Literature DB >> 35757897

Oxygen uptake kinetics and ventilatory and metabolic parameters do not differ between moderate-intensity front crawl and breaststroke swimming.

Mitch Lomax1, Joshua T Royal1, Jernej Kapus2, Heather Massey1, Zoe Saynor1.   

Abstract

Pulmonary oxygen uptake ( V ̇ O 2 ) kinetics have been well studied during land-based exercise. However, less is known about V ̇ O 2 kinetics during swimming exercise and comparisons between strokes is non-existent. We aimed to characterize and compare the V ̇ O 2 kinetics, ventilatory,e and metabolic response to constant velocity moderate-intensity freely breathing front crawl (FC) and breaststroke (BR) swimming in a swimming flume. These two strokes reflect predominantly upper body versus lower body modes of swimming locomotion, respectively. Eight trained swimmers (4 females, 20 ± 1 years, 1.74 ± 0.06 m; 66.8 ± 6.3 kg) attended 5-6 laboratory-based swimming sessions. The first two trials determined FC and BR V ̇ O 2 max and the ventilatory threshold (VT), respectively, during progressive intensity swimming to the limit of tolerance. Subsequent trials involved counterbalanced FC and BR transitions from prone floating to constant velocity moderate-intensity swimming at 80% of the velocity at VT (vVT), separated by 30-min recovery. Breath-by-breath changes in pulmonary gas exchange and ventilation were measured continuously using a snorkel and aquatic metabolic cart system. The ventilatory and metabolic responses were similar (p > 0.05) between strokes during maximal velocity swimming, however, vVT and maximal velocity were slower (p < 0.05) during BR . During moderate-intensity swimming, V ̇ O 2 kinetics, ventilatory and metabolic parameters were similar (p > 0.05) between strokes. In conclusion, when breathing ad libitum, V ̇ O 2 kinetics during moderate-intensity constant velocity swimming, and ventilatory and metabolic responses during moderate-intensity and maximal velocity swimming, are similar between FC and BR strokes.
© 2022 The Authors. Physiological Reports published by Wiley Periodicals LLC on behalf of The Physiological Society and the American Physiological Society.

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Keywords:  zzm321990 zzm321990 zzm321990 Vzzm321990 ̇zzm321990 zzm321990 zzm321990 Ozzm321990 2zzm321990 zzm321990 zzm321990 kinetics; flume; muscle metabolism; swimming

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Year:  2022        PMID: 35757897      PMCID: PMC9234746          DOI: 10.14814/phy2.15361

