotor performance have been discussed widely
(Losos and Sinervo, 1989;
Losos, 1990
;
Irschick and Losos, 1998
).
However, a neglected but important functional consideration for movement in
arboreal habitats is the clearance between the body of the lizard and the
perch upon which it moves and adjacent perches that obstruct the path traveled
by the animal.
The clearance between the ventral surface of the body of a lizard and the locomotor surface depends on both the curvature of the locomotor surface and the lateral distance between the contralateral points of contact with the locomotor surface. Decreasing the height of the hip relative to the point of foot contact with the perch is beneficial for decreasing the tendency of the body to tip away from the locomotor surface. On a flat surface, theoretically, the height of the hip and ankle could be equal if the femur were either rotated or elevated considerably. However, on a round perch the upward bulge of the surface between the points of foot contact precludes the possibility of having the foot and hip at the same height. For example, for typical sprawling limb posture and the anatomical dimensions of A. sagrei (Fig. 1A), the upward bulge of a 3.5 cm diameter perch is as great as the length of the tibia and hence, the ventral surface of the lizard would contact the top of this perch (Fig. 1D). For perch diameters of 4.0, 4.8 and 9.7 cm theclearances between the ventral surface and the top of the perch are 25%, 50% and 75% of the length of the tibia, respectively (Fig. 1D). Thus, for A. sagrei, potentially large differences in the clearance between the body and the top of the perch occur for perches with diameters less than 10 cm. Locating the feet more medially reduces the magnitude of the effects of perch curvature on the clearance between the top of the perch and the ventral surface of the lizard, and we previously discussed several mechanisms that the lizards use to locate the foot more medially.
In natural arboreal habitats, as perch diameter decreases the distances between nearest neighbor perches usually decrease, resulting in a relatively cluttered environment. Thus, the diameter of a cylinder that could penetrate vegetation without touching it would be expected to decrease as the average diameter of perches in an area decrease. Consequently, the limbs of a moving animal are more likely to bump into an obstacle when it travels through environments that are increasingly cluttered with smaller perch diameters. The limbs of A. sagrei used less lateral space for locomotion on perches with decreased diameters (Figs 7C, 8). Thus, altering the kinematics of the limbs can facilitate moving through a cluttered environment, and the kinematics during the swing phase of the stride are likely to be most important for affecting the clearance of the limbs relative to the obstacles in the environment.
Shorter limbs have evolved convergently in several species of
Anolis lizards that are found mostly on narrow perches and known as
twig ecomorphs (Moermond,
1979; Williams,
1983
; Losos,
1990
). Twig ecomorphs uniformly have slow maximal speeds of
running, which change little with perch diameter, whereas species with longer
limbs can attain quite rapid maximal speeds, which decrease substantially with
decreased perch diameter (Losos and
Sinervo, 1989
; Irschick and
Losos, 1996
). Some studies suggest the short limbs of twig
ecomorphs may increase their stability when moving on narrow perches
(Losos and Sinervo, 1989
;
Irschick and Losos, 1996
).
However, a frequently neglected fact is that long-limbed species manage to run
faster on narrower perches than short-limbed species in laboratory tests. We
suggest that the short limbs of twig ecomorphs have additional benefits that
have rarely been considered. If the kinematics of species with different limb
dimensions are similar, then the shorter-limbed species will have more medial
foot placement, which may benefit the orientation of the foot on the substrate
as well as increasing the clearance between the top of the perch and the
ventral surface of the body. Furthermore, shorter-limbed species will have
greater lateral clearance in cluttered natural environments. Most studies of
locomotion emphasize morphology and movements that are involved in enhancing
propulsive forces and hence are relevant to variation in maximal locomotor
speed. However, a relatively neglected factor for locomotion in arboreal and
cluttered environments is the simple ability to fit the body within confined
spaces.
