Physiologists have long been interested in which intrinsic factors of organisms affect their maximum speed of locomotion. Among other factors, the total amount of power that animals can produce may play a central role in limiting maximum speed, but testing this hypothesis is challenging(Farley, 1997; Irschick et al., 2001). Previous authors have suggested that if the speed of an animal moving up successively steeper inclines (or moving with increasingly large loads)declines, but its power output increases, then power is not limiting(Farley, 1997; Irschick et al., 2001)(Fig. 1A). By contrast, if maximum speed on increasingly steep inclines, or with increasingly large loads, decreases, but maximum power output remains the same, then the total amount of power an animal can produce may limit maximum speed(Fig. 1B). However, it is important to consider that although Fig. 1B is consistent with a hypothesis of power limitation, another possible explanation that could explain such a pattern is that power output covaries with some other mechanical variable. If this were the case, then the decline in speed might not be due to a lack of power. Nevertheless, studies that examine how extrinsic factors affect power output could shed light on the general issue of whether power output limits maximum speed. Here, we attempt to differentiate between the two above hypotheses by examining power output in two species of arboreal geckos climbing vertically with large loads.

Fig. 1.

Theoretical relationships between mass-specific power output (yaxis) versus speed (x axis) if (A) mass-specific power output does not limit speed and (B) mass-specific power output limits speed. Different lines represent different loading conditions (Load A < Load B< Load C < Load D). Vmax is defined as the maximal speed the animal can attain under any circumstances; Pmaxis defined as the maximal mass-specific power output the animal can attain under any circumstances.

Fig. 1.

Theoretical relationships between mass-specific power output (yaxis) versus speed (x axis) if (A) mass-specific power output does not limit speed and (B) mass-specific power output limits speed. Different lines represent different loading conditions (Load A < Load B< Load C < Load D). Vmax is defined as the maximal speed the animal can attain under any circumstances; Pmaxis defined as the maximal mass-specific power output the animal can attain under any circumstances.

A second factor that could influence power output during locomotion is animal size (Hill, 1950; Marden, 1987). Previous authors have suggested that large animals should produce less power than small animals per unit body mass because of the manner by which surface area (and hence force) scales with size (e.g. Wilson et al., 2000; Toro et al.,2003), although this expectation has not always been borne out(Pennycuick, 1969, 1972; Marden, 1987). While several studies have addressed the general issue of whether large and small animals differ in power output during various activities(Marden, 1987; Wilson et al., 2000), we are aware of no studies that have examined this issue for vertical locomotion,such as observed in many arboreal lizard or insect species (but see Farley, 1997). Thus, another aspect of our study concerns a comparison of power output between two gecko species that vary greatly in size (see below). While such two-species comparisons are commonplace in physiological studies, their interpretation is often controversial (Garland and Adolph,1994), so we interpret these data cautiously.

The effects of size and loading on limb kinematics are also poorly resolved for vertical locomotion. As the amount of a load increases, one predicts that maximum speed should decrease when moving vertically, but whether animals achieve this by equally diminishing stride length or stride frequency is unknown. Furthermore, how the addition of loads affects the manner by which animals increase in speed on vertical surfaces has rarely been examined, and there are no studies on the interactive effects of size and loading on kinematics. This last issue is of particular interest to physiologists because previous work has shown that, on horizontal surfaces, small animals tend to modulate speed by changing stride frequency, whereas larger animals tend to change stride length (Gatesy and Biewener,1991). Furthermore, a recent study has shown that a climbing gecko(Gekko gecko) modulates speed almost entirely by changing stride frequency, whereas a similarly sized terrestrial gecko (Eublepharis macularius) changes speed primarily by changing stride length(Zaaf et al., 2001). Thus,data on how size and loading affect limb kinematics during vertical climbing might shed light on these issues.

Small climbing lizards such as geckos provide an excellent opportunity for testing the effects of size and loading on locomotion. Female geckos frequently carry large eggs prior to laying, which can approximate 10-30% of their body mass (D. J. Irschick, personal observation), so geckos are accustomed to carrying large loads. Furthermore, climbing geckos differ dramatically in size among species (e.g. 1-70 g difference in mass among species) (Zaaf and Van Damme,2001).