Source DB:  PubMed          Journal:  Physiol Rep        ISSN: 2051-817X


INTRODUCTION

Pulmonary oxygen uptake () kinetics have been widely studied during land‐based exercise to provide insight into the instantaneous rate of energy transfer, substrate utilization and the tolerable duration of exercise (Burnley & Jones, 2007). Only relatively recently have technological advancements led to the development of aquatic‐specific metabolic carts or attachments (e.g., MetaSwim by Cortex, Aquatrainer by Cosmed). This has permitted the examination of kinetics during swimming and a more detailed examination of the components of ventilation during this mode of exercise. Since these developments, studies have compared the impact of exercise intensity (Pelarigo et al., 2017; Sousa et al., 2013, 2014), sex (Reis et al., 2017), fitness level (Reis et al., 2012a), and time‐trial performance (Reis et al., 2012b) on kinetics during front crawl (FC) swimming. These studies have greatly elucidated the pulmonary kinetic responses to FC in trained swimmers. For example, it has been shown that as swimmers transition from moderate‐intensity exercise (equivalent to 80% of the ventilatory threshold: VT) to heavy‐intensity (Δ25% i.e., VT + 0.25*(maximal  − VT)) the primary time constant (τp) and primary time delay (TDp) shorten or remain unchanged (Reis et al., 2017). The τp is limited by the rate of skeletal muscle oxidative metabolism (Barstow et al., 1990; Pringle et al., 2003) and represents the time taken to achieve 63% of the change in (Jones & Poole, 2005a). Reis et al. (2012b) have shown that the τp is positively correlated with the time taken to complete 400 m FC swimming during transitions to both heavy (Δ25%) and severe (Δ70%) exercise. The τ p does not appear to differ between male and female swimmers, at least not during moderate‐ and heavy‐intensity FC swimming, although the absolute amplitude of the primary component (A p) may be higher in males (Reis et al., 2017). Importantly, swimmers who demonstrate a shorter τ p and TDp may be better able to minimize the slow component amplitude (A s) (Pelarigo et al., 2017). This is important as the A s reflects an increase in type‐II muscle fiber recruitment and, in turn, enhanced metabolic inefficiency (Jones et al., 2011). It has been shown that an inverse correlation exists between VT and the A s meaning that the faster the FC velocity at the VT, the smaller the A s will be (Reis et al., 2012a). To date, however, the investigation of kinetics during swimming has focused only on FC; only one other study has examined kinetics during BR but they focused solely on the mathematical modeling of the slow component (Oliveira et al., 2016). The contribution made to propulsion by the upper body and lower body differs between swimming strokes. Despite being whole‐body strokes, the upper body contributes more than the lower body during FC, but this is reversed during breaststroke (BR) (Bartolomeu et al., 2018; Holmér, 1972). Consequently, FC and BR reflect different modes of locomotion during swimming exercise. Whether or not such differences influence the kinetic responses is unknown and warrants further investigation. The primary aim of the present study was therefore to characterize the kinetic response during moderate‐intensity upper (FC) and lower (BR) body dominant modes of swimming locomotion. A secondary aim was to compare the ventilatory and metabolic responses to moderate‐intensity and maximal velocity FC and BR flume swimming. We hypothesized that when a snorkel was used to permit ad libitum breathing, and hence remove the stroke‐induced constraint to breathing, kinetics, and the ventilatory and metabolic responses would be similar between FC and BR flume swimming despite the different modes of swimming locomotion.

MATERIALS AND METHODS

Experimental approach to the problem

Trained swimmers attended the swimming flume laboratory on five or six occasions for experimental testing. Following familiarization with the swimming flume and equipment, the first two trials were used to determine FC and BR‐specific , respectively. The subsequent three or four experimental trials consisted of one FC and one BR constant velocity moderate‐intensity swim per trial, separated by 30 min seated rest. Each swim consisted of a transition from 3 min of prone floating to 6 min of constant work rate exercise at an intensity equivalent to 80% of the velocity at VT (vVT). While six‐minute constant velocity, moderate‐intensity FC, and BR swimming step transitions have little applicability to swimming performance per se, this duration is consistent with that adopted in the wider kinetics literature and the choice of strokes permits a comparison between predominantly upper versus lower body modes of swimming locomotion. All testing took place in a swimming flume (SwimEx, 600‐T, USA) housed in a climatically controlled chamber (water temperature: 29.9 ± 0.3°C; air temperature: 24.0 ± 0.3°C: barometric pressure: 760.8 ± 4.4 mmHg; humidity: 78.8 ± 6.3%). Breath‐by‐breath changes in pulmonary gas exchange and ventilation were measured continuously throughout each trial using a snorkel connected to an aquatic metabolic cart (MetaSwim, Cortext, Germany) with a total dead space (mouthpiece, snorkel, volume flow sensor and splash water protector) of 222 ml. This approach permitted the assessment of stroke‐specific , at VT, percentage at VT, vVT, peak minute ventilation ( Epeak), peak carbon dioxide output (), peak respiratory exchange ratio (RERpeak), peak tidal volume (TVpeak), and peak f (f ) values between maximal intensity FC and BR swimming. It also allowed the end‐tidal partial pressures of O2 and CO2 (PETO2 and PETCO2, respectively), inspiratory and expiratory time (TI and TE, respectively) and the proportion of the total breath cycle time spent in inspiration (TI/TTOT) to be assessed during maximal swimming. Finally, the constant velocity swims permitted the relevant O2 kinetic parameters (τ p, TDp, A p, mean response time [MRT]) and various ventilatory ( E, TV, f , PETO2, and PETCO2, TI, TE, TI/TTOT) and metabolic (, , RER) parameters to be measured during moderate‐intensity FC and BR swimming. This study was undertaken in accordance with the principles of the Declaration of Helsinki.

