ABSTRACT
The human musculoskeletal system is well adapted to use energy-efficient muscle–tendon mechanics during walking and running, but muscle behaviour during on-snow locomotion is unknown. Here, we examined muscle and muscle–tendon unit behaviour during diagonal-style cross-country roller skiing at three speed and incline conditions to examine whether skiers can exploit energy-saving mechanisms of the muscle–tendon unit. We assessed lower leg muscle and muscle–tendon unit mechanics and muscle activity in 13 high-level skiers during treadmill roller skiing using synchronised ultrasound, motion capture, electromyography and ski-binding force measurements. Participants skied using diagonal style at 2.5 and 3.5 m s−1 up 5 deg, and at 2.5 m s−1 up 10 deg. We found an uncoupling of muscle and joint behaviour during most parts of the propulsive kick phase in all conditions (P<0.01). Gastrocnemius muscle fascicles actively shortened ∼0.9 cm during the kick phase, while the muscle–tendon unit went through a stretch–shortening cycle. Peak muscle–tendon unit shortening velocity was 5 times faster than fascicle velocity (37.5 versus 7.4 cm s−1, P<0.01). Steeper incline skiing was achieved by greater muscle activity (24%, P=0.04) and slower fascicle shortening velocity (3.4 versus 4.5 cm s−1, P<0.01). Faster speed was achieved by greater peak muscle activity (23%, P<0.01) and no change in fascicle shortening velocity. Our data show that, during diagonal-style cross-county skiing, muscle behaviour is uncoupled from the joint movement, which enables beneficial contractile conditions and energy utilisation with different slopes and speeds. Active preloading at the end of the glide phase may facilitate these mechanisms.
INTRODUCTION
The human musculoskeletal system is well adapted to the two primary forms of terrestrial locomotion: walking and running (e.g. Arnold and Delp, 2011; Farris and Sawicki, 2012). Both gaits are characterised by ground contact periods where the foot is stationary on the ground, held in place by friction forces. During the ground contact phases of these gaits, elastic energy is stored and released as the muscle–tendon unit (MTU) elongates and shortens, allowing leg muscles to operate at substantially slower velocities than the MTU (Ishikawa et al., 2005; Lichtwark et al., 2007; Lichtwark and Wilson, 2006). Utilisation of elastic energy and the energy-efficient way to generate muscle tension explains why these gaits are metabolically efficient (Fletcher and MacIntosh, 2015). However, this energy-efficient contraction mode is not apparent in all locomotor activities. Recent studies examining muscle behaviour during race walking and rowing showed that fascicles followed the stretch–shortening cycle of the MTU, resulting in less-efficient contractile patterns (Cronin et al., 2016; Held et al., 2022).
Diagonal stride (DIA) is a skiing gait typically used on uphill terrain (Fig. 1). It is a four-limbed gait, where the arms and legs move in opposite phase (i.e. stance on left ski and right pole simultaneously, and vice versa). The arms apply force to the ground through ski poles, but they only comprise a small fraction of the forces generated by the legs (7–8% of the body weight on average over a cycle; Vähäsöyrinki et al., 2008). Similar to running, DIA has in-phase fluctuations of kinetic and gravitational energy (Pellegrini et al., 2014). It has therefore been suggested to be a ‘bouncing gait’, similar to running, which utilizes the MTU’s capacity to store elastic energy. However, DIA lacks the aerial phase seen in running. Instead of an aerial phase, DIA has a glide phase, where the skier glides on one ski as the contralateral leg is in its swing phase. Hence, DIA has been characterized as a form of ‘grounded running’ (Pellegrini et al., 2014). The energy-efficient contraction dynamics seen in running can also appear in these bouncing gaits without aerial phases (i.e. grounded running; Davis et al., 2020; Reinhardt and Blickhan, 2014). However, by analysing fluctuations of mechanical energy, Kehler et al. (2014) concluded that the mechanical energy fluctuations in DIA are most likely dissipated as frictional heat during the glide phase, indicating that the gait might not take advantage of the energy-saving mechanisms of other bouncing gaits. Hence, the term ‘grounded running’ might be an inappropriate description for the gait.