In the present study, we tested the effects of size and loading on the vertical locomotion of two species of geckos (Gekko gecko and Hemidactylus garnoti). Whereas G. gecko is the largest extant gecko with derived toepads, and achieves a mass greater than 70 g, H. garnoti is a small (<5 g) climbing gecko that is more representative of the large family of geckos. However, these two species are generally similar in terms of their morphology, relative toepad dimensions and natural history, making them an excellent case study for comparison. We addressed three primary issues. First, does mass-specific power output limit locomotor performance in geckos? If the hypothesis of power limitation is correct, then as lizards are loaded with successively greater weights, speed should decrease, but mass-specific power (per unit body mass) should remain constant. Alternatively, if power is not limiting, then as successively greater weights are added, speed should decrease, but mass-specific power (per unit body mass) should increase. Second, how does loading affect the kinematics of limb movement? Third, does size affect mass-specific power output? More specifically, we predicted that larger geckos (G. gecko)would produce less mass-specific power (relative to size) than smaller geckos(H. garnoti).

### Trial subjects

We elicited suitable locomotion from six Gekko gecko L.(mass=43.3±1.5 g, mean ± s.d.) and twelve Hemidactylus garnoti Dumeril and Bibron (mass 2.4±0.2 g, mean± s.d.). Geckos were maintained alone or in pairs in cages(40 cm × 100 cm × 30 cm for G. gecko; 15 cm × 25 cm× 20 cm for H. garnoti) placed in a temperature controlled room(29±2°C) illuminated for 12 h a day. They were provided crickets with a vitamin/mineral supplement three times a week, and watered once daily.

### Locomotion trials

We induced geckos to run vertically up a custom-built racetrack. The racetrack had Plexiglas walls attached on either side to a wooden base that was 13 cm wide and 150 cm long. We filmed the lizards from a dorsal perspective at 250 Hz with a motionscope PCI camera (Redlake, San Diego, CA,USA) attached to a PC computer. All locomotion clips were digitized using Peak performance MOTUS software.

Prior to each locomotion trial, lizards were placed either in plastic bags(H. garnoti) or canvas bags (G. gecko) inside an incubator set to 30°C for at least 30 min. We placed loads of 100-200% body mass(BM) on all individuals of H. garnoti, and loads of 100% BM on all individuals of G. gecko. For G. gecko, we acquired locomotion for movement uphill when unloaded and with a 100% BM load, whereas for H. garnoti, we acquired locomotion when moving uphill unloaded and with loads of 100%, 150% and 200% BM. We used small, thin lead weights that were wrapped approximately around the center of mass of each lizard(placed centrally between each girdle)(Fig. 2). The weights were attached to the body by placing a small piece of tape on the dorsal and ventral sides of the lizard. The width and thickness of the strips for the four load types were similar for each species, but the strips for the heavier loads were longer, and hence wrapped around the body to a greater degree. The loads did not appear to affect the overall locomotor behavior of the lizards,or the amount of lateral flexion of the back (see below). To determine whether the presence of the weight itself affected locomotion, we wrapped a piece of thin paper around the body of each H. garnoti that was similar in dimensions to the above weights, but only approximated 2% BM.

Fig. 2.

Large (top, G. gecko) and small (bottom, H. garnoti)geckos with representative loads of 100% body mass. Photograph by Margarita Ramos.

Fig. 2.

Large (top, G. gecko) and small (bottom, H. garnoti)geckos with representative loads of 100% body mass. Photograph by Margarita Ramos.

Each lizard was given ten opportunities to run at maximum speed with each of these weights. Loading condition was randomly assigned across days and lizards were tested on multiple, non-consecutive, days with the same loads. For each trial, we attempted to gain 2-5 strides of steady speed locomotion. We did not include any strides in which the animal was clearly accelerating or decelerating over the course of several strides. All data were analyzed on a stride-by-stride basis. We recorded footfall patterns of the hindfoot for each lizard, and defined a stride as the interval between consecutive footfalls of the right hindfoot (from a dorsal perspective). For each stride, we calculated stride length and stride frequency, and duty factor, speed and mean mass-specific power output per stride. Stride length was calculated as the displacement of the tip of the snout between consecutive footfalls; stride frequency was calculated as the reciprocal of stride duration (the time between consecutive footfalls); duty factor was calculated as the duration of foot contact (i.e. step duration) divided by stride duration; speed was calculated as stride length divided by stride duration. Since we used strides of steady speed locomotion, we only took into account gravitational forces to calculate mass-specific power output per unit body mass. Thus, mass-specific power output per unit body mass was calculated as the product of total mass m, gravitational acceleration (i.e. F=mg) and speed, divided by body mass. In this case, total mass equals the sum of body mass and the weight of the load.

