Muscle function in glenohumeral joint stability during lifting task

Yoann Blache; Mickaël Begon; Benjamin Michaud; Landry Desmoulins; Paul Allard; Fabien Dal Maso

doi:10.1371/journal.pone.0189406

Abstract

Ensuring glenohumeral stability during repetitive lifting tasks is a key factor to reduce the risk of shoulder injuries. Nevertheless, the literature reveals some lack concerning the assessment of the muscles that ensure glenohumeral stability during specific lifting tasks. Therefore, the purpose of this study was to assess the stabilization function of shoulder muscles during a lifting task. Kinematics and muscle electromyograms (n = 9) were recorded from 13 healthy adults during a bi-manual lifting task performed from the hip to the shoulder level. A generic upper-limb OpenSim model was implemented to simulate glenohumeral stability and instability by performing static optimizations with and without glenohumeral stability constraints. This procedure enabled to compute the level of shoulder muscle activity and forces in the two conditions. Without the stability constraint, the simulated movement was unstable during 74%±16% of the time. The force of the supraspinatus was significantly increased of 107% (p<0.002) when the glenohumeral stability constraint was implemented. The increased supraspinatus force led to greater compressive force (p<0.001) and smaller shear force (p<0.001), which contributed to improved glenohumeral stability. It was concluded that the supraspinatus may be the main contributor to glenohumeral stability during lifting task.

Citation: Blache Y, Begon M, Michaud B, Desmoulins L, Allard P, Dal Maso F (2017) Muscle function in glenohumeral joint stability during lifting task. PLoS ONE 12(12): e0189406. https://doi.org/10.1371/journal.pone.0189406

Editor: Lucas van der Woude, Rijksuniversiteit Groningen, NETHERLANDS

Received: February 6, 2017; Accepted: November 26, 2017; Published: December 15, 2017

Copyright: © 2017 Blache et al. This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

Data Availability: All relevant data are within the paper and its Supporting Information files.

Funding: The authors received no specific funding for this work.

Competing interests: The authors have declared that no competing interests exist.

Introduction

The glenohumeral joint enables the greatest articular mobility in the human body at the expense of its stability [1–3]. Clinical instability is usually defined as any translation of the humeral head [4, 5] while, from a biomechanical point of view, glenohumeral joint instability occurs when the resultant glenohumeral reaction force points outside the glenoid surface [6].

Although glenohumeral instability may be caused by an external contact, internal forces produced by the muscles surrounding the humeral head may also result in glenohumeral instability. Near the maximal glenohumeral range of motion, translational forces parallel to the glenoid surface are counteracted by passive structures (e.g. capsulo-ligamentar elements, labrum and intra-joint vacuum) [7]. Nevertheless, translational forces may also be observed during the mid-range of humerus movements and therefore cause glenohumeral instability. Especially, Escamilla et al. [8] pointed out that the activation of the anterior deltoid may cause a translation of the humeral head and consequently reduce the stability of the glenohumeral joint. Therefore, movements such as lifting task for which middle and anterior deltoids are the main prime movers [9, 10] may be subject to glenohumeral instability.

It is commonly accepted that the rotator cuff muscles are the main glenohumeral joint stabilizers [5, 11, 12]. However, some patients with severe rotator cuff tears still manage shoulder function with a sufficient stability [13], meaning that glenohumeral stability results from a complex process. While, many studies assessed glenohumeral instability during analytical movements through cadaveric studies [1, 11, 14, 15] or electromyography approaches [16–18], only one study [19] investigated glenohumeral stability during daily living activities such as lifting task. The authors assumed that during a lifting movement, the latissimus dorsi and teres minor stabilize the glenohumeral joint. Nevertheless, their conclusions were based on cross-correlation analysis of the shoulder muscle activity measured without any condition of glenohumeral instability. Consequently, to the best of our knowledge, either with cadaveric or EMG methods, no study has clearly identified which muscles enable to stabilize glenohumeral joint during a lifting task. An analysis based on quantification of shoulder muscle forces with and without glenohumeral stability during a lifting task may provide relevant information on the muscles directly involved in glenohumeral stability.