A cycle of the diagonal stride (DIA) technique. For the right leg, the poses show: start kick (A), start swing (B), mid-swing (C), start glide (D), mid-glide (E) and start kick (F).
Nonetheless, joint-level kinematic and kinetic analyses of DIA have shown that the lower leg MTUs undergo a stretch–shortening cycle during the kick phase (Komi and Norman, 1987; Vähäsöyrinki et al., 2008). This suggests that the last part of the glide phase is used to produce pre-tension, stretching elastic tissue by active muscle contraction. A pre-tension during the glide phase could enable similar muscle–tendon behaviour to that in jumping from a still position, where a catapult-like function of the lower leg was observed (Farris et al., 2016; Kurokawa et al., 2001). The stretch–shortening cycle of the MTU described by Komi and Norman (1987) is in line with this reasoning. However, their study could not distinguish between muscle and tendon contributions to joint movement, which hindered conclusions on the muscles' contraction mode. Hence, it is still unclear whether, and how, the DIA technique can exploit energy-saving mechanisms found in bouncing gaits.
In running, muscle contraction velocity is relatively unaffected by changes in running speed, incline or external load (i.e. vertical force). Rather, the main adaptation to increased demand (i.e. speed, incline or vertical load) is increased muscle activation (Farris and Sawicki, 2012; Lichtwark and Wilson, 2006). For DIA, the kick phase duration increases with incline and decreases with speed (Nilsson et al., 2004; Pellegrini et al., 2013). If the pre-tension during the late glide and early kick phase of DIA is initiated by active muscle contraction, it is likely that fascicle contraction velocity and muscle activation will increase with skiing speed, as less time is available for the kick phase. Muscle activation is also likely to increase with incline as greater gravitational forces must be overcome. Fascicle contraction velocity, however, might decrease on steeper inclines because the kick phase duration becomes longer.
The aim this study was to explore gastrocnemius medialis muscle and MTU behaviour during DIA roller skiing, and to investigate the effect of skiing speed and incline on these variables. We hypothesised that during the late glide phase and kick phase, there would be active shortening of the gastrocnemius muscle, while the MTU undergoes a stretch–shortening cycle during the late glide phase and kick phase. Furthermore, with increased speed, we expected greater muscle activation and faster fascicle shortening velocities during the kick phase, due to a shorter kick duration. On steeper inclines, we expected greater muscle activation during the kick but similar fascicle velocity, due to increased kick duration when the resisting force is greater.
MATERIALS AND METHODS
Participants
Thirteen cross-country skiers [8 male and 5 female; mean±s.d. age 26.5±4.8 years, height 179.3±8.0 cm, body mass 72.8±6.2 kg and Fédération Internationale de Ski (FIS) ranking: 107.4±62.7 points] with at least 5 years of competitive experience in cross-country skiing at national or international level, gave written informed consent to participate in the study. All participants were familiar with the use of roller skis on a treadmill. The protocol was approved by the ethics committee of the Norwegian School of Sport Sciences (137-180620).
Experimental protocol
Prior to testing, participants performed 10 min of low-intensity roller skiing on a motorised treadmill used during the whole test session (Rodby, Vänge, Sweden) as a warm-up and to ensure that the roller ski rubber wheels and bearings reached a proper temperature for testing (Ainegren et al., 2008). The roller skis' (IDT Sport classic, Lena, Norway) back and front wheels were interchanged, so that the ratchet wheel was mounted in the front wheel to better mimic on-snow skiing. The participants used ski poles (Swix Triac 3.0, BRAV Norge, Lørenskog, Norway) with special ferrules for use on treadmill surfaces and self-selected length, within official international regulations (FIS, 2020; maximum 83% of body height).
During the test, participants roller skied with the DIA technique at three different conditions with different speeds and inclines: 2.5 m s−1 up a 5 deg incline (DIAref), 3.5 m s−1 up a 5 deg incline (DIAfast) and 2.5 m s−1 up a 10 deg incline (DIAsteep). To avoid confusion, in this study, we use the word speed in reference to the treadmill (which is always positive), whereas velocity is used to describe the rate of different tissue length changes (which is negative for contraction and positive for elongation). Data were recorded twice for each condition for 10 s and each trial lasted for ∼30 s. Ultrasonography, surface electromyography (EMG), force-sensitive resistors (FSRs) under the ski binding and 3D kinematics data were synchronized by a trigger signal. Participants were given 2 min of rest between each trial.