To determine whether the addition of loads altered locomotor posture, we digitized the tip of the snout and tail, and three small evenly spaced white dots on the back, and calculated the angles of the head, trunk and tail over the whole stride cycle. The angle of the head was defined as the angle between the tip of the snout and the two dorsal points closest to the head, with angles of 180° indicating that the head was in alignment with the body,and angles greater or less than 180° indicating movement of the head towards the left or right, respectively. The angle of the trunk was defined as the angle between the three dorsal points, with angles of 180° indicating that the trunk was straight, and angles greater or less than 180°indicating lateral flexion towards the left or right, respectively. The angle of the tail was defined as the angle between the tip of the tail and the two most posterior dorsal points, with angles of 180° indicating that the tail was in alignment with the body, and angles greater or less than 180°indicating movement of the tail towards the left or right, respectively. For the same set of strides used in step (1) below, we calculated maximum and minimum values of each kinematic variable for each stride and compared loading conditions.

### Statistical analyses

All values were log10-transformed prior to statistical analyses. To determine whether loading affected angular kinematics, we conducted separate multivariate analyses of variance (MANOVAs) within each species,using the maximum and minimum values for each kinematic variable as dependent variables, and loading condition as the independent variable. If the MANOVA was significant within either species, we then used ANOVAs with loading condition as a factor and the different angles as dependent variables. We then used LSD post-hoc tests to determine where differences lie in the data structure.

### Angular kinematics

The MANOVA comparing loading conditions for H. garnoti was barely significant (Wilks' λ=0.344, F24,112=1.68, P=0.037), whereas the MANOVA for G. gecko was non-significant (Wilks' λ=0.125, F2,6=2.334, P>0.30) (Tables 1, 2). One-way ANOVAs within H. garnoti showed that the only variable that differed significantly among loading conditions was the minimum value of trunk angle(F4,37=2.91, P=0.034), which only differed significantly between the unloaded and 200% loading conditions(post-hoc test, P=0.025). Thus, overall, loading does not substantially affect angular kinematics during vertical locomotion in either gecko species.

Table 1.

Descriptive angular kinematic statistics for small (H. garnoti) geckos running vertically with various loads

VariableLoadNAngle of variable (deg.)Speed (m s-1)
Max. 203.67±2.81 0.83±0.08
202.30±3.18 1.45±0.19
100 209.20±3.00 0.61±0.05
150 205.90±2.81 0.64±0.05
200 203.90±2.81 0.53±0.03
Min. 160.37±2.99 0.83±0.08
156.91±3.39 1.45±0.19
100 158.33±3.17 0.61±0.05
150 159.20±3.00 0.64±0.05
200 157.23±3.00 0.53±0.03
Trunk
Max. 212.12±3.05 0.83±0.08
208.07±3.46 1.45±0.19
100 208.27±2.24 0.61±0.05
150 202.27±3.05 0.64±0.05
200 210.16±3.05 0.53±0.03
Min. 147.19±3.05 0.83±0.08
155.78±3.46 1.45±0.19
100 150.28±2.24 0.61±0.05
150 151.41±3.05 0.64±0.05
200 160.72±3.05 0.53±0.03
Tail
Max. 209.37±6.06 0.83±0.08
212.97±6.88 1.45±0.19
100 193.78±6.43 0.61±0.05
150 197.28±6.06 0.64±0.05
200 205.78±6.06 0.53±0.03
Min. 149.37±4.63 0.83±0.08
157.69±5.25 1.45±0.19
100 163.14±4.91 0.61±0.05
150 164.16±4.63 0.64±0.05
200 165.67±4.63 0.53±0.03
VariableLoadNAngle of variable (deg.)Speed (m s-1)
Max. 203.67±2.81 0.83±0.08
202.30±3.18 1.45±0.19
100 209.20±3.00 0.61±0.05
150 205.90±2.81 0.64±0.05
200 203.90±2.81 0.53±0.03
Min. 160.37±2.99 0.83±0.08
156.91±3.39 1.45±0.19
100 158.33±3.17 0.61±0.05
150 159.20±3.00 0.64±0.05
200 157.23±3.00 0.53±0.03
Trunk
Max. 212.12±3.05 0.83±0.08
208.07±3.46 1.45±0.19
100 208.27±2.24 0.61±0.05
150 202.27±3.05 0.64±0.05
200 210.16±3.05 0.53±0.03
Min. 147.19±3.05 0.83±0.08
155.78±3.46 1.45±0.19
100 150.28±2.24 0.61±0.05
150 151.41±3.05 0.64±0.05
200 160.72±3.05 0.53±0.03
Tail
Max. 209.37±6.06 0.83±0.08
212.97±6.88 1.45±0.19
100 193.78±6.43 0.61±0.05
150 197.28±6.06 0.64±0.05
200 205.78±6.06 0.53±0.03
Min. 149.37±4.63 0.83±0.08
157.69±5.25 1.45±0.19
100 163.14±4.91 0.61±0.05
150 164.16±4.63 0.64±0.05
200 165.67±4.63 0.53±0.03

N, number of individuals (one stride per individual).