Simulations based on musculoskeletal models may be an alternative approach, since some models include glenohumeral stability constraint, namely, the resultant of the reaction force between the humeral head and the scapula should point toward the glenoid cavity [20–22]. Dickerson et al. [23] used thresholds of glenohumeral dislocation in eight directions estimated from the ratio between the shear and compressive reaction forces between the glenoid fossa and the humeral head to ensure glenohumeral stability. Using such models, Steenbrink et al. [6] assessed the function of shoulder muscles in glenohumeral stability with different rotator cuff tears during static arm elevations, nevertheless, no information is given for healthy people.

Therefore, this study aimed to assess the stabilization function of the shoulder muscles in a healthy population during a lifting task. This repetitive task, usually performed in manufactory industry, may result in glenohumeral instability because of the main activation of the anterior and middle deltoids [9, 10]. We hypothesized that the glenohumeral stability constraint led to a greater force produced by the rotator cuff muscles and the latissimus dorsi in comparison to the condition without stability constraint.

Materials and methods

The study was approved by the “Comité d’éthique de la recherche en santé (CERES)” (Montréal, QC, Canada) (N°11-068-CERSS-D). All the participants provided a written informed consent before the experimentation.

Participants

Thirteen healthy participants (nine male: [mean ± SD] age, 25.8 ± 1.61 years; height, 1.81 ± 0.08 m; mass, 74.4 ± 11.9 kg; arm length, 35.1 ± 2.4 cm; forearm length, 27.0 ± 1.8 cm and four female: age, 21.8 ± 1.26 years; height, 1.68 ± 0.02 m; mass, 57.3 ± 2.2 kg; arm length, 33.9 ± 1.5 cm; forearm length, 24.5 ± 1.5 cm) right-handed subjects volunteered in this study. None of the participants presented current or previous shoulder, elbow or wrist injuries.

Instrumentation and data collection

Only the right (dominant) side of each participant was evaluated during the box lifting task, assuming that the right and left sides of the upper body moved symmetrically [24]. Based on the upper-limb kinematic model developed by Jackson et al. [25], 25 reflective skin markers were placed on the thorax, right clavicle, scapula, humerus, forearm, hand, and on the box used for the lifting task (Fig 1). Trials were recorded using an 18-camera Vicon^TM motion analysis system at 200 Hz (Oxford Metrics Ltd, Oxford, UK). Surface EMG electrodes (Trigno^TM EMG Wireless System, Delsys, USA; 1000 Hz) were positioned on nine muscles: biceps and triceps brachialis; anterior; middle and posterior deltoid; latissimus dorsi superior head; upper, middle and lower trapezius, according to SENIAM recommendations [26].

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Fig 1. Picture of the lifting task performed by a representative participant (left) and representation of the OpenSim musculoskeletal model of the upper limb.

Twenty-five reflective skin markers were placed on the thorax (xiphoid process, 3 markers on the manubrium, 1st and 10ththoracic vertebrae), on the right clavicle (sterno-clavicular joint, acromio-clavicular joint), scapula (acromion tip, acromial angle, inferior angle, trigonum spinae, superior angle), humerus (lateral and medial epicondyles), forearm (ulnar and radial styloid process), hand (proximal part of the 2nd and 3rd metacarpus, distal part of the 2nd and 5th metacarpus), and on the box used for the lifting task (four superior angles).

https://doi.org/10.1371/journal.pone.0189406.g001

The experimental test consisted of lifting a box (39.5 x 34.5 x 8 cm; 6 kg) positioned on a shelf from hip level to a shelf located at shoulder level. To standardize the grip of the box and ensure symmetrical movement, cylindrical handles (Ø 45 mm) were horizontally positioned on each side of the box. A 3D handle force sensor (SH2653-1106B3, Sensix, Poitiers, France; 2000 Hz) measured the 3D forces and torques between the box and the right hand. Kinematic, kinetic and EMG signals were synchronized using Nexus 1.8.2 software (Vicon, Oxford, UK).