Joint kinematics and MTU length
We used a 12-camera 3D motion capture system (Qualisys 400 and 700 series, Qualisys AB, Gothenburg, Sweden) to record the 3D trajectories of 26 reflective markers (12 mm, Qualisys AB) at 150 Hz. Twelve markers were placed at key anatomical landmarks on the pelvis and the right leg. The pelvis segment and the joints centres of the hip were defined by markers on the right and left anterior–superior and posterior–superior iliac spine (Bell et al., 1989). The knee joint centre was defined as the mid-distance between markers on the medial and lateral epicondyles, and ankle joint centre was defined as the mid-point between the lateral and medial malleoli. To track the foot segment, markers were placed on the calcaneus and the first, second and fifth metatarsal head (these markers were placed on the ski boot, not directly on the skin). The movement of the thigh and shank was tracked with a three-marker cluster positioned midway along these segments. Ankle, knee and hip angles were calculated based on the model described by Robertson et al. (2013) (Visual 3D, C-motion, Germantown, MD, USA). Eight additional reflective markers were placed on relevant sites of the equipment (i.e. at the back and front wheel axle of each roller ski, and one 15 cm below the handle of each pole, and one 60 cm above the tip for each pole). Reference frames for all segments were defined during a static capture where participants stood still holding their arms straight out in front. Marker trajectories were filtered using a second-order lowpass digital zero phase-shift Butterworth filter with a cut-off frequency 15 Hz.
We calculated individual gastrocnemius medialis MTU length based on ankle and knee joint angles along with shank segment length (Hawkins and Hull, 1990). Shank length was defined as the mean distance between the lateral femoral epicondyle and the lateral malleolus of the shank length. MTU velocity was calculated by numerical differentiation of the length.
Muscle fascicle length
Gastrocnemius medialis muscle fascicles were imaged by an ultrasound linear array transducer (LV8-5N60-A2 ArtUs, Telemed, Vilnius, Lithuania), which was placed over the muscle belly using a custom-made holder and self-adhesive tape. B-mode images were recorded at 117 Hz with a field of view of 50 mm and depth of 65 mm. To make sure the cable of the ultrasound system did not obstruct the participants, the ultrasound control unit was placed in a box above the participants with an adjustable pulley system and cables were fastened with tape. A semi-automated tracking algorithm was used to analyse fascicle length and pennation angle (Cronin et al., 2011; Farris and Lichtwark, 2016). Fascicle length was defined as the linear trajectory between the superficial and deep aponeurosis in the direction of the visible fascicle fragments. Linear extrapolation was used when fascicle insertion exceeded the ultrasound image.
Fascicle length and pennation angle were resampled to the motion capture system's frequency (150 Hz) using linear interpolation and filtered using the same digital lowpass filter. Subsequently, fascicle velocity was calculated by numerical differentiation of the length.
Forces under the ski bindings
Muscle activity
EMG data were recorded at 2100 Hz using a telemetered system (Aktos, Myon, Schwarzenberg, Switzerland). The skin was first shaved and rinsed with isopropanol, and bipolar surface electrodes (24 mm diameter; Kendall Arbo H124SG electrode, Coviden, Minneapolis, MN, USA) were then mounted over the muscle belly of gastrocnemius lateralis, soleus and tibialis anterior as recommended in the Seniam guidelines (Hermens et al., 2000). EMG data were filtered with a second-order bandpass Butterworth filter with passband from 10 to 500 Hz before a moving root mean square (RMS) with a window length of 100 ms was calculated. RMS-filtered EMG data were individually normalised for each individual participant to the maximum value during DIAref. The threshold to classify the muscle as active was set to 25% of peak based on the recommendations of Ozgünen et al. (2010).
Cycle characteristics
A cycle was defined by the start of the kick until the start of the subsequent kick. The initiation of the kick phase was defined by the roller ski's speed becoming equal to that of the treadmill belt with a threshold of 0.5 km h−1, i.e. when the ski is no longer moving relative to the ground surface (Pellegrini et al., 2014). We used the reflective marker placed on the anterior wheel of the right roller ski as reference for the position of the ski in the anterior–posterior direction. The ski's speed was calculated using numerical differentiation of the marker position. To calculate speed along the treadmill belt, we rotated the coordinate system to be parallel to two markers placed along the progression axis on the treadmill. The speed data were filtered using a bidirectional second-order Butterworth filter with a cut-off frequency of 20 Hz.