Values are means ± s.e.m.

Max., maximum; Min., minimum.

Speeds are slightly different from the values in Table 3 because slightly different groups of animals were used.

Table 2.

Descriptive angular kinematic statistics for large (G. gecko) geckos running vertically with various loads

VariableLoadNAngle of variable (deg.)Speed (m s−1
Max. 198.79±5.97 0.96±0.07
100 191.83±6.67 0.69±0.07
Min. 162.03±5.31 0.96±0.07
100 150.44±5.93 0.69±0.07
Trunk
Max. 203.94±6.10 0.96±0.07
100 217.11±6.82 0.69±0.07
Min. 152.56±3.48 0.96±0.07
100 166.84±3.89 0.69±0.07
Tail
Max. 197.74±8.41 0.96±0.07
100 213.94±9.40 0.69±0.07
Min. 154.48±10.64 0.96±0.07
100 121.57±11.90 0.69±0.07
VariableLoadNAngle of variable (deg.)Speed (m s−1
Max. 198.79±5.97 0.96±0.07
100 191.83±6.67 0.69±0.07
Min. 162.03±5.31 0.96±0.07
100 150.44±5.93 0.69±0.07
Trunk
Max. 203.94±6.10 0.96±0.07
100 217.11±6.82 0.69±0.07
Min. 152.56±3.48 0.96±0.07
100 166.84±3.89 0.69±0.07
Tail
Max. 197.74±8.41 0.96±0.07
100 213.94±9.40 0.69±0.07
Min. 154.48±10.64 0.96±0.07
100 121.57±11.90 0.69±0.07

N, number of individuals (one stride per individual).

Values are means ± s.e.m.

Max., maximum; Min., minimum.

Speeds are slightly different from the values in Table 3 because slightly different groups of animals were used.

### Power output and speed

Table 3.

Descriptive statistics for power output and speed for small (H. garnoti) and large (G. gecko) geckos running vertically with various loading conditions

Mass-specific power (W kg−1)
Speed (m s−1)
H. garnoti 11 8.27±0.66 4.14-11.04 0.84±0.07 0.42-1.13
11 13.01±1.47 6.06-19.96 1.30±0.15 0.61-2.00
100 12.47±0.82 9.93-16.98 0.63±0.05 0.48-0.91
150 15.99±1.07 12.10-22.95 0.64±0.14 0.46-0.94
200 16.16±0.93 12.28-20.01 0.53±0.10 0.39-0.63
G. gecko 9.78±0.70 7.93-12.03 1.00±0.07 0.81-1.23
100 13.61±1.30 10.07-16.32 0.69±0.07 0.52-0.83
Mass-specific power (W kg−1)
Speed (m s−1)
H. garnoti 11 8.27±0.66 4.14-11.04 0.84±0.07 0.42-1.13
11 13.01±1.47 6.06-19.96 1.30±0.15 0.61-2.00
100 12.47±0.82 9.93-16.98 0.63±0.05 0.48-0.91
150 15.99±1.07 12.10-22.95 0.64±0.14 0.46-0.94
200 16.16±0.93 12.28-20.01 0.53±0.10 0.39-0.63
G. gecko 9.78±0.70 7.93-12.03 1.00±0.07 0.81-1.23
100 13.61±1.30 10.07-16.32 0.69±0.07 0.52-0.83

N, number of individuals (one stride per individual).

2' condition, the paper control; 0', unloaded condition.

*

The loads are denoted as % body mass.

Table 4.

Results from one-way ANOVAs using loading condition as a factor for detecting differences in mass-specific power output and speed within H. garnoti and G. gecko

Fd.f.P-value
H. garnoti
Mass-specific power 10.75 1,4 <0.0001
Speed 14.19 1,4 <0.0001
G. gecko
Mass-specific power 7.66 1,1 0.02
Speed 9.55 1,1 0.02
Fd.f.P-value
H. garnoti
Mass-specific power 10.75 1,4 <0.0001
Speed 14.19 1,4 <0.0001
G. gecko
Mass-specific power 7.66 1,1 0.02
Speed 9.55 1,1 0.02

Analyses using only the strides that produced the maximum mass-specific power within each species (regardless of loading condition) show that mean maximum mass-specific power output is 33% greater in H. garnoti than in G. gecko (one-way ANOVA, F1,1=7.2, P<0.025; Fig. 3A),whereas maximum speed is only slightly, and non-significantly, greater (19%)in G. gecko (one-way ANOVA, F1,1=1.6, P>0.20; Fig. 3B).