Participants

Eight (4 females) trained swimmers (age: 20 ± 1 year; stature: 1.74 ± 0.06 m; body mass: 66.8 ± 6.3 kg) volunteered for this study. All undertook at least 6 h of swim training per week and competed at national university level. All provided fully informed written consent (which also acknowledged that they cannot be identified in the paper and that their data is fully anonymized) and institutional ethics approval was received before the start of the study.

Protocol

and VT determination

After a separate swimming flume and equipment familiarization session, swimmers completed two progressive velocity swimming tests to the limit of tolerance (Tlim) to determine on separate days: 1 FC and 1 BR. Each progressive velocity swimming test was followed by a verification test 15 min later. Both incremental tests, for the determination of , began with a 3 min baseline period during which participants remained stationary in a prone position in the flume. This was followed by a 3 min warm‐up and then progressive‐intensity swimming test until Tlim (starting velocity of 1.00 ± 0.11 m s−1 for FC and 0.81 ± 0.04 m s−1 for BR). At the end of each 2 min stage, velocity was increased 0.05–0.1 m s−1 until Tlim. Subsequently, swimmers undertook a 5 min cool down at warm‐up velocity, followed by 10 min of seated passive rest outside of the water. Swimmers then completed a supramaximal constant‐velocity test to verify . A 3 min warm‐up preceded a step transition to 105% of the final velocity achieved during the progressive velocity test to Tlim (Lomax et al., 2019). The highest 10 s average value achieved during either the or verification test was taken to represent . Epeak, , RERpeak, TVpeak, and f were taken from the or verification test, whichever elicited the highest . Additionally, PETO2, PETCO2, TE, TI, and TI/TTOT observed during maximal exercise (i.e., coinciding with ) were also reported. The VT during FC and BR was identified from the respective tests using the V‐slope method. This was verified using the ventilatory equivalents for O2 and CO2 and the partial pressure end‐tidal O2 and CO2 methods by two independent observers trained in the technique (Beaver et al., 1986; Lomax et al., 2019). The VT during FC and BR tests was used to determine the velocity of all subsequent FC and BR 6 min constant velocity swims (Lomax et al., 2019).

Constant velocity swims and analysis of kinetics

Swimmers completed 3 or 4 FC and BR constant velocity swimming trials. One FC and 1 BR swim were completed per trial. The order of the swims was counterbalanced between participants and within trials. Each swim consisted of 3 min of prone floating (baseline), 6 min of constant velocity swimming at 80% vVT and 6 min of prone floating (recovery). A 30 min seated rest then separated the end of the first swim and the start of the next swim. from each swim per stroke and per repeat trial was first blinded and a 5‐breath moving average was used to identify outliers: With any breath greater than 2.5 standard deviations from the moving average removed. The remaining data per stroke and trial were then linearly interpolated to 1 s, time‐aligned to the start of the 6 min swim (t = 0 s) and ensemble averaged. As the cardiodynamic phase is typically 15–20 s in length, the first 15 s from the onset of exercise were visually identified and omitted to remove this phase from analysis (Breese et al., 2019). The phase II monoexponential portion of the response was then characterized using the following equation (GraphPad Prism) adapted from Jones and Poole (2005b). where is the absolute at a given time in s, Δ is the change in amplitude from baseline, TD is the time delay in s and τ is the time constant. The MRT was derived to define the overall kinetics during FC and BR by constraining TD to 0 s and fitting from the start of the 6 min swim. The entire kinetic response was expressed both in absolute terms and relative to by stroke. As a plateau was observed in the second half of each swim (minutes 3–6), E, TV, f r, , RER, PETO2, PETCO2, TI, TE, and TI/TTOT were averaged per stroke. The mean of each swim was then averaged across all trials to give a single value for each stroke. We have shown previously that the test‐re‐test coefficient of variation for , , E, TV, f , PETO2, and PETCO2 during moderate‐intensity FC flume swimming is 2.8%–8.5% (6.2% for ) when using the MetaSwim metabolic cart (Lomax et al., 2019).