Each cycle was further divided into three phases: kick phase, swing phase and glide phase. The start of swing phase was defined as when the ski’s speed was greater than the treadmill velocity (with a threshold of 0.5 km h−1). The start of the glide phase was defined as the greatest force increase (i.e. peak slope) from the force ski measurement, calculated from the numerical differential of the force curve.
Data analysis
Six complete cycles were included in the analysis for each participant and each condition. All data were visually inspected to identify and exclude potential cycles that deviate from the pattern of most cycles. All data were time normalized to 101 points per cycle by linear interpolation. For the statistical analysis, scalars were extracted from the variables [i.e. mean and peak fascicle and MTU length changes and velocities, and mean normalized and integrated EMG (iEMG) for each participant from the kick phase]. For all velocities, positive values indicate shortening and negative values indicate lengthening.
Statistics
Statistical comparisons of the extracted scalars were performed using Prism (version 9.1.1, GraphPad Software, LLC, San Diego, CA, USA). All variables were confirmed to be normally distributed using a Shapiro–Wilk's test (P>0.05). To assess our hypothesis that there is a stretch–shortening cycle at the MTU level, we tested whether net MTU elongation and shortening during the kick phase was greater than zero (for elongation) or less than zero (for shortening), using two single-sided one-sample t-tests (one test for net elongation, one test for net shortening). To test our hypothesis that the muscle fascicles shortened during the kick phase, we tested whether fascicle length change during the kick phase was less than zero using a single-sided one sample t-test. Muscles were considered active when EMG activity exceeded 2 times standard deviation.
To test the effect of speed and incline on the outcome variables, a repeated measures one-way ANOVA with a Greenhouse–Geisser correction was performed. Šídák post hoc tests were performed in cases of significant main effects of the condition, to compare the effect of incline and speed with DIAref. The significance level was set to P<0.05 for all statistical tests, and all data are presented as means±s.d.
RESULTS
Cycle characteristics
Repeated measures ANOVA revealed a main effect for average cycle time (P<0.0001) and kick duration (P<0.0001), while the kick phase was shortest compared with swing and glide phase in all conditions (Table 1). Cycle duration was longest for DIAref and shortest for DIAsteep. Kick duration was longest for DIAsteep for absolute and relative duration. The shortest absolute kick duration was measured for DIAfast, while the relative kick duration in DIAfast was not different from that in DIAref.
Binding forces and joint kinematics
During the kick phase, the ankle joint dorsiflexed at the beginning of the kick and subsequently underwent plantarflexion, while the knee joint underwent a flexion–extension cycle (Fig. 2). During the swing phase, force was approximately equal to body weight, while the ankle joint dorsiflexed, and the knee joint flexed. During the glide phase, force was around the normalized body mass. In all conditions, force declined slightly to 0.8±0.4 N during the glide phase, prior to an increase in force to 1.4±0.6 N before the end of the cycle. During force decline, the ankle dorsiflexed, and the knee extended before they changed direction in the end of the glide phase.
Binding forces and joint kinematics. Mean and individual values for ankle joint angle, knee joint angle and force (normalised to body weight, BW) measured under the ski bindings during diagonal-style roller skiing at a steep (DIAsteep, 2.5 m s−1, 10 deg), a fast (DIAfast, 3.5 m s−1, 5 deg) and a reference condition (DIAref, 2.5 m s−1, 5 deg). Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
Binding forces and joint kinematics. Mean and individual values for ankle joint angle, knee joint angle and force (normalised to body weight, BW) measured under the ski bindings during diagonal-style roller skiing at a steep (DIAsteep, 2.5 m s−1, 10 deg), a fast (DIAfast, 3.5 m s−1, 5 deg) and a reference condition (DIAref, 2.5 m s−1, 5 deg). Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
Fascicle and MTU behaviour
The MTU followed a stretch–shortening cycle, with a stretch of 0.99±0.03 cm (P<0.0001) and a shortening of 2.43±0.78 cm (P<0.0001), while gastrocnemius muscle fascicles shortened (0.91 ±0.27 cm; P<0.0001). Total MTU shortening was 1.44±0.87 cm, which was significantly more than total fascicle shortening (P<0.0001) (Fig. 3). Accordingly, peak shortening velocity was significantly faster for the MTU (37.53±6.48 cm s−1) than for the fascicles (7.38±3.20 cm s−1) (Figs 4 and 5). During swing and glide phases, the fascicles followed the pattern of the MTU length changes but at slower velocities.