Fig. 3.

Maximum values (means ± 1 s.e.m.) of mass-specific power(A) and speed (B) for small (H. garnoti) and large (G. gecko) geckos.

Fig. 3.

Maximum values (means ± 1 s.e.m.) of mass-specific power(A) and speed (B) for small (H. garnoti) and large (G. gecko) geckos.

### Speed modulation

The bivariate regression analyses show that under all loading conditions,and in both species, stride frequency increases to a greater extent with speed than does stride length (Table 5;Fig. 4). This suggests that in all cases, the geckos modulate speed primarily by altering stride frequency. However, duty factor shows no obvious relationship with speed, with the exception of H. garnoti moving unloaded(Table 5). Based on multiple regression analyses, speed and loading condition (independent variables)explain 70% and 89% of the variation in stride length and frequency,respectively, for H. garnoti(Table 6), whereas for G. gecko, they explain 69% and 70% of the variation, respectively. Speed and loading condition explain 58% (H. garnoti) and 70% (G. gecko) of the variation in duty factor from these multiple regressions.

Table 5.

Results from regression analyses using stride length, stride frequency or duty factor as dependent variables, and speed as the independent variable

Stride length
Stride frequency
Duty factor
H. garnoti
0.24±0.05*** −1.19±0.02*** 0.76±0.05*** 1.19±0.02*** −0.13±0.05** −0.33±0.01***
0.19±0.04*** −1.23±0.01*** 0.81±0.04*** 1.23±0.01*** 0.01±0.04 −0.13±0.01***
100 0.33±0.05*** −1.21±0.02*** 0.67±0.05*** 1.21±0.02*** −0.09±0.05 −0.27±0.02***
150 0.30±0.06*** −1.24±0.02*** 0.70±0.06*** 1.24±0.02*** −0.10±0.07 −0.25±0.02***
200 0.32±0.06*** −1.25±0.02*** 0.68±0.06*** 1.25±0.02*** −0.003±0.07 −0.21±0.03***
G. gekko
0.34±0.15* −0.84±0.02*** 0.66±0.15*** 0.84±0.02*** −0.08±0.11 −0.31±0.02***
100 0.27±0.13* −0.95±0.04*** 0.73±0.13*** 0.95±0.04*** −0.02±0.07 −0.21±0.02***
Stride length
Stride frequency
Duty factor
H. garnoti
0.24±0.05*** −1.19±0.02*** 0.76±0.05*** 1.19±0.02*** −0.13±0.05** −0.33±0.01***
0.19±0.04*** −1.23±0.01*** 0.81±0.04*** 1.23±0.01*** 0.01±0.04 −0.13±0.01***
100 0.33±0.05*** −1.21±0.02*** 0.67±0.05*** 1.21±0.02*** −0.09±0.05 −0.27±0.02***
150 0.30±0.06*** −1.24±0.02*** 0.70±0.06*** 1.24±0.02*** −0.10±0.07 −0.25±0.02***
200 0.32±0.06*** −1.25±0.02*** 0.68±0.06*** 1.25±0.02*** −0.003±0.07 −0.21±0.03***
G. gekko
0.34±0.15* −0.84±0.02*** 0.66±0.15*** 0.84±0.02*** −0.08±0.11 −0.31±0.02***
100 0.27±0.13* −0.95±0.04*** 0.73±0.13*** 0.95±0.04*** −0.02±0.07 −0.21±0.02***

Asterisks indicate significant relationships between the independent and dependent variables; *P<0.05, ***P<0.0001. Values of stride length (cm), stride frequency (Hz), duty factor and speed (m s−1) were log10-transformed prior to statistical analyses.

Values are ±1 s.e.m.

Fig. 4.

Scatterplots of stride length (A,C,E) and stride frequency (B,D,F) versus speed (x axis) for various loading conditions during uphill climbing for small (open circles; H. garnoti) and large(filled squares; G. gecko) geckos. Note that in none of the plots does stride length or stride frequency level off as speed increases. Values are log10-transformed.

Fig. 4.