Data analysis

Normality of data were assessed using Shapiro–Wilks tests. Paired samples t‐tests assessed for differences in all parameters between FC and BR with the exception that Wilcoxon Signed‐Rank tests were used to compare absolute and relative and vVT during maximal velocity FC and BR swimming, and relative , f and RER during constant velocity swimming. Additionally, Spearman's rho was used to assess for a correlation between and τ p per stroke and Pearson's r to assess for a correlation between τ p and maximal velocity per stroke. Effects sizes were calculated using Cohen's d for parametric data with an effect size of 0.2 deemed small, 0.6 moderate, 1.2 large, 2.0 very large and 4.0 extremely large (Hopkins et al., 2009). For non‐parametric data, r was used, whereby r is the z score divided by the square root of the total number of observations. A value of 0.1 was deemed small, 0.3 moderate, and 0.5 and above large (Field, 2013). Effect sizes less than small were reported as no effect. Unless otherwise stated, data are presented as mean and standard deviation (SD).

RESULTS

, at VT, percentage of at VT, Epeak, . RERpeak, and f were similar (p > 0.05) between maximal velocity FC and BR. Similarly, PETO2, PETCO2, TE, TI and TI/TTOT at maximal exercise were similar (p > 0.05) between strokes (Table 1). In contrast, both vVT (z = −2.214, p = 0.03) and maximal velocity (t = 7.000, p < 0.001) were faster in FC (Table 1).
TABLE 1

Ventilatory and metabolic data in response to maximal FC and BR swimming: Group mean ± SD

VariableFCBREffect size
V˙O2max (L min‐1)3.78 ± 0.893.36 ± 0.78Small effect
V˙O2max (ml−1 kg−1 min−1)54.12 ± 13.3750.62 ± 12.20Small effect
V˙O2 at VT (L min−1)1.97 ± 0.831.90 ± 0.59No effect
Percentage V˙O2max at VT53 ± 1257 ± 8Small effect
vVT (m s−1)1.18 ± 0.200.91 ± 0.04* Large effect
Maximal velocity (m s−1)1.60 ± 0.131.35 ± 0.14** Very large
V˙CO2peak (L min−1)3.97 ± 0.943.42 ± 0.96Moderate effect
V˙ Epeak (L min−1)103.8 ± 21.788.9 ± 24.5Moderate effect
TVpeak (L)2.54 ± 0.512.23 ± 0.37Small effect
f rpeak (breaths min−1)46 ± 944 ± 7Small effect
RERpeak 1.11 ± 0.091.14 ± 0.13Small effect
PETO2 (mmHg)110.33 ± 4.48109.18 ± 6.31Small effect
PETCO2 (mmHg)39.73 ± 2.9241.71 ± 4.80Small effect
TI (s)0.80 ± 0.190.90 ± 0.25Small effect
TE (s)0.60 ± 0.110.68 ± 0.17Small effect
TI/TTOT (%)57 ± 557 ± 10No effect

Abbreviations: BR, breaststroke; FC, front crawl; PETCO2, end‐tidal partial pressures of CO2; PETO2, end‐tidal partial pressures of O2; RERpeak, peak respiratory exchange ratio; TE, expiratory time; TI, inspiratory time; TVpeak, peak tidal volume, f , peak f ; , peak carbon dioxide output; Epeak, peak minute ventilation; VT, ventilatory threshold; vVT, velocity at VT.

p ≤ 0.05 different to FC

p ≤ 0.01.