Mean length changes for the muscle–tendon unit (MTU) and fascicles during roller skiing at the reference condition. Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
Fascicle and MTU length and velocity. Mean and individual data for MTU and fascicle length and velocity during roller skiing at a steep (DIAsteep), a fast (DIAfast) and a reference condition (DIAref). Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
Fascicle and MTU length and velocity. Mean and individual data for MTU and fascicle length and velocity during roller skiing at a steep (DIAsteep), a fast (DIAfast) and a reference condition (DIAref). Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
Fascicle and MTU shortening velocity. Mean and individual data points for MTU and fascicle peak shortening velocity during the kick phase of DIA roller skiing at a steep (DIAsteep), a fast (DIAfast) and a reference condition (DIAref). Shortening is denoted as positive velocities. N=13.
MTU peak length was longer in DIAsteep (52.22±3.18 cm) and DIAfast (51.86±3.14 cm) than in DIAref (51.67±3.04 cm). Length changes during the stretch phase were 0.65 cm greater for DIAfast (P=0.0003) and 0.61 cm greater for DIAsteep (P=0.0015) compared with DIAref. Peak MTU shortening velocity was also greater for both DIAfast and DIAsteep (DIAref 37.53±6.48 cm s−1, DIAfast 53±10.9 cm s−1 and DIAsteep 48.79±9.89 cm s−1), with a mean difference from DIAref of 15.47 cm s−1 (P<0.0001) and 11.26 cm s−1 (P<0.0001) for DIAfast and DIAsteep, respectively (Fig. 4). Across conditions, comparison of operating fascicle length showed no differences (P>0.05). However, fascicle length change was significantly smaller in DIAsteep (0.76±0.32 cm) than in DIAref (0.91±0.27 cm), with a mean difference of 0.15 cm (P=0.027). Multiple-comparison tests also showed that mean gastrocnemius medialis fascicle shortening velocity was slower in DIAsteep (3.42±1.48 cm s−1) than in DIAref (4.48 cm s−1; P=0.0007).
Muscle activity
Gastrocnemius lateralis and soleus were active during the kick phase (P<0.0001) and inactive during the swing phase (Fig. 6). Both muscles showed another increase in activity at the swing to glide transition and the last part of the stride cycle, which was only significant for soleus muscle (P=0.0227). At the faster speed, peak muscle activity was greater in gastrocnemius (23.1%, P=0.0006) and soleus (10.7%, P=0.025). On the steeper incline, peak muscle activity was also greater in gastrocnemius (23.8%, P=0.037) and soleus (15.4%, P<0.0001). Tibialis anterior muscle was also active during the kick phase but peak activity was during the swing phase.
Mean and individual muscle activity. Electromyography (EMG) data during roller skiing at a steep (DIAsteep), a fast (DIAfast) and a reference condition (DIAref) for the gastrocnemius lateralis (GL), soleus (SOL) and tibialis anterior (TA). Muscle activity data were normalised to the peak activity during DIAref. Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
Mean and individual muscle activity. Electromyography (EMG) data during roller skiing at a steep (DIAsteep), a fast (DIAfast) and a reference condition (DIAref) for the gastrocnemius lateralis (GL), soleus (SOL) and tibialis anterior (TA). Muscle activity data were normalised to the peak activity during DIAref. Vertical lines denote the phase transition between kick, swing and glide phase for each condition. N=13.
DISCUSSION
Combining ultrasound with motion analysis during diagonal-style roller skiing, we found that the MTU underwent a stretch–shortening cycle, while gastrocnemius muscle fascicles actively shortened during the kick phase. The MTU operated at significantly faster velocities compared with the fascicles. In the last part of the glide phase, which succeeds the kick, MTU already starts to lengthen, while muscle activity is increasing, and fascicles are contracting isometrically (i.e. fascicle velocity is around zero).