Scatterplots of stride length (A,C,E) and stride frequency (B,D,F) versus speed (x axis) for various loading conditions during uphill climbing for small (open circles; H. garnoti) and large(filled squares; G. gecko) geckos. Note that in none of the plots does stride length or stride frequency level off as speed increases. Values are log10-transformed.

Table 6.

Results from multiple regressions within both H. garnoti and G. gecko attempting to explain variation in stride length,stride frequency and duty factor (dependent variables) using speed and the loading condition (independent variables) in each regression

Variable
DependentIndependentrFPPartial r
H. garnoti
Stride length Speed 0.70 175.2 <0.0001 0.50
Stride frequency Speed 0.89 686.5 <0.0001 0.88
Duty factor Speed 0.58 93.4 <0.0001 −0.13
G. gecko
Stride length Speed 0.69 26.71 <0.0001 0.36
Stride frequency Speed 0.70 28.3 <0.0001 0.69
Duty factor Load 0.70 56.7 <0.0001 0.70
Variable
DependentIndependentrFPPartial r
H. garnoti
Stride length Speed 0.70 175.2 <0.0001 0.50
Stride frequency Speed 0.89 686.5 <0.0001 0.88
Duty factor Speed 0.58 93.4 <0.0001 −0.13
G. gecko
Stride length Speed 0.69 26.71 <0.0001 0.36
Stride frequency Speed 0.70 28.3 <0.0001 0.69
Duty factor Load 0.70 56.7 <0.0001 0.70

With the addition of increasingly large loads, both gecko species take smaller but more strides per unit distance for a given speed(Table 7). The multiple regression analyses with stride length or stride frequency as dependent variable, and species, loading condition and speed as independent variables,show that for a given speed and load, the two species differ in stride length and stride frequency: G. gecko takes larger but fewer strides than H. garnoti (Table 7). For a given speed and load, G. gecko has a greater duty factor than H. garnoti, which is not surprising, as larger lizards likely need more time to push off with larger loads(Table 7).

Table 7.

Results from multiple regressions pooling all H. garnoti (species=1) and G. gecko (species=2), attempting to explain variation in stride length, stride frequency and duty factor (dependent variables) using speed, loading condition and species (independent variables)in each regression

Variable
DependentIndependentrFPPartial r
Stride length Speed 0.91 307.2 <0.0001 0.50
Species    0.88
Stride frequency Speed 0.91 316.6 <0.0001 0.80
Species    −0.88
Duty factor Speed 0.62 40.8 <0.0001 0.48
Species    −0.22
Variable
DependentIndependentrFPPartial r
Stride length Speed 0.91 307.2 <0.0001 0.50
Species    0.88
Stride frequency Speed 0.91 316.6 <0.0001 0.80
Species    −0.88
Duty factor Speed 0.62 40.8 <0.0001 0.48
Species    −0.22

We also repeated the analyses in Table 7 by analyzing speed and stride length on a size-adjusted basis,by dividing both variables by mass, but keeping the other variables(independent variables = loading and species type; dependent variables =stride frequency and duty factor) constant(Table 8). This reanalysis shows that for a given relative speed and load, G. gecko takes larger relative strides at a lower frequency. At a given relative speed, both species use similar duty factors (no species effect)(Table 8).

Table 8.

Results from multiple regressions pooling all H. garnoti (species=1) and G. gecko (species=2), attempting to explain variation in relative stride length, stride frequency and duty factor(dependent variables) using relative speed, loading condition and species(independent variables) in each regression

Variable
DependentIndependentrFPPartial r
Relative stride length Relative speed 0.93 449.5 <0.0001 0.30
Species    0.79
Stride frequency Relative speed 0.76 92.2 <0.0001 −0.28
Species    −0.64
Duty factor Relative speed 0.62 40.8 <0.0001 0.33
Species    0.07 (NS)
Variable
DependentIndependentrFPPartial r
Relative stride length Relative speed 0.93 449.5 <0.0001 0.30
Species    0.79
Stride frequency Relative speed 0.76 92.2 <0.0001 −0.28
Species    −0.64
Duty factor Relative speed 0.62 40.8 <0.0001 0.33
Species    0.07 (NS)

NS, non-significant.

Relative stride length, stride length divided by mass; Relative speed,speed divided by mass.