Experimental procedures

To normalize the experimental EMG signals recorded during the lifting and to compare the latter to the musculoskeletal activations tasks (see below), two trials of 5 s isometric maximal voluntary contraction with verbal encouragement for each of the nine muscles were performed in random order by the participants in line with the recommendations of Dal Maso et al. [27]. The participants had to exert maximum force against an experimenter during five seconds with verbal encouragement. Two trials per muscle were performed and the rest interval was 30 seconds between repetitions and 60 seconds between trials for different muscles.

To get familiarized with the box lifting procedure, participants performed a total of 10 practice sagittal lifting movements. Finally, three trials were recorded with 30 s rest in-between, without any instruction about the speed and the handgrip technique. The participants chose their preferred horizontal distance from the shelves and were instructed to limit their foot displacements to one step back.

Data processing

After having analyzed the frequency and residual of the raw signals [28], EMG raw signal was band-pass filtered using a recursive 2^nd-order Butterworth band-pass filter (15–500 Hz) [29]. The root mean square (RMS) EMG was calculated on a 250-ms sliding window [30]. The RMS EMG of each muscle calculated for the lifting task was normalized in amplitude with respect to the maximum RMS EMG amplitude obtained from the maximal voluntary contractions.

Musculoskeletal model

We used an OpenSim generic model of the shoulder adapted to lifting task investigation (fully described in [9]) which was based on a combination of previous Opensim models [31–33]. Briefly the model was composed of 9 segments and 22 degrees-of-freedom and actuated by 22 muscle-tendon units (including 47 lines of actions with the muscle properties described in [34]) and 22 residual torque actuators (i.e. additional torque performed by the joint when the muscles cannot produce the joint torque required) (Fig 1). Assuming, the bilateral symmetry of the lifting movement [24], only the right upper-limb was modelled. The generic model was scaled to match each subject’s anthropometry using the experimental positions of the skin markers during a static pose. In addition, muscle maximal isometric forces were optimized for each subject-scaled-model by minimizing the difference between the normalized EMG and simulated muscle activations obtained during the lifting movement according to the method developed by Blache et al. [9].

Stability and instability simulations

Joint angles were obtained using an inverse kinematics procedure with a point-to-ellipsoid constraint to enforce the scapula to follow the thoracic curvature throughout the movement [35, 36]. The ellipsoid was locally fitted [35, 36] and only the technical skin markers defined in Jackson et al. [25] were considered. In addition, ranges of motion were controlled by implementing boundaries for each degree of freedom obtained from data free from soft-tissue artefact [37]. These joint kinematics and the handle forces/moments were introduced into two static optimization algorithms to estimate the muscle activations and forces required to perform the lifting task in the glenohumeral instability and stability conditions.

The first algorithm was performed from the graphical user interface of OpenSim 3.2 [38]. At each time sample, the quadratic sum of muscle activations and residuals torques were minimized, such that the sum of the muscle moments is equal to the torques computed from the inverse dynamic procedure. In the second algorithm an inequality constraint was added to ensure glenohumeral stability using dislocation thresholds (ratio of shear and compression glenohumeral joint forces) determined in eight directions on cadavers [23, 39]. The joint reaction force was calculated using the jointReaction algorithm of OpenSim 3.2 [38, 40] and the glenohumeral dislocation thresholds of [23] were expressed as eight inequality linear constraints using a polygon of friction [41]. To summarize, in the first algorithm, lifting movements were simulated with an instability of the glenohumeral joint, while in the second algorithm, the movements were simulated with a constraint ensuring the stability of the glenohumeral joint.