As hypothesised, skiers had a longer kick duration on the steeper incline (absolute and relative), which was accompanied by slower fascicle shortening velocity and greater muscle activity. Faster speed did not result in statistical differences in fascicle velocities or iEMG, but peak EMG activity was greater for both the steeper incline and the faster speed. During the kick phase, MTU stretch was greater and faster when the skier speed was faster and the incline was steeper, but MTU shortening velocity, i.e. recoil, was unaffected.
Uncoupled fascicle and MTU behaviour during the kick
During running, elastic elements in the MTU enable energy conservation. The mechanism is characterised by a fast MTU stretch and shortening pattern during the stance phase, while fascicles work isometrically or concentrically at much slower velocities (Lichtwark et al., 2007; Roberts and Azizi, 2011). Our data show that muscle fascicles follow a comparable pattern during the kick phase of diagonal-style roller skiing to that during running, despite the glide phase prior to the kick during DIA skiing. Similar mechanisms during skiing and running may be surprising considering that ground contact duration during skiing is much longer because of the added glide phase. Similar to walking, the foot's duty factor (i.e. percentage of cycle time with foot contact) during skiing is greater than 0.5. Notably, race walking was characterised by significantly more energetically expensive contractile patterns compared with running (Cronin et al., 2016). Thus, the glide phase during diagonal-style skiing, where calf muscles are mostly passive, seems to be unlike ground contact phases during walking and race walking, where muscle activation is high during the whole ground contact phase. Our results support, at least in part, the description of DIA skiing as ‘grounded running’ by Pellegrini et al. (2014). The term was originally used to describe a certain type of animal locomotion, highlighting the combination of characteristics from running where the gliding phase replaces parts of the aerial phase. Notably, grounded running has been associated with reduced musculoskeletal loading compared with other gaits (Bonnaerens et al., 2019).
Conservation of elastic energy and/or power amplification – as apparent in different types of locomotion (Roberts and Azizi, 2011) – may also play a role during diagonal-style skiing. Komi and Norman (1987) were the first to demonstrate a stretch–shortening pattern of the MTU during the kick phase of this gait. Interestingly, the stretch had already started at the end of the glide phase, immediately before the kick, and was suggested to be used as a preloading phase. Our data show a similar pattern in addition to an increase in gastrocnemius and soleus muscle activity (Fig. 5) at the end of the glide phase, supporting the notion that the muscles are active. This stretch–shortening cycle might indicate elastic energy storage and release during the glide and kick phases. Based on fluctuations of mechanical energy, Kehler et al. (2014) concluded that most of the mechanical energy is dissipated during the glide phase (through ski/snow friction) rather than being stored elastically. Hence, unlike running, the elastic energy released during the kick phase of DIA skiing is most likely actively generated during a brief preload phase prior to the kick, rather than a result of mechanical energy conservation throughout the stride cycle (as in a bouncing gait). The notion of energy dissipation during the glide phase based on mechanical energy transfer is consistent with our data showing little muscle activation during this phase (e.g. Brennan et al., 2018; Kehler et al., 2014).
Jumping is another movement with similarities to uphill cross-country skiing because both require positive work (Dahl et al., 2017). During jumping, elastic mechanisms in the MTU allow for power amplification by storing muscle work slowly and releasing it rapidly (Farris et al., 2016; Wade et al., 2018). In our results, the initial lengthening of the MTU with concurrent fascicle shortening at the transition between the glide and kick phases, along with the observation that MTU contraction velocity is substantially greater than fascicle contraction velocity (Fig. 4), provide a strong indication of a power amplification mechanism, similar to jumping. Besides jumping, positive work production by fascicles has been shown during running up an incline (Lichtwark and Wilson, 2006) and during accelerative movements in walking (Farris and Raiteri, 2017) and sprint running (Werkhausen et al., 2021). Those findings support the hypothesis that the compliant lower leg muscles contribute to positive work production when required. Indeed, the average fascicle shortening during DIAref of 0.91 cm was similar to fascicle shortening during accelerative sprinting (0.96 cm) and also MTU velocities were similar at around 50 cm s−1 (Werkhausen et al., 2021).