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Abu-Ghalyun, Y., Greenwald, L., Hetherington, T. E. and Gaunt, A. S. (1988). The physiological basis of slow locomotion in chameleons. J. Exp. Zool. 245,225 -231.[Medline]
Blickhan, R. (1989). The spring-mass model for running and hopping. J. Biomech. 22,1217 -1227.[Medline]
Biewener, A. (1989). Scaling body support in mammals: Limb posture and muscle mechanics. Science 245, 45-48.[Medline]
Bonine, K., Gleeson, T. T. and Garland T. (2001). Comparative analysis of fiber-type composition in the iliofibularis muscle of phrynosomatid lizards (Squamata) J. Morphol. 250,265 -280.[CrossRef][Medline]
Buczek, F. L. and Cavanagh, P. R. (1990). Stance phase knee and ankle kinematics and kinetics during level and downhill running. Med. Sci. Sports Ex. 22,669 -677.
Carlson-Kuhta, P., Trank, T. V. and Smith, J. L.
(1998). Forms of forward quadrupedal locomotion. II. A comparison
of posture, hindlimb kinematics, and motor patterns for upslope and level
walking. J. Neurophysiol.
79,1687
-1701.
Cartmill, M. (1974). Pads and claws in arboreal locomotion. In Primate Locomotion (ed. F. A. J. Jenkins), pp. 45-83. New York: Academic Press.
Cartmill, M. (1985). Climbing. In Functional Vertebrate Morphology (ed. M. Hildebrand, D. M. Bramble, K. F. Liem and D. B. Wake), pp. 73-88. Cambridge: Belknap Press.
Crome, F. H. J. and Richards, G. C. (1988). Bats and gaps: microchiropteran community structure in a Queensland rain forest. Ecology 69,1960 -1969.
Farley, C. T. and Emshwiller, M. (1996).
Efficiency of uphill locomotion in nocturnal and diurnal lizards.
J. Exp. Biol. 199,587
-592.
Fieler, C. L. and Jayne, B. C. (1998). Effects
of speed on the hind limb kinematics of the lizard, Dipsosaurus dorsalis.J. Exp. Biol. 201,609
-622.
Full, R. J. and Tullis, A. (1990). Energetics of ascent: Insects on inclines. J. Exp. Biol. 149,307 -317.[Abstract]
Gatesy, S. M. (1991). Hind limb movements of the American alligator (Alligator mississippiensis) and postural grades. J. Zool. Lond. 224,577 -588.
Gatesy, S. M. and Biewener, A. A. (1991). Bipedal locomotion: effects of speed, size and limb posture in birds and humans. J. Zool. Lond. 224,127 -147.
Goslow, G. E. and Jenkins, F. A. (1983). The functional anatomy of the shoulder of the savannah monitor lizard (Varanus exanthematicus). J. Morphol. 175,195 -216.
Higham, T. E., Davenport, M. S. and Jayne, B. C.
(2001). Maneuvering in an arboreal habitat: the effects of
turning angle on the locomotion of three sympatric ecomorphs of
Anolis lizards. J. Exp. Biol.
204,4141
-4155.
Higham, T. E. and Jayne, B. C. (2004).
Locomotion of lizards on inclines and perches: hindlimb kinematics of an
arboreal specialist and a terrestrial generalist. J. Exp.
Biol. 207,233
-248.
Huey, R. B. and Hertz, P. E. (1982). Effects of body size and slope on sprint speed of a lizard (Stellio (Agama) stellio). J. Exp. Biol. 97,401 -409.
Irschick, D. J., Austin, C. C., Petren, K., Fisher, R. N., Losos, J. B. and Ellers, O. (1996). A comparative analysis of clinging ability among pad-bearing lizards. Biol. J. Linn. Soc. 59,21 -35.[CrossRef]
Irschick, D. J. and Jayne, B. C. (1998).
Effects of incline on speed, acceleration, body posture, and hindlimb
kinematics in two species of lizard, Callisaurus draconoides and
Uma scoparia. J. Exp. Biol.
201,273
-287.
Irschick, D. J. and Jayne, B. C. (1999).
Comparative three-dimensional kinematics of the hindlimb for high-speed
bipedal and quadrupedal locomotion of lizards. J. Exp.
Biol. 202,1047
-1065.
Irschick, D. J. and Losos, J. B. (1996). Morphology, ecology, and behavior of the twig anole, Anolis angusticeps. In Contributions to West Indian Herpetology: A Tribute to Albert Schwartz, vol. 12 (ed. R. Powell and R. W. Henderson), pp. 291-301. Ithaca: Society for the Study of Amphibians and Reptiles.