Evaluation of the model outputs with the stability constraint

Considering that the model with the glenohumeral stability constraint was the closest to human body mechanics, the outputs of the model were assessed by computing the RMS differences between normalized RMS EMG and the modelled muscle activations. Since some modelled muscles have up to five fascicles (biceps and triceps brachialis; upper, middle and lower trapezius), their mean activations were compared to the corresponding normalized EMG. Among the three trials performed by the participants, the trial with the lowest RMS difference was kept for further analysis. Finally, residual torques, which represent the capacity of the model to produce joint torques solely with its muscles were reported.

Analysis

The ratio between the duration for which the glenohumeral reaction force was outside the friction polygon and the total trial duration was calculated for the two conditions (with and without stability constraint). The mean muscle activations and forces resulting from the static optimization with and without the stability constraint were reported.

Statistics

The effect of the glenohumeral stability constraint on the mean residual torques; shear and compressive forces; ratio between the shear and compressive forces; muscle activations and forces was tested using linear mixed models. Linear mixed-model is an alternative method to the ANOVA on repeated measures that may be more advantageous especially with categorical data (Barr Levy, Scheepers, & Tily, 2013). As within-participants repeated measures were performed, participants were entered as random intercept. The p-values were obtained by likelihood ratio tests of full model (H₁) against the model without the effect of the glenohumeral stability constraint (H₀). The level of significance was initially set a p<0.05. Nevertheless, as 22 muscles were tested, a Bonferroni correction was applied (only for muscle activations and forces) to the initial level of significance that was finally set at p<0.002 (0.05/22). The linearity, homoscedasticity and normality of the residuals were graphically controlled. All analyses were executed using R software (R 3.2, RCore Team 2014, package lme4).

Results

Evaluation of the model outputs with the stability constraint

Residual mean torques were equal to 1.13 ± 0.80 N·m on average. Particularly, the residual mean torques for the three glenohumeral rotations (plane of elevation, elevation and rotation) were equal 0.22 ± 0.29 N·m, 0.15 ± 0.21 N·m and 0.41 ± 0.42 N·m, respectively (S1 Fig). The average RMS difference between the normalized EMG and the muscle model activations was 12.6 ± 6.3% of the maximal activation. (S2 Fig). The constraint of stability was respected throughout the simulated movement.

Glenohumeral stability constraint

All individual data are presented in supplementary materials (S1 File). The residual torques curves were similar with and without glenohumeral stability constraint (Fig 2). Furthermore, significant difference in the mean residual torques (with vs. without glenohumeral stability constraints) were only found for axial rotation of the humerus and elbow prono-supination (p = 0001; difference = 0.11 ± 0.10 Nm) and could be considered as negligible.

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Fig 2. Average (±1 standard deviation represented by the shaded envelop) residual torques obtained with (in red) and without (in blue) glenohumeral stability constraint for all the participants (n = 13).

Time is normalized with respect to trial duration.

https://doi.org/10.1371/journal.pone.0189406.g002

In the case without stability constraint, 74.0 ± 16.0% of the total lifting duration corresponded to glenohumeral reaction forces outside of the friction polygon, especially in an upward and backward direction (Fig 3).

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Fig 3. Representation of the friction polygon (in grey) and the ratio between the shear (postero-anterior and caudal-cranial) and compression forces (black cross) with (left) and without (right) glenohumeral stability constraint from all the participants (n = 13).

The stability of the glenohumeral joint was ensured when the ratio was inside the friction polygon.