### Does power limit performance?

A central, yet largely unresolved, issue among physiologists interested in locomotion is which factors limit maximum speed during running, swimming or flying (Ellington, 1991; Swoap et al., 1993; Wakeling and Johnston, 1998; Irschick et al., 2001; Askew and Marsh, 2002). Some authors have suggested that mechanical power output can limit maximum speed,at least for certain taxa such as large, flying animals (Pennycuick, 1969, 1972; Ellington, 1991). Determining whether maximum power output is limiting is difficult, but our data suggest that maximum mass-specific power output may limit maximum speed in at least one of the two gecko species (H. garnoti). Our results show a significant difference in mass-specific power output per unit body mass between the unloaded condition and any given loaded condition. However, one surprising result was that speed was somewhat higher in the control' (2% body mass condition) compared to the unloaded condition for the small gecko (H. garnoti). This result is unexpected, as geckos in both conditions were run an approximately equal number of times. One possibility is that the addition of loads presented an additional stimulus to the animals that elicited higher speeds. In any case, since H. garnoti with the 2%load and all other loads all experienced similar conditions, any comparisons among them should be valid.

Fig. 5.

Scatterplots of mass-specific power output versus speed for all strides obtained for both gecko species. (A) Mass-specific power output against speed for H. garnoti under five loading conditions (filled circles, unloaded; open squares, 2% BM; filled triangles, 100% BM; grey inverted triangles, 150% BM; grey diamonds, 200% BM). We obtained one extremely high value of mass-specific power output under the 150% loading condition. (B) Mass-specific power output against speed for G. geckounder two loading conditions (filled circles, unloaded; filled triangles, 100%BM). Extrapolation of maximal mass-specific power output to maximal speed (R. Van Damme, unpublished data) gives a value of 14.17 W kg-1 (filled circles). For both species, most of the loading conditions tend to level off near Pmax, supporting the hypothesis that mass-specific power output limits speed in these lizards.

Fig. 5.

Scatterplots of mass-specific power output versus speed for all strides obtained for both gecko species. (A) Mass-specific power output against speed for H. garnoti under five loading conditions (filled circles, unloaded; open squares, 2% BM; filled triangles, 100% BM; grey inverted triangles, 150% BM; grey diamonds, 200% BM). We obtained one extremely high value of mass-specific power output under the 150% loading condition. (B) Mass-specific power output against speed for G. geckounder two loading conditions (filled circles, unloaded; filled triangles, 100%BM). Extrapolation of maximal mass-specific power output to maximal speed (R. Van Damme, unpublished data) gives a value of 14.17 W kg-1 (filled circles). For both species, most of the loading conditions tend to level off near Pmax, supporting the hypothesis that mass-specific power output limits speed in these lizards.

Irschick et al. (2001)examined the power output of H. garnoti running at submaximal preferred speeds with 30% BM and 60% BM loads on a vertical force platform,and concluded that power output did not limit maximum speed. However, that conclusion was based on submaximal running, as opposed to maximal or near-maximal running in the current study. Thus, power may not limit uphill loaded locomotion until geckos run at maximum speeds. Farley(1997) examined power output in two species of small (<10 g) terrestrial lizards when running unloaded on level and inclined surfaces (+20°, +40°) and concluded that the mechanical power required to lift the body vertically was 3.9 times greater than the external mechanical power output when moving on the level surface. By comparison, H. garnoti double their mean power output on changing from running unloaded uphill to running uphill with a 200% BM load. Farley(1997) found that power output continued to increase as each lizard species ran up successively steeper inclines, even though maximum speed declined, thus refuting the hypothesis that mass-specific power limits maximum speed. This difference between the work of Farley (1997) and ours can be explained by the different demands of horizontal and vertical running in lizards. When running either horizontally or on an incline when unloaded,maximum power output clearly does not limit maximum speed in lizards, but in our experiments, we forced the lizards to conduct tasks (running uphill with a load) that we knew would result in much higher total power outputs. Thus, it is possible that power output does not limit maximum speed for lizards running up relatively shallow inclines, or that move on horizontal surfaces, but power may limit vertical locomotion in lizards, particularly when moving with large loads.

Another aspect of locomotion that requires high power output is acceleration, especially during sharp turns such as observed in the C-start escape response of fish (Wakeling and Johnston, 1998). The ability to make abrupt turns is a key part of the escape response of geckos, although few studies have examined suchmaneuvering' ability in lizards (but see Van Damme and Vanhooydonck,2002; Vanhooydonck and Van Damme, 2003), and its relation to power output.

