Postural adaptations may contribute to the unique locomotor energetics seen in hopping kangaroos

  1. Lauren Thornton
  2. Taylor Dick
  3. John R Hutchinson
  4. Glen A Lichtwark
  5. Craig P McGowan
  6. Jonas Rubenson
  7. Alexis Wiktorowicz-Conroy
  8. Christofer J Clemente  Is a corresponding author
  1. School of Science, Technology, and Engineering, University of the Sunshine Coast, Australia
  2. School of Biomedical Sciences, University of Queensland, Australia
  3. Structure and Motion Lab, Department of Comparative Biomedical Sciences, The Royal Veterinary College, United Kingdom
  4. School of Exercise and Nutrition Science, Queensland University of Technology, Australia
  5. Department of Integrative Anatomical Sciences, Keck School of Medicine University of Southern California, United States
  6. Biomechanics Laboratory, Department of Kinesiology, The Pennsylvania State University, United States
7 figures, 8 tables and 1 additional file

Figures

Figure 1 with 3 supplements
Illustration of the kangaroo model and moment arms for the ankle.

(a) Illustration of the kangaroo model. Total leg length was calculated as the sum of the segment lengths (solid black lines) in the hindlimb and compared to the pelvis-to-toe distance (dashed line) to calculate the crouch factor. Joint angles were determined for the hip, h, knee, k, ankle, a, and metatarsophalangeal, m, joints. The model markers (red circles) indicate the position of the reflective markers placed on the kangaroos in the experimental trials and were used to characterise the movement of segments in the musculoskeletal model. (b) Illustration of ankle effective mechanical advantage, EMA, muscle moment arm, r, and external moment arm, R, as the perpendicular distance to the Achilles tendon line of action and ground reaction force (GRF) vector, respectively. The centre of pressure (CoP) was tracked in the fore-aft direction.

Figure 1—figure supplement 1
Distribution of trial speeds and number of trials (n) per kangaroo (6.25±5.02 trials per kangaroo).
Figure 1—video 1
A red kangaroo hopping on the force plate during data collection.
Figure 1—video 2
Driving the musculoskeletal model with a recorded hopping trial.

The gastrocnemius and plantaris muscle-tendon unit (Achilles) is shown in blue. The GRF appears in green. Markers associating the recorded kangaroos with the model are in pink.

Figure 2 with 3 supplements
Horizontal fore-aft (dashed lines) and vertical (solid lines) components of the ground reaction force (GRF) (a) coloured by body mass subsets (small 17.6±2.96 kg, medium 21.5±0.74 kg, large 24.0±1.46 kg) and (b) coloured by speed subsets (slow 2.52±0.25 ms–1, medium 3.11±0.16 ms–1, fast 3.79±0.27 ms–1).

In (a) and (b), the medial-lateral component of the GRF is not shown as it remained close to zero, as expected for animals moving in a straight-line path. Lower panels show average time-varying effective mechanical advantage (EMA) for the ankle joint subset by (c) body mass and (d) speed.

Figure 2—figure supplement 1
Kinematics of the stride with speed and stance.

(a) Mean vertical and horizontal components of whole body acceleration for kangaroos in the slow, medium, and fast subsets (respectively: 2.52±0.25 ms–1, 3.11±0.16 ms–1, 3.79±0.27 ms–1). (b) Ground contact duration across hopping speeds from current study (black circles) and for red kangaroos reported in Kram and Dawson, 1998 (red circles). Regression equation: tc = 0.342 speed-0.477 where tc is contact duration and s is hopping speed. (c) Relationship between stride length and speed, and (d) stride frequency and speed.

Figure 2—figure supplement 2
Vertical ground reaction force with mass and speed.

(a) Relationship between peak vertical ground reaction force (GRF) as a multiple of body weight (BW) with body mass and (b) with speed.

Dotted line is insignificant and solid line is significant, see Appendix 1—table 2 for interaction.

Figure 2—figure supplement 3
Peak vertical ground reaction force (GRF) plotted against tendon stress (Β=0.080, SE = 0.009, p<0.001, R2=0.486).
Figure 3 with 2 supplements
Average time-varying crouch factor (see Figure 1a) of the kangaroo hindlimb grouped by (a) body mass and (c) speed.

Position of the limb segments during % stance intervals (b). Average time-varying joint angles for the hip (solid lines) and knee (dashed lines) displayed for kangaroos grouped by (d) body mass and (e) speed. Average time-varying joint angles for the ankle (solid lines) and metatarsophalangeal (MTP) joints (dashed lines) displayed for kangaroos grouped by (f) body mass and (g) speed. For (f–g), increased plantarflexion represents a decrease in joint flexion, while increased dorsiflexion represents increased flexion of the joint. Body mass subsets: small 17.6±2.96 kg, medium 21.5±0.74 kg, large 24.0±1.46 kg. Speed subsets: slow 2.52±0.25 ms–1, medium 3.11±0.16 ms–1, fast 3.79±0.27 ms–1.