https://doi.org/10.1371/journal.pone.0189406.g003

The implementation of the glenohumeral stability constraint resulted in a significant greater mean normalized activation of the supraspinatus compared to the model without glenohumeral stability constraint (10 ± 11% vs. 20 ± 14%; χ²(4) = 16.4, p<0.002, power = 0.99), while the normalized activity of the biceps long head was significantly decreased (19 ± 8% vs. 14 ± 3%; χ²(4) = 10.2, p<0.002, power = 0.93) (Fig 4). The other mean muscle activations remained similar with vs. without glenohumeral stability constraint, but tendencies were found for the serratus anterior (p = 0.01, power = 0.77) and the triceps brachialis long head (p = 0.004, power = 0.90). The change in muscle activations resulted in a mean force of the supraspinatus on average two times larger due to the glenohumeral stability constraint (41 ± 34 N vs. 83 ± 49 N, χ²(4) = 15.0, p<0.002, power = 0.99), while the mean force was about 50 N lower for the biceps long head (185 ± 107 N vs. 132 ± 97 N, χ²(4) = 10.9, p<0.002, power = 0.95) (Fig 4). The other muscle mean forces remained similar with and without glenohumeral stability constraint, but tendencies were found for the pectoralis major (p = 0.008, power = 0.77), middle trapezius (p = 0.004, power = 0.86), serratus anterior (p = 0.01, power = 0.72) and triceps brachialis long head (p = 0.004, power = 0.90).

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Fig 4. Mean normalized activations (left) and muscle forces (right) obtained with the musculoskeletal model with (in red) and without (in blue) stability constraint from all the participants (n = 13).

Notes: Coracobrac: Coracobrachialis; Scap. Elev.: Scapular Elevator; Trap.: Trapezius; Latiss: Latissimus; Pect: Pectoralis; Sup: Superior; Mid: Middle; Low: Lower, Post: Posterior; Mid: Middle; Ant: Anterior. * means that the difference was significative with a p-value < 0.002.

https://doi.org/10.1371/journal.pone.0189406.g004

The mean compressive force was significantly greater (p<0.01, power = 0.90) with the implementation of the glenohumeral stability constraint and the shear forces significantly lower (p<0.001, power = 0.99). Consequently, the mean ratio between shear and compressive forces was significantly reduced with glenohumeral stability constraint (p<0.001, power = 0.99) (Fig 5).

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Fig 5. Average (±1 standard deviation represented by the shaded envelop) glenohumeral force oriented toward and orthogonally to the glenoid fossa (compressive force in newtons–Top) and tangential to the glenoid fossa, namely, in anterior-posterior and cranio-caudal directions (shear force in newtons—middle).

Ratio between the shear and compression glenohumeral forces (bottom). Red and blue curves correspond to the condition with and without stability constraint respectively for all the participants (n = 13). Time is normalized with respect to trial duration, corresponding to the time from the onset of the lifting movement to the release of the box.

https://doi.org/10.1371/journal.pone.0189406.g005

Discussion

Our objective was to assess stabilization function of shoulder muscles during a lifting task using an upper-limb musculoskeletal model with vs. without glenohumeral stability constraint. Our hypothesis was partially verified since only the supraspinatus among rotator cuff muscles was sensitive to the glenohumeral stability constraint. We may assume that the supraspinatus has a significant function in the glenohumeral stabilization during lifting task.

Evaluation of the model outputs with the stability constraint

Using static optimization, musculoskeletal model outputs depend mainly on the measured marker trajectories [42]. Although we cannot quantify the accuracy of the shoulder kinematics in the present study, we have used state-of-the-art methods that enable the limitation of the negative effects of tissue artifact. Indeed, multibody kinematics optimization with Jackson et al. [25] technical markers combined to an ellipsoid constraint should lead to error inferior to 10° and 5° for the scapulo-thoracic and humerothoracic joints respectively [42].

Although the musculoskeletal model was not subject-specific but scaled, it respected the salient characteristics of the participants’ lifting movements. Firstly, the residual torques were low compared to the torques computed from inverse dynamics (e.g. residuals < 0.41 N·m for the glenohumeral joint), meaning that the joint torques were mainly ensured by the modelled muscles. However, elbow pro-supination and wrist joint torques were produced by the residual torque actuators due to the absence of modeled muscles implemented around the elbow and wrist joints. Since the upper-limb is a kinetic chain, the absence of wrist and some elbow modeled muscles may lead to discrepancies between modeled and in-vivo muscle forces. Nevertheless, all bi-articular muscles, such as the biceps brachii, crossing both the glenohumeral joint and the wrist have been implemented in the model. Consequently, we believe that all muscles crossing the glenohumeral joint play their part into the shoulder/upper-limb chain, limiting therefore the negative effect of virtual torque actuators on shoulder muscle estimate.