Overall, the simultaneous MTU stretch and fascicle shortening in the end of the glide phase and the beginning of the kick phase indicates that using stretch–shortening cycle exercises may be beneficial in training for skiers. They may also benefit from adjusting their technique for optimal energy storage by preloading elastic tissues at the end of the glide phase.
Speed and incline affect fascicle and muscle–tendon dynamics
Faster skiing speed and steeper incline altered cycle characteristics, forces and kinematics during diagonal-style roller skiing, in line with previous studies (Nilsson et al., 2004; Pellegrini et al., 2013). These differences were associated with differences in fascicle and MTU behaviour. At the faster speed, greater muscle activation for gastrocnemius and soleus muscles may be necessitated by the shorter kick phase. Fascicle behaviour, such as operating length and velocity, was preserved although peak MTU length was longer and velocity was greater in DIAfast compared with DIAref. Interestingly, this modulation of muscle behaviour to speed increases resembles that of running at faster speeds (Farris and Sawicki, 2012; Werkhausen et al., 2019). Based on the modulation of further speed increases during running, we speculate that greater increases in skiing speed (than in the current protocol) would lead to faster fascicle shortening velocities. Nevertheless, a concomitant increase in MTU velocity (while fascicle velocity did not differ) may indicate a greater stretch of elastic elements and thereby greater potential for energy recycling and power amplification when increasing speed at 1 m s−1 or 40%.
On the steeper incline, when the resistive force was greater, skiers increased absolute and relative kick duration. Contrary to the response to faster skiing speed, fascicle velocity was slower at DIAsteep, although MTU excursion and velocity were greater, probably allowing for increased force potential (according to the force–velocity relationship) of the muscle and thereby lower energy requirements (Lieber and Fridén, 2000). Yet, the greater peak muscle activity counteracts a possible energy saving of slower fascicle operating velocities by requiring more energy. Besides fascicle velocity, changes in operating lengths have a potential effect on energy consumption (Beck et al., 2022) but were not present when comparing our conditions. Lichtwark and Wilson (2006) reported that fascicles operated at longer lengths when running uphill compared with level running but concluded that this difference was marginal. Overall, differences in muscle behaviour in the different speed and incline conditions indicate that training at specific conditions may be necessary if athletes wish to train specific contractile modes.
Methodological considerations
Roller skiing on a treadmill closely resembles skiing on snow but it is important to note that small differences may influence the results in terms of muscle behaviour found in our study. Myklebust et al. (2022) found differences in pole push time and hip kinematics during skating (V2 skating technique) and several studies have discussed the importance of grip on snow for diagonal stride (e.g. Kehler et al., 2014). In our study, we used very experienced skiers and placed the ratchet mechanism on the front wheel to reduce grip, to minimise the differences between roller skiing and on-snow skiing. We consider including both sexes in our study a strength in general, but it is important to note that we have not considered sex differences in our analyses (Stöggl et al., 2018).
Conclusion
Uncoupling of fascicle behaviour of the gastrocnemius muscle from the limb joint movement during diagonal-style cross-country skiing suggests the use of elastic energy at different inclines and speeds. Skiers may use the end of the glide phase to preload the MTU for the stretch–shortening cycle during the kick, when muscle fascicles shorten actively. The muscle fascicle contractile patterns were overall similar at the two speeds and inclines studied here. Both faster skiing speed and steeper incline required greater muscle activation, but the fascicle contraction velocities were slower uphill.
Acknowledgements
Footnotes
Author contributions
Conceptualization: A.W., O.G.; Methodology: A.W., A.L., O.G.; Software: A.W., O.G.; Validation: O.G.; Formal analysis: A.W., A.L., O.G.; Investigation: A.W., A.L.; Data curation: A.W., A.L., O.G.; Writing - original draft: A.W.; Writing - review & editing: A.L., O.G.; Visualization: A.W.; Supervision: A.W.; Project administration: A.W., O.G.
Funding
This research received no specific grant from any funding agency in the public, commercial or not-for-profit sectors.
Data availability
All relevant data can be found within the article.
References
Competing interests
The authors declare no competing or financial interests.