### Does body size affect mass-specific power output?

Due to a lack of loading studies for animals moving uphill, the most relevant available studies for examining the effects of loading on mass-specific power output are of flying organisms such as insects, bats and birds. The dynamics of moving directly uphill and flying are similar, in that in both cases animals must work against gravity, and thus produce a substantial amount of power. Marden(1987) examined the largest load that several insect, bat and bird species could carry to understand whether species of different sizes can carry the same percentage of body mass. Contrary to theoretical predictions, the maximum lift per unit flight muscle mass was similar among taxonomic groups (54-63 N kg-1). On this basis, large flying animals (e.g. birds, bats) were capable of carrying similar loads (as a percentage of body mass) to relatively small flying animals, such as insects. In addition, interspecific differences in short-duration power output were primarily related to the flight muscle ratio(ratio of the mass of flight muscles divided by all other muscles in the wing; Marden, 1987), suggesting that species with high mass-specific power outputs have evolved large amounts of flight muscle.

While our results show that H. garnoti has a higher maximal mass-specific power output than G. gecko, one should interpret this difference cautiously. Because the unloaded speeds of G. gecko may be slightly less than maximum capacity, it is possible that we have underestimated their maximum power output. Extrapolation of our results to the maximal speed measured by Van Damme and Zaaf (see above) gives a mass-specific power output of 14.13 W kg-1. If we replace lower values ofmaximal mass-specific power output' (for each individual) with this value,the difference between H. garnoti and G. gecko is not significant (one way ANOVA; F1,16=2.63, P=0.12). This result corresponds to those from studies on flying animals (see above). Thus, more data on the maximum speeds of G. gecko as well as its relationship to power output and loading appear to be necessary before firm conclusions can be drawn.

Several studies have investigated the effects of loading on energetics(Taylor et al., 1980; Herreid and Full, 1985; Kram, 1996), kinematics(Wren et al., 1998; Zani and Claussen, 1995; Hoyt et al., 2000) and performance (Zani and Claussen,1995; Wren et al.,1998), but few studies have studied the effects of loading on mass-specific power output and kinematics when moving uphill.

First, it is clear from our results that the addition of weights does not affect the speed modulation strategy of either H. garnoti or G. gecko. Regardless of loading condition, speed increases primarily by increasing stride frequency in both species. The fact that geckos modulate their speed mainly by altering stride frequency and not stride length is in accordance with the results of Zaaf et al.(2001), who found that G. gecko is primarily a frequency modulator on both vertical and horizontal surfaces.

At a given speed, however, the addition of loads significantly affects both stride length and stride frequency. Both species take smaller but more strides with heavier loads and thus, the effect of loading condition seems to be the same in H. garnoti and G. gecko. It is unclear why this is the case. Smaller steps (and hence strides) with heavier loads might reflectuncertainty' on part of the animal, analogous to the hesitant small steps of humans walking on slippery surfaces, or of impaired or elderly people(Zatsiorsky et al., 1994; Grabiner, 1997; Vaughan, 1997). The increase in stride frequency when carrying a load, as observed in this study,corresponds to the results of some studies on load carrying (e.g. Cooke et al., 1991), but differs from others (e.g. Hoyt et al.,2000). The effects of loading and size on duty factor are also apparent. First, within H. garnoti at a given speed, duty factor increases with increased loading, while for a given load, duty factor declines with speed. Similarly, within G. gecko at a given speed, duty factor also increases with loading. These results make intuitive sense, as the addition of loads probably forces these lizards to spend more time pushing against the ground to generate the required forces for movement.

In sum, several key findings are apparent from our data. First, several lines of evidence suggest that power limits maximum speed in both gecko species. Stride frequency does not level off as speed increases for any loading condition in either species, suggesting that lizards do not reach a maximum stride frequency that they cannot exceed. Further, even though mass-specific power output increases significantly between the unloaded and any loaded condition, the small H. garnoti produces similar amounts of power when running with 150% and 200% BM loads, suggesting that they have reached their power limit. Second, while the large gecko produced approximately 33% less maximum power than the smaller H. garnoti,this difference disappeared when we used the slightly higher speeds for G. gecko gathered by other researchers. Finally, speed is primarily modulated by changes in stride frequency, regardless of loading condition and species. At a given speed, on the other hand, the addition of loads causes both species to take smaller, but more, strides per unit distance.

We thank Peter Aerts and two anonymous reviewers for helpful comments on previous versions of this manuscript, and especially thank Robert Full and Kellar Autumn for providing the original inspiration for this study. This work was supported by an NSF grant to D. Irschick (IBN 9983003) and generous funding from DARPA. A. Herrel and B. Vanhooydonck are postdoctoral fellows at the Fund for Scientific Research Flanders (FWO-Vl).

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