Secondly, similarly to Hawkes et al. [19], we observed that among the superficial muscles, the musculoskeletal model yielded greater averaged activations of the upper trapezius and anterior deltoid in comparison to the posterior deltoid and latissimus dorsi. Nevertheless, even if the modeled activations and EMG amplitude were close (12% of difference on average), the musculoskeletal model underestimated muscle activations as in Huang et al. [43] because of the least activation criterion. The co-activation between agonist and antagonist muscles is limited to the glenohumeral stability condition. For example, the activations of the trapezius and serratus anterior that ensure the scapula stabilization using co-contraction [44] were underestimated (S2 Fig). Although assessing the effect of such an underestimation on our outcomes is not straightforward, it may be limited since trapezius and serratus anterior are not inserted on the humerus and do not affect directly glenohumeral joint stability. Advanced musculoskeletal algorithms using the EMG as input [45] could be implemented in future studies.

Finally, we did not compare the simulated glenohumeral joint reaction forces to experimental data. Nevertheless, a previous study [46] based on the Delft Shoulder and Elbow model put forward that the glenohumeral joint reaction forces computed with their model were similar to those measured in patients for similar shoulder ranges of motion [47]. The simulated glenohumeral joint reaction forces measured in our study were slightly greater than those observed in their patient group but in the same order of magnitude (933±205 N vs. ~650 N, respectively). These discrepancies may be due to the higher load lifted in our study (6 kg vs. 0 kg). Consequently, we may assume that our glenohumeral reaction forces were realistic.

Modeled glenohumeral stability and instability

From a clinical point of view, glenohumeral joint instability has been defined as a too large displacement that may lead to joint dislocation in an extreme case [3, 5]. Therefore, using a musculoskeletal model with the implementation of a constraint of glenohumeral stability based on dislocation thresholds seems to be relevant to simulate glenohumeral stability or instability. Threshold values of Dickerson et al. [23] implemented as inequality linear constraints as proposed in Wieber [48] enabled to respect glenohumeral stability with an efficient computing approach. Indeed, 100% of the glenohumeral joint reaction forces were inside the polygon friction when the constraint was implemented compared to about 25% without the constraint.

A limitation related to our musculoskeletal model was that glenohumeral joint reaction force was only the resultant of muscle forces. Therefore, glenohumeral joint stability was only ensured by the muscles, while passive structures such as the labrum and glenohumeral ligaments may also participate to glenohumeral joint stability [12]. This simplification could lead to an overestimation of the role of the shoulder muscles in glenohumeral joint stability. However, Engin and Chen [7] observed that passive contribution of the glenohumeral ligament were negligible during the mid-range of motion and increased only from the last 20° of the humerus elevation. In our studied lifting task, the glenohumeral joint was not close to its maximal elevation, since the box was lifted from the hip to the shoulder level. Consequently, we may assume that the glenohumeral ligament had a negligible effect on glenohumeral stability. In addition, Halder et al. [2] observed that the labrum contributed to less than 10% of the glenohumeral stability whatever the direction of the humerus movement. Therefore, during the lifting task investigated here, we may assume that the contribution of the passive structures to the glenohumeral stability was small and the shoulder muscles mainly ensured that glenohumeral joint stability.

Stabilisation function of the shoulder muscles

Only the supraspinatus developed significantly more force when the glenohumeral stability constraint was implemented. Other muscles such as the pectoralis major, middle trapezius, serratus anterior and triceps long head tended to produce more force with the glenohumeral stability constraint. Although the supraspinatus is most sensitive to the glenohumeral stability constraint, the tendency of the other muscles to produce more force denotes that the stability of the shoulder is a complex system. Indeed, the stabilization function of a given muscle is possible only with the co-activation of the other shoulder muscles [12, 49].