Ventilatory and metabolic data in response to maximal FC and BR swimming: Group mean ± SD Abbreviations: BR, breaststroke; FC, front crawl; PETCO2, end‐tidal partial pressures of CO2; PETO2, end‐tidal partial pressures of O2; RERpeak, peak respiratory exchange ratio; TE, expiratory time; TI, inspiratory time; TVpeak, peak tidal volume, f , peak f ; , peak carbon dioxide output; Epeak, peak minute ventilation; VT, ventilatory threshold; vVT, velocity at VT. p ≤ 0.05 different to FC p ≤ 0.01. The verification tests did not (p > 0.05) result in higher values (FC: 3.48 ± 0.64 L min−1; BR: 3.26 ± 0.86 L min−1) compared with the progressive velocity swimming tests to Tlim (FC: 3.47 ± 0.64 L min−1; BR: 3.36 ± 0.82 L min−1). τp, TDp, A p and MRT were similar (p > 0.05) during moderate‐intensity FC and BR swimming (Table 2; Figure 1). There were no correlations between and τp (FC: rho = −0.024, p = 0.955; BR: rho = −0.381, p = 0.352) or between τp and maximal velocity (FC: r = −0.287, p = 0.491; BR: r = −0.481, p = 0.227) for either stroke. Likewise, all other ventilatory and metabolic parameters were similar (p > 0.05) between moderate‐intensity FC and BR swimming (Table 2).
TABLE 2

Pulmonary kinetics and ventilatory and metabolic data in response to constant velocity moderate‐intensity FC and BR swimming: Group mean ± SD

VariableFCBREffect size
Baseline V˙O2 (L min−1)0.42 ± 0.130.51 ± 0.27Small/moderate
Exercise V˙O2 (L min−1)1.38 ± 0.491.47 ± 0.35Small effect
Exercise V˙O2 (ml−1 kg−1 min−1)20.53 ± 6.7322.13 ± 5.50Small effect
τp (s)24.44 ± 7.3027.37 ± 9.12Small/moderate
TDp (s)18.33 ± 4.9816.27 ± 7.01Small effect
A p (L min−1)1.04 ± 0.430.96 ± 0.22Small effect
MRT (s)41.63 ± 8.5839.94 ± 7.73Small effect
V˙O2 (L min−1)1.22 ± 0.431.26 ± 0.33No effect
V˙ E (L min−1)32.0 ± 10.334.8 ± 8.3Small effect
TV (L)1.87 ± 0.291.83 ± 0.25No effect
f r (breaths min−1)18 ± 520 ± 5Small effect
RER0.89 ± 0.040.86 ± 0.05Moderate effect
PETO2 (mmHg)102.28 ± 4.70101.48 ± 7.20No effect
PETCO2 (mmHg)40.60 ± 2.7940.03 ± 4.37No effect
TE (s)1.54 ± 0.521.48 ± 0.49No effect
TI (s)2.47 ± 0.971.99 ± 0.81No effect
TI/TTOT (%)59 ± 1354 ± 13Small effect

Abbreviations: BR, breaststroke; FC, front crawl; MRT, mean response time; PETCO2, end‐tidal partial pressures of CO2; PETO2, end‐tidal partial pressures of O2; RER, respiratory exchange ratio; TDP, primary time delay; TV, tidal volume; TE, expiratory time; TI, inspiratory time; , peak carbon dioxide output; E, minute ventilation; VT, ventilatory threshold; vVT, velocity at VT.

FIGURE 1

Baseline corrected group mean response during FC (open circles) and BR (filled circles) constant velocity swimming. Residuals are also shown.

Pulmonary kinetics and ventilatory and metabolic data in response to constant velocity moderate‐intensity FC and BR swimming: Group mean ± SD Abbreviations: BR, breaststroke; FC, front crawl; MRT, mean response time; PETCO2, end‐tidal partial pressures of CO2; PETO2, end‐tidal partial pressures of O2; RER, respiratory exchange ratio; TDP, primary time delay; TV, tidal volume; TE, expiratory time; TI, inspiratory time; , peak carbon dioxide output; E, minute ventilation; VT, ventilatory threshold; vVT, velocity at VT. Baseline corrected group mean response during FC (open circles) and BR (filled circles) constant velocity swimming. Residuals are also shown.