Figure 3—figure supplement 1
Average time-varying gastrocnemius and plantaris muscle moment arm, r, grouped by (a) body mass and (b) speed; external moment arm to the ankle, R, grouped by (c) body mass, and (d) speed.

Vertical displacement of the ankle marker from the ground throughout stance grouped by (e) body mass and (f) speed. Ankle angles and corresponding r arm length (g). Length of the r and R moment arms at midstance at different speeds (h). Body mass subsets: small 17.6±2.96 kg, medium 21.5±0.74 kg, large 24.0±1.46 kg. Speed subsets: slow 2.52±0.25 ms–1, medium 3.11±0.16 ms–1, fast 3.79±0.27 ms–1.

Figure 3—figure supplement 2
Average time-varying net joint moments (dimensionless, as moments were divided by body weight * leg length) for the hip (solid lines) and knee (dotted lines) displayed for kangaroos grouped by (a) body mass and (b) speed.

Average time-varying net joint moments (dimensionless) for the ankle (solid lines) and metatarsophalangeal (MTP; dotted lines) joints displayed for kangaroos grouped by (c) body mass and (d) speed. Data for tammar wallabies was also included (McGowan et al., 2005) in green. Peak ankle moment occurred at 47.37±4.91% of the stance phase. Positive values represent extensor moments and negative values represent flexor moments. Body mass subsets: small 17.6±2.96 kg, medium 21.5±0.74 kg, large 24.0±1.46 kg. Speed subsets: slow 2.52±0.25 ms–1, medium 3.11±0.16 ms–1, fast 3.79±0.27 ms–1.

EMA with stress and mass.

(a) Relationship between ankle effective mechanical advantage, EMA, at midstance and Achilles tendon stress (stress = 11.6 EMA-1.04, R2=0.593) (black), with other mammals (green). (b) Scaling of mean ankle EMA at midstance for each individual kangaroo against body mass (black), with data for a wider range of macropods (purple) (Bennett and Taylor, 1995), and other mammals (green, EMA = 0.269 M0.259, shaded area 95% confidence interval) (Biewener, 1990) shown.

Time-varying joint powers.

Average time-varying joint powers for the hip (a, b), knee (c, d), ankle (e, f), and MTP (g, h) displayed for kangaroos grouped by body mass (a, c, e, g) and speed (b, d, f, h). Power in all panels is set to the same scale. Body mass subsets: small 17.6±2.96 kg, medium 21.5±0.74 kg, large 24.0±1.46 kg. Speed subsets: slow 2.52±0.25 ms–1, medium 3.11±0.16 ms–1, fast 3.79±0.27 ms–1.

Figure 6 with 3 supplements
Variation with speed of (a) positive and negative ankle work, and (b) net ankle work per hop.
Figure 6—figure supplement 1
Positive (purple) and negative (green) joint work over stance for the hip, knee, ankle, and metatarsophalangeal (MTP) plotted against body mass (a, c, e, g) and speed (b, d, f, h).

Solid lines represent significant trends, dotted lines are not significant (see Appendix 1—table 6).

Figure 6—figure supplement 2
Net joint work for the hip, knee, ankle, and metatarsophalangeal (MTP) joint over stance plotted against body mass (a, c, e, g) and speed (b, d, f, h).

Solid lines represent significant trends, dotted lines are not significant (see Appendix 1—table 6).

Figure 6—figure supplement 3
Ankle work with EMA at midstance.

Negative (a) (Β=−3.04, SE=0.75, p<0.001, R2=0.155), positive (b) (Β=−7.42, SE=0.61, p<0.001, R2=0.622), and net ankle work (c) (Β=−4.37, SE=0.84, p<0.001, R2=0.230) plotted against effective mechanical advantage (EMA) at 50% of stance.

How the relationship between posture and speed is proposed to change tendon stress.

Forces are not to scale and joint angles are exaggerated for illustrative clarity. A slow hop (left panel) compared to a fast hop (right panel). The increase in ground reaction force (GRF) with speed, while a more crouched posture changes the muscle moment arm, r, and external moment arm, R, which allows the ankle to do more negative work (storing elastic potential energy in the tendons due to greater tendon stresses), without increasing net work, and thereby metabolic cost. Ankle moment was calculated by OpenSim and includes inertial terms.

Tables

Appendix 1—table 1
Stride parameter multiple linear regression results as slopes, standard errors, and p-values.

Models with a significant interaction are displayed in full, and as a simplified model without the interaction term included (marked *). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

InteractionBody massSpeedR2
βSEPβSEPβSEP
Maximum vertical acceleration (ms–2)–1.190.5670.0382.721.640.10032.512.50.0110.190
Maximum vertical acceleration (ms–2)*–0.6730.2940.0246.321.600.0000.152
Minimum vertical acceleration (ms–2)0.2210.2080.290–0.2681.130.8140.012
Maximum horizontal acceleration (ms–2)–0.0360.2960.9030.1591.610.9220.000
Minimum horizontal acceleration (ms–2)0.4070.3700.275–6.052.020.0030.087
Contact duration (ms)2.870.3930.000–34.22.120.0000.735
Stride length (m)0.0140.0040.0010.3760.0200.0000.815
Stride frequency (Hz)0.0220.0080.007–0.0820.0230.001–0.3920.1800.0320.303
Stride frequency (Hz)*–0.0190.0040.0000.1020.0230.0000.245
Appendix 1—table 2
Ground reaction force and centre of pressure (CoP) multiple linear regression results as slopes, standard errors, and p-values.

Models with a significant interaction are displayed in full, and as a simplified model without the interaction term included (marked *). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

InteractionBody massSpeedR2
βSEPβSEPβSEP
Normalised peak GRF (BW)–0.0550.0240.0260.1110.0700.1171.340.5350.0140.172
Normalised peak GRF (BW)*–0.0450.0130.0010.1420.0680.0400.128
Peak vertical GRF (N)–11.55.310.03247.915.40.0022811170.0190.332
Peak vertical GRF (N)*15.02.760.00028.414.90.0600.299
Peak braking GRF (N)4.872.040.019–14.85.900.014–13045.00.0050.218
Peak braking GRF (N)*–0.9171.070.392–23.25.760.0000.172
Peak propulsive GRF (N)2.030.8180.01521.54.420.0000.285
CoP location at midstance (mm)–0.1231.540.937–15.28.340.0710.036
CoP location at midstance corrected for phalanx size (mm)–0.43717.00.980–62.791.90.4970.005
Appendix 1—table 3
Crouch factor (CF) and kinematics multiple linear regression results as slopes, standard errors, and p-values.

Models with a significant interaction are displayed in full, and as a simplified model without the interaction term included (marked *). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

InteractionBody massSpeedR2
βSEPβSEPβSEP
 Maximum CF–2.191.070.043–15.85.740.0070.122
Minimum CF–2.450.8850.007–1.534.760.7490.064
Change in CF0.2560.6610.699–14.23.550.0000.129
Pelvis pitch ROM (deg)0.9350.2980.002–2.600.8620.003–19.96.580.0030.100
Pelvis pitch ROM (deg)*0.0660.1590.6770.5340.8580.5350.008
Hip ROM (deg)–0.4880.2120.0240.4901.150.6700.052
Minimum hip flexion (deg)–0.6550.3150.0400.7031.700.6810.043
Maximum hip flexion (deg)–0.1670.2600.5200.2131.400.8800.004
Knee ROM (deg)–1.310.5200.0132.881.500.05828.611.50.0140.154
Knee ROM (deg)*–0.8500.2720.002–0.1201.470.9350.098
Minimum knee flexion (deg)–1.720.6490.0103.761.880.04839.514.30.0070.162
Minimum knee flexion (deg)*–1.130.340.0011.951.840.2940.101
Maximum knee flexion (deg)–0.2770.2650.2992.071.430.1520.026
Ankle ROM (deg)1.020.1660.0001.630.8990.0730.339
Peak ankle plantarflexion (deg)–0.1730.2400.474–3.871.300.0040.104
Peak ankle dorsiflexion (deg)–1.190.1980.000–5.491.070.0000.466
MTP ROM (deg)–0.0980.2590.7077.161.400.0000.219
Peak MTP plantarflexion (deg)0.8750.3060.0055.641.650.0010.216
Peak MTP dorsiflexion (deg)0.9730.2210.000–1.521.200.2050.166
Appendix 1—table 4
Multiple linear regression results of dimensionless peak joint moments as slopes, standard errors, and p-values.

Models with a significant interaction are displayed in full, and as a simplified model without the interaction term included (marked *). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

InteractionBody massSpeedR2
βSEPβSEPβSEP
Hip extensor moment–0.0200.0060.0010.0490.0180.0070.5250.1360.0000.268
Hip extensor moment*–0.0090.0030.0100.0790.0180.0000.184
Knee extensor moment0.0000.0010.7660.0030.0080.7210.003
Knee flexor moment0.0200.0050.000–0.0480.0150.002–0.4870.1160.0000.264
Knee flexor moment*0.0080.0030.007–0.0600.0150.0000.158
Ankle extensor moment–0.0040.0040.2560.0430.0200.0360.048
MTP extensor moment–0.0010.0020.7670.0000.0130.9860.001
Appendix 1—table 5
Tendon stress and effective mechanical advantage (EMA) multiple linear regression results as slopes, standard errors, and p-values.