According to the mechanical definition of the glenohumeral stability or instability given in our introduction [3] and previous study using the same method [6], we may assume that the supraspinatus ensures a great part of the glenohumeral stability during a lifting task. This outcome is in accordance with several studies [12, 15–17, 39, 50] that pointed out that the main function of the supraspinatus is to stabilize the glenohumeral joint. The increase in the supraspinatus force would enable to decrease the glenohumeral shear forces and to increase the compressive forces (Fig 5). In addition, previous studies assumed that the direction of the supraspinatus line of action enables the latter to compress the glenohumeral head against the glenoid fossa [3, 51], especially to act against humeral head translations caused by the deltoids muscle activations [8]. During lifting task, the anterior and middle deltoids are activated to ensure arm flexion and abduction (similar activation with and without stability constraint). Therefore, we may assume that the extra activation of the supraspinatus is necessary to overcome the pulling effect of the deltoids, since the deltoid muscles may pull the humeral head outside the glenoid fossa.

Contrary to previous studies and our hypothesis, we did not observe that the other rotator cuff muscles and the latissimus dorsi produced more force with the stability glenohumeral constraint. One explanation may be that during the lifting task most of the glenohumeral forces pointed in a backward and upward directions (Fig 3), consequently the stabilization function of the subscapularis (i.e. to limit anteroposterior translations of the humeral head [12]) may be limited. The force produced by the subscapularis with and without the stability constraint was probably used to ensure the internal rotation of the humerus observed during the lifting phase. These results reinforce the hypothesis that the function of the rotator cuff muscles may differ depending on the direction of the arm movement [50]. Our results should however be taken with caution, because rotator cuff activations were not measured using invasive intramuscular EMG as in [52, 53].

A last limitation was that only one box dimension was chosen regardless the participant’s anthropometry and strength. In consequence, the relative load and dimension differed between participants increasing the inter-subject joint kinematics and kinetics variability. However, in manufactory industry, the mass of the box that need to be lifted are not dependent of the employee anthropometry. In consequence, only one box dimension corresponding to the manufacturing standards was used in this study such as previous investigations in ergonomics field [19, 31, 54]. Further studies are needed to assess the effect of box mass and dimension on glenohumeral stability during lifting tasks.

Conclusion

To the best of our knowledge, this study is the first that evaluated the contribution of shoulder muscles in glenohumeral stability during dynamic movement such as a lifting task. Considering that the musculoskeletal model has reproduced the salient characteristics of the participants’ movements, the simulations with and without glenohumeral stability constraint enabled to better understand the role of stabilizing muscles during a lifting task. We observed that only the supraspinatus muscle was sensitive to the glenohumeral stability constraint. This outcome provides further evidences that the supraspinatus may be a main stabilizer of the glenohumeral joint in a healthy population during lifting task. Thus, it may be assumed that the integrity of the supraspinatus is necessary to prevent glenohumeral instability and therefore limit the risk of shoulder injuries during lifting tasks.

Supporting information

S1 Fig. Average (±1 standard deviation represented by the shaded envelop) joints torques obtained with inverse dynamics (red), and residuals torques obtained with static optimization (blue) for the 13 degrees of freedom actuated by the muscles model.

Time is normalized with respect to trial duration.

https://doi.org/10.1371/journal.pone.0189406.s001

(DOCX)

S2 Fig. Average (±1 standard deviation represented by the shaded envelop) muscle model activations obtained with static optimization (in red) and normalized EMG (in blue).

Time is normalized with respect to trial duration.

https://doi.org/10.1371/journal.pone.0189406.s002

(DOCX)

S1 File. Individual data used to perform the statistics.

https://doi.org/10.1371/journal.pone.0189406.s003

(XLSX)

Acknowledgments

We would like to thank the Institut National du Sport du Québec for the loan of the electromyographic wireless system.

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Figures

Abstract

Introduction

Materials and methods

Participants

Instrumentation and data collection

Experimental procedures

Data processing

Musculoskeletal model

Stability and instability simulations

Evaluation of the model outputs with the stability constraint

Analysis

Statistics

Results

Evaluