| Literature DB >> 34276417 |
Marcel Lemire1,2,3, Mathieu Falbriard4, Kamiar Aminian4, Grégoire P Millet5, Frédéric Meyer5,6.
Abstract
The aim of this study was first to determine if level, uphill, and downhill energy cost of running (ECR) values were correlated at different slopes and for different running speeds, and second, to determine the influence of lower limb strength on ECR. Twenty-nine healthy subjects completed a randomized series of 4-min running bouts on an instrumented treadmill to determine their cardiorespiratory and mechanical (i.e., ground reaction forces) responses at different constant speeds (8, 10, 12, and 14 km·h-1) and different slopes (-20, -10, -5, 0, +5, +10, +15, and +20%). The subjects also performed a knee extensor (KE) strength assessment. Oxygen and energy costs of running values were correlated between all slopes by pooling all running speeds (all r 2 ≥ 0.27; p ≤ 0.021), except between the steepest uphill vs. level and the steepest downhill slope (i.e., +20% vs. 0% and -20% slopes; both p ≥ 0.214). When pooled across all running speeds, the ECR was inversely correlated with KE isometric maximal torque for the level and downhill running conditions (all r 2 ≥ 0.24; p ≤ 0.049) except for the steepest downhill slope (-20%), but not for any uphill slopes. The optimal downhill grade (i.e., lowest oxygen cost) varied between running speeds and ranged from -14% and -20% (all p < 0.001). The present results suggest that compared to level and shallow slopes, on steep slopes ~±20%, running energetics are determined by different factors (i.e., reduced bouncing mechanism, greater muscle strength for negative slopes, and cardiopulmonary fitness for positive slopes). On shallow negative slopes and during level running, ECR is related to KE strength.Entities:
Keywords: biomechanics; energy cost; ground reaction forces; muscle strength; running gait; treadmill
Year: 2021 PMID: 34276417 PMCID: PMC8281813 DOI: 10.3389/fphys.2021.697315
Source DB: PubMed Journal: Front Physiol ISSN: 1664-042X Impact factor: 4.566
Cardiorespiratory and biomechanical parameters by pooling all running speeds.
| N | 21 | 29 | 26 | 29 | 26 | 29 | 16 | 6 |
| Corrected | 26.5 ± 4.4 | 28.8 ± 3.5 | 32.5 ± 3.0 | 39.9 ± 3.5 | 47.1 ± 4.4 | 53.6 ± 4.0 | 58.2 ± 9.3 | 67.5 ± 4.2 |
| Respiratory exchange ratio (%) | 0.77 ± 0.05 | 0.78 ± 0.03 | 0.81 ± 0.04 | 0.86 ± 0.05 | 0.90 ± 0.06 | 0.94 ± 0.03 | 0.95 ± 0.06 | 1.00 ± 0.03 |
| VE (l· | 56.0 ± 9.3 | 54.8 ± 9.4 | 60.2 ± 10.1 | 73.1 ± 13.3 | 86.5 ± 16.7 | 100.1 ± 17.9 | 107.4 ± 20.7 | 120.4 ± 18.9 |
| RF (breaths· | 46 ± 10 | 39 ± 7 | 37 ± 7 | 36 ± 8 | 39 ± 8 | 41 ± 9 | 39 ± 7 | 40 ± 7 |
| HR (bpm) | 133 ± 17 | 129 ± 20 | 132 ± 16 | 144 ± 19 | 156 ± 14 | 167 ± 15 | 169 ± 12 | 174 ± 10 |
| b[La] (mmol· | − | − | 3.0 ± 1.5 | 3.5 ± 1.2 | 4.3 ± 2.4 | 5.2 ± 1.6 | 5.6 ± 3.0 | 7.5 ± 1.9 |
| RPE | 10 ± 2 | 9 ± 1 | 9 ± 2 | 11 ± 2 | 12 ± 2 | 14 ± 1 | 15 ± 2 | 16 ± 2 |
| Step length (cm) | 116 ± 10 | 112 ± 7 | 113 ± 6 | 112 ± 6 | 104 ± 11 | 93 ± 8 | 86 ± 9 | 82 ± 3 |
| Step frequency (Hz) | 2.76 ± 0.10 | 2.70 ± 0.11 | 2.72 ± 0.12 | 2.76 ± 0.11 | 2.76 ± 0.14 | 2.79 ± 0.13 | 2.79 ± 0.13 | 2.71 ± 0.09 |
| Contact time (ms) | 255 ± 29 | 273 ± 25 | 275 ± 24 | 274 ± 25 | 285 ± 27 | 298 ± 29 | 301 ± 25 | 322 ± 12 |
| Aerial time (ms) | 107 ± 32 | 98 ± 21 | 95 ± 18 | 89 ± 20 | 78 ± 17 | 62 ± 20 | 58 ± 22 | 48 ± 12 |
| Fz (N) | 1,467 ± 225 | 1,438 ± 232 | 1,430 ± 243 | 1,409 ± 252 | 1,347 ± 240 | 1,259 ± 193 | 1,206 ± 193 | 1,194 ± 106 |
| Δy (cm) | 6.3 ± 0.6 | 6.6 ± 0.5 | 6.5 ± 0.5 | 6.2 ± 0.5 | 6.1 ± 0.6 | 5.8 ± 0.5 | 5.7 ± 0.7 | 5.9 ± 0.6 |
Values are means ± SD, corrected oxygen uptake (corrected
) indicate a statistically significant difference vs. all other conditions,
vs. 0% slope, and
vs. −20% slope (p < 0.05).
Figure 1Energy cost of running relationships between level running (LR) and downhill (DR) (A), between LR and uphill running (UR) (B) and between UR and DR (C). Each point represents a speed averaged ECR of a given subject who sustained the exercise at same (absolute) slope value ↓±5%, υ±10%, υ+15% and υ±20%; † indicate a statistically significant correlation (p < 0.05).
Figure 2Metabolic and cardiorespiratory responses in inclined running. The energy cost (A), the heart rate (B), the pulmonary ventilation (C), the respiratory frequency (D), and the tidal volume (E) of running at different speeds (▴ 8 km·h−1, υ 10 km·h−1, • 12 km·h−1, ■ 14 km·h−1, ■ By pooling all speeds) and slopes. For energy cost, fixed effects are calculated by pooling all speeds: slope effect: p < 0.001, speed fixed: p = 0.006, slope*speed interaction effect: p = 0.180. SD has been omitted for clarity. Panel (F) shows the ratio of inspiration time (Ti in black) and breathing duty cycle time as a function of treadmill slope. Error bars show SD; #p < 0.05 vs. 0% slope; $p < 0.05 vs. −20% slope.
Regression coefficients and optimum treadmill slope for each running speed.
| 8 | 199.44 | 8.9189 | 0.2657 | −0.0024 | 0.998 | −14.09 |
| 10 | 190.56 | 8.913 | 0.2686 | 0.0007 | 0.998 | −17.84 |
| 12 | 187.8 | 8.9383 | 0.2639 | 0.0005 | 0.996 | −17.84 |
| 14 | 192.24 | 8.9895 | 0.2283 | −0.00009 | 0.998 | −19.46 |
The regression coefficients are for the equation C = a + bi + ci.
indicate a statistically significant difference vs. 10 and 12 km·h.
Figure 3Relationships between the knee extensor torque and the energy cost of running in level (LR) (A), downhill (DR) (B) and uphill running (UR) (C). Symbols “+” for 0%, ↓ for ±5%, υ for ±10%, υ for +15% and υ for ±20%; † indicate a statistically significant correlation (p < 0.05).