Irschick, D. J. and Losos, J. B. (1998). A comparative analysis of the ecological significance of maximal locomotor performance in Caribbean Anolis lizards. Evol. 52,219 -226.
Jayne, B. C. and Irschick, D. J. (1999).
Effects of incline and speed on the three-dimensional hindlimb kinematics of a
generalized iguanian lizard (Dipsosaurus dorsalis). J.
Exp. Biol. 202,143
-159.
Jenkins, F. A. (1974). Primate Locomotion. New York: Academic Press.
Losos, J. B. (1990). The evolution of form and function: morphology and locomotor performance in West Indian Anolis lizards. Evol. 44,1189 -1203.
Losos, J. B. and Irschick, D. J. (1996). The effect of perch diameter on escape behavior of Anolis lizards: lab predictions and field tests. Anim. Behav. 51,593 -602.[CrossRef]
Losos, J. B. and Sinervo, B. (1989). The effects of morphology and perch diameter on sprint performance of Anolis lizards. J. Exp. Biol. 145, 23-30.
Mattingly, W. B. and Jayne, B. C. (2004). Resource use in arboreal habitats: structure affects locomotion in four ecomorphs of Anolis lizards. Ecology 85, in press.
Moermond, T. (1979). Habitat constraints on the behavior, morphology, and community structure of Anolis lizards. Ecology 60,152 -164.
Moermond, T. C. (1986). A mechanistic approach to the structure of animal communities: Anolis lizards and birds. Am. Zool. 26,23 -37.
Pianka, E. R. (1969). Sympatry of desert lizards (Ctenotus) in Western Australia. Ecology 50,1012 -1030.
Peterson, J. A. (1984). The locomotion of Chamaeleo (Reptilia: Sauria) with particular reference to the forelimb. J. Zool. Lond. 202, 1-42.
Reilly, S. M. and Delancey, M. J. (1997). Sprawling locomotion in the lizard Sceloporus clarkii: the effects of speed on gait, hindlimb kinematics, and axial bending during walking. J. Zool. Lond. 243,417 -433.
Russell, A. P. and Bels, V. (2001). Biomechanics and kinematics of limb-based locomotion in lizards: review, synthesis and prospectus. Comp. Biochem. Physiol. 131A,89 -112.
Scheffe, H. (1959). The Analysis of Variance. New York: John Wiley & Sons, Inc.
Schoener, T. W. (1968). The Anolis lizards of Bimini: resource partitioning in a complex fauna. Ecology 49,704 -726.
Strasser, E., Fleagle, J., Rosenberger, A., and McHenry, H. (1998). Primate Locomotion: Recent Advances. New York: Plenum Press.
Taylor, C. R., Caldwell, S. L. and Rowntree, V. J. (1972). Running up and down hills: some consequences of size. Science 178,1096 -1097.[Medline]
Vilensky, J. A., Moore, A. M. and Libii, J. N. (1994). Squirrel monkey locomotion on an inclined treadmill: Implications for the evolution of gaits. J. Human Evol. 26,375 -386.[CrossRef]
Williams, E. E. (1983). Ecomorphs, faunas, island size, and diverse end points in island radiations of Anolis. In Lizard Ecology: Studies of a Model Organism (ed. R. B. Huey, E. R. Pianka and T. W. Schoener), pp.326 -370. Cambridge: Harvard University Press.
Williams, E. E. and Peterson, J. A. (1982). Convergent and alternative designs in the digital pads of scincid lizards. Science 215,1509 -1511.
Zaaf, A., Van Damme, R., Herrel, A. and Aerts, P.
(2001a). Spatio-temporal gait characteristics of level and
vertical locomotion in a ground-dwelling and a climbing gecko. J.
Exp. Biol. 204,1233
-1246.
Zaaf, A., Van Damme, R., Herrel, A. and Aerts, P. (2001b). Limb joint kinematics during vertical climbing and level running in a specialist climber: Gekko gecko Linneus, 1758 (Lacertilia: Gekkonidae). Belg. J. Zool. 131,173 -182.