DISCUSSION

As propulsion is achieved predominantly via the upper body in FC and by the lower body in BR (Bartolomeu et al., 2018; Holmér, 1972), these two strokes represent different modes of swimming locomotion. The primary aim of the current study was to characterize and compare the kinetic responses during moderate‐intensity swimming locomotion whereby propulsion was achieved by predominantly the upper body (FC) or the lower body (BR). The secondary aim was to compare the ventilatory and metabolic responses to these two modes of locomotion during moderate‐intensity and maximal velocity swimming. This study is the first to show that when the stroke‐induced differences in fr were removed by use of a snorkel, kinetics were similar during constant velocity, moderate‐intensity FC, and BR flume swimming in trained swimmers. Similarly, so too were the ventilatory and metabolic parameters during maximal velocity and moderate‐intensity FC and BR flume swimming. The FC of our swimmers (54 ml−1 kg−1 min−1) was similar (50–61 ml−1 kg−1 min−1) to that reported by others, but the kinetic response during FC was slower in our swimmers (Pelarigo et al., 2017; Reis et al., 2012a, 2012b, 2017; Sousa et al., 2014). For example, our swimmers had a longer τp, TDp, and MRT during FC, and a smaller A p compared to those undertaking moderate intensity 200, 600 m, and 30 min of FC swimming (Pelarigo et al., 2017; Reis et al., 2017; Sousa et al., 2013). More specifically, when compared to the findings of Reis et al. (2017), who also utilized a swimming velocity equivalent to 80% of VT, the τp of our swimmers was 9–10 s slower. The vVT was also slower (1.18 m s−1 vs. 1.49 m s−1) despite similar values (54 ml−1 kg−1 min−1 vs. 50–58 ml−1 kg−1 min−1), and VT occurred at a much lower percentage of (53 ± 12% vs. ~76%–78%). As the VT is a more sensitive indicator of aerobic conditioning than (Edwards et al., 2003), this suggests that our swimmers were less aerobically conditioned than those in the aforementioned studies; our FC τp data also supports this notion. The slower kinetics of our swimmers could be indicative of less metabolic stability (Grassi et al., 2011). Prior research has suggested that τp is inversely correlated with velocity at during FC swimming but not (Reis et al., 2012a). The present study did not observe any correlations between τp and nor τp and maximal velocity. Nevertheless, as the τ during moderate‐intensity exercise reflects the time taken to achieve steady‐state (Berger et al., 2006), a longer τp would indicate slower cardiovascular and muscular adaptations. This means that a greater length of time would elapse before steady state is achieved (Berger et al., 2006; Sousa et al., 2013) and a larger oxygen deficit would occur (Berger et al., 2006; Burnley & Jones, 2007). This increases both the requirement for anaerobic energy and the production of metabolites (Burnley & Jones, 2007). The longer FC τp observed in the current study therefore, suggests that our swimmers’ cardiovascular and muscular systems ability to adapt to a moderate‐intensity transition was worse than that reported previously, despite similar values (Reis et al., 2017). Although we are unable to delineate the mechanism(s) responsible, this may reflect worse metabolic stability in our swimmers. It has been suggested that kinetics might be a marker of metabolic stability, which improves with endurance training (Grassi et al., 2011). Unfortunately, neither the current study nor that of Reis et al. (2017) provided data to assess this, but differences in the magnitude of ADP, Pi, and PCr concentration changes in relation to could underpin this. For example, metabolic stability would be worse in our swimmers compared to those in the study of Reis et al. (2017) if they experienced a greater fall in PCr concentration and a greater increase in ADP and Pi concentration for a given . Alternatively, metabolic stability would also be worse if was lower but for a similar change in ADP, Pi, and PCr (Grassi et al., 2011). Regardless of the underpinning cause(s), our data indicate that relying solely on as a means of comparing aerobic function between swimmers is limited. If the integrated capacity to transport and utilize oxygen is of interest, kinetics should be included in any evaluation (Burnley & Jones, 2007). When the stroke‐induced differences in f were removed by use of a snorkel, both maximal and submaximal E, TV, , , RER, TI, TE, TI/TTOT, PETO2, PETCO2 were similar between the two modes of swimming locomotion. Likewise, τp, TDp, A p, and MRT were similar between moderate‐intensity FC and BR swimming (Table 2). Cerretteli et al. (1977) have previously shown that kinetics (time taken to reach 50% of the change from baseline to steady state ) are slower during land‐based, supine arm only exercise than supine leg only exercise, indicating that muscle group usage impacts the kinetic responses. However, Cerretelli et al. (1979) went on to show that training specificity is more important than muscle group usage in determining the kinetic response. They found that the on‐kinetics (half time of the on‐response) in trained swimmers and kayakers were faster during supine arm cranking and slower during supine leg peddling, but this pattern was reversed in trained runners. Overall, our data indicate that in trained swimmers, kinetics are similar during moderate intensity, and hence steady‐state, upper body and lower body dominant modes of swimming locomotion when breathing is ad libitum via the use of a snorkel. Likewise, the ventilatory and metabolic parameters are also similar during both steady‐state and maximal velocity freely breathing FC and BR swimming. However, it should be noted that while BR relies more on the legs for propulsion than the arms, and FC relies more on the arms for propulsion than the legs (Bartolomeu et al., 2018; Holmér, 1972), both strokes do require activation of the arms, legs and other musculature throughout the stroke cycle (Maglischo, 1993; Nuber et al., 1986). Unfortunately, logistical and time constraints prevented the inclusion of high‐intensity exercise domains and assessment of butterfly and backstroke; this would have required at least an additional 10 trials per swimmer. Further work is therefore required to confirm whether differences in kinetic parameters exist between strokes at faster velocities. Past studies utilizing the FC stroke have observed a slow component during high‐intensity swimming (Pelarigo et al., 2017; Reis et al., 2012a; Sousa et al., 2013, 2014). Given that the slow component is indicative of muscle inefficiency, which will reduce exercise tolerance (Grassi et al., 2015), any stroke differences will have implications for swimming performance. It should be acknowledged that the use of a snorkel device will add an additional dead space to the breathing circuit compared to a mask or mouthpiece. This means that during inhalation there will be an increase in the amount of re‐inspired CO2. Indeed, it has been shown that wearing a full‐face snorkel increases resting PETCO2 by between 4 and 7 mmHg (Lisker et al. (2020). An increase in external dead space volume will compromise alveolar ventilation and cause arterial hypercapnia unless ventilatory compensation occurs (Ward & Whipp, 1980). Ward and Whipp (1980) showed an upward progressive displacement in the E– relationship during steady‐state incremental cycling exercise as external dead space volume increased from 100 ml through to 1000 ml. McParland et al. (1991) also showed an increase in exercise ventilation with the addition of an external dead space (940 ml). However, they also showed that when ventilation was fixed during both moderate‐intensity (~ E of 67 L min−1) and high‐intensity (~ E of 120 L min−1) cycling exercise, TV increased (moderate‐intensity: 0.24 L; high‐intensity: 0.41 L) and f fell (moderate‐intensity: 2 breaths.min−1; high‐intensity: 5 breaths.min−1) compared with normal breathing conditions. Thus, an increase in external dead space volume can impact both ventilation and its component parts. When translating our findings to a pool environment, it should be noted that the biomechanics of swimming in a flume and the fluid mechanics are different to that of a pool (Guignard et al., 2017). For example, in a swimming flume, the flow of water is directed towards the swimmer and originates from the front of the flume. This pushes the upper limbs backwards and might increase the stroke rate (Guignard et al., 2017; Wilson et al., 1998). Additionally, during flume swimming, the non‐propulsive phases are reduced and the propulsive underwater phases are increased, with the latter aimed at maintaining the correct position in the flume (Guignard et al., 2017); interestingly our swimmers commented that it was harder to maintain the correct position in the flume during BR than FC. Nevertheless, we do not believe that these fluid and biomechanical differences significantly affect the applicability of our findings to a pool setting. In support of this, tethered and untethered flume swimming results in similar and Epeak values, as do pool swimming and tethered flume swimming (Bonen et al., 1980). It is also pertinent to note here that there were no differences (p > 0.05) between the highest observed during the progressive velocity swimming tests to Tlim and the verification tests, regardless of stroke. However, we do still advocate the inclusion of a verification test, as although at a group level there were no differences, some swimmers (three in the case of both FC and BR) did achieve a higher during the verification test. Finally, while terrestrial studies typically identify the intensity domain(s) to be used in kinetic studies by using a combination of physiological parameters (e.g., VT, critical power, ) identified from a physiological stress profile test, this approach is not consistently adopted in swimming. Reis et al. (2012a, 2012b, 2017) did adopt this approach with moderate (80% VT), heavy (Δ25%) or severe (Δ70%) intensity constant velocity swims undertaken in their studies. However, others have based transition intensities on a single parameter such as , maximal lactate steady state, the individual anaerobic threshold, or on race paced velocity (Pelarigo et al., 2017; Sousa et al., 2013, 2014). It remains to be seen if this is a more appropriate approach to adopt in swimming.