Models with a significant interaction are displayed in full, and as a simplified model without the interaction term included (marked *). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

InteractionBody massSpeedR2
βSEPβSEPβSEP
r at midstance (mm)–0.0630.0880.477–1.880.4740.0000.173
R at midstance (mm)3.491.030.001–0.935.590.8690.117
EMA at midstance–6.641.980.001–11.010.70.3100.142
Peak tendon stress (MPa)1.030.3850.0085.612.080.0080.168
Normalised peak tendon stress–0.0480.0180.0080.2580.0960.0080.107
Peak tendon stress timing % stance–0.1510.1540.328–3.130.8310.0000.159
Ankle height from ground (mm)–0.2980.7060.674–23.03.810.0000.295
Appendix 1—table 6
Joint net positive, negative and net work simple linear regression (lm(joint work ~mass), lm(joint work ~speed)) results as slopes, standard errors, and p-values.

Work is normalised by body mass (BM). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

Body massSpeed
βSEPR2βSEPR2
Hip pos–0.0100.0080.2380.0140.0300.0440.4970.005
Hip neg–0.0270.0050.0000.225–0.0580.0310.0660.034
Hip net0.0180.0070.0180.0550.0870.0410.0340.045
Knee pos–0.0210.0110.0520.0380.1450.0570.0130.061
Knee neg–0.0040.0040.2670.013–0.0460.0200.0260.050
Knee net–0.0170.0120.1690.0190.1910.0640.0030.084
Ankle pos0.0590.0190.0030.0870.4780.0970.0000.197
Ankle neg0.0220.0170.2000.0170.3210.0870.0000.122
Ankle net0.0370.0170.0370.0440.1560.0950.1020.027
MTP pos–0.0030.0080.7430.001–0.0460.0430.2860.012
MTP neg0.0230.0140.0890.0290.1490.0730.0440.041
MTP net–0.0260.0120.0350.045–0.1940.0640.0030.086
Appendix 1—table 7
Positive, negative and net joint work multiple linear regression results as slopes, standard errors, and p-values.

Work is normalised by body mass (BM). Models with a significant interaction are displayed in full, and as a simplified model without the interaction term included (marked *). The fit of the model is represented by R2 and relationships are considered significant at p<0.05.

Joint work (Jkg–1 BM)InteractionBody massSpeedR2
βSEPβSEPβSEP
Hip positive0.0460.0450.307–0.0120.0080.1610.025
Hip negative–0.0210.0290.472–0.0260.0050.0000.229
Hip net0.0670.0420.1100.0150.0080.0580.080
Knee positive–0.0720.0200.0001.7660.4310.0000.1750.0570.0030.241
Knee positive*0.1870.0570.002–0.0300.0110.0060.133
Knee negative–0.0430.0210.045–0.0020.0040.5700.053
Knee net–0.0730.0220.0021.8180.4910.0000.1790.0640.0070.219
Knee net*0.2300.0640.001–0.0280.0120.0210.133
Ankle positive0.4240.0990.0000.0390.0180.0380.232
Ankle negative–0.0800.0320.0152.0520.7070.0050.2340.0930.0130.176
Ankle negative*0.3110.0910.0010.0070.0170.6710.123
Ankle net0.1220.0330.000–2.5510.7320.001–0.3150.0960.0010.173
Ankle net*0.1120.0970.2500.0310.0180.0840.057
MTP positive–0.0450.0440.3120.0000.0080.9560.012
MTP negative0.1250.0750.1010.0170.0140.2170.056
MTP net–0.1700.0660.011–0.0180.0120.1490.106
Appendix 1—table 8
The mean and standard deviation of joint work for all trials.

Positive, negative, and net work is presented for each joint.

Joint work (Jkg–1 BM)MeanSD
Hip positive0.380.246
Hip negative0.1870.178
Hip net0.1930.235
Knee positive0.4320.334
Knee negative0.1040.117
Knee net0.3280.375
Ankle positive1.990.613
Ankle negative1.3240.525
Ankle net0.6660.542
MTP positive0.2940.242
MTP negative0.6520.42
MTP net–0.3580.377

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  1. Lauren Thornton
  2. Taylor Dick
  3. John R Hutchinson
  4. Glen A Lichtwark
  5. Craig P McGowan
  6. Jonas Rubenson
  7. Alexis Wiktorowicz-Conroy
  8. Christofer J Clemente
(2025)
Postural adaptations may contribute to the unique locomotor energetics seen in hopping kangaroos
eLife 13:RP96437.
https://doi.org/10.7554/eLife.96437.3