CONCLUSION

The impact of swimming locomotion on kinetics, ventilatory, and metabolic parameters in trained swimmers were examined during FC and BR flume swimming. These two strokes were chosen as they represent predominantly upper body (FC) and lower body (BR) modes of propulsion. Furthermore, the use of a snorkel permitted ad libitum breathing thereby removing any stroke‐induced breathing constraint. In this situation, vVT and maximal velocity are slower during BR. However, all other ventilatory and metabolic parameters, including , are similar between the two modes of locomotion during maximal swimming. Likewise, kinetics and both the ventilatory and metabolic responses are similar during fixed velocity moderate‐intensity FC and BR swimming.

ETHICS STATEMENT

This study received ethical approval from the University of Portsmouth, Science Faculty Ethics Committee.

FUNDING INFORMATION

There is no direct funding to report for this study.

CONFLICT OF INTEREST

No conflicts of interest to declare.
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Journal:  Med Sci Sports Exerc       Date:  2009-01       Impact factor: 5.411

Review 3.  Slow component of VO2 kinetics: mechanistic bases and practical applications.

Authors:  Andrew M Jones; Bruno Grassi; Peter M Christensen; Peter Krustrup; Jens Bangsbo; David C Poole
Journal:  Med Sci Sports Exerc       Date:  2011-11       Impact factor: 5.411

4.  Oxygen uptake during swimming in man.

Authors:  I Holmér
Journal:  J Appl Physiol       Date:  1972-10       Impact factor: 3.531

5.  Influence of continuous and interval training on oxygen uptake on-kinetics.

Authors:  Nicolas J A Berger; Keith Tolfrey; Alun G Williams; Andrew M Jones
Journal:  Med Sci Sports Exerc       Date:  2006-03       Impact factor: 5.411

6.  Ventilatory control during exercise with increased external dead space.

Authors:  S A Ward; B J Whipp
Journal:  J Appl Physiol Respir Environ Exerc Physiol       Date:  1980-02

7.  Fine wire electromyography analysis of muscles of the shoulder during swimming.

Authors:  G W Nuber; F W Jobe; J Perry; D R Moynes; D Antonelli
Journal:  Am J Sports Med       Date:  1986 Jan-Feb       Impact factor: 6.202

8.  VO2 kinetics and metabolic contributions whilst swimming at 95, 100, and 105% of the velocity at VO2max.

Authors:  Ana C Sousa; João P Vilas-Boas; Ricardo J Fernandes
Journal:  Biomed Res Int       Date:  2014-06-18       Impact factor: 3.411

9.  The oxygen uptake slow component at submaximal intensities in breaststroke swimming.

Authors:  Diogo R Oliveira; Lio F Gonçalves; António M Reis; Ricardo J Fernandes; Nuno D Garrido; Victor M Reis
Journal:  J Hum Kinet       Date:  2016-07-02       Impact factor: 2.193

Review 10.  Skeletal muscle fatigue and decreased efficiency: two sides of the same coin?

Authors:  Bruno Grassi; Harry B Rossiter; Jerzy A Zoladz
Journal:  Exerc Sport Sci Rev       Date:  2015-04       Impact factor: 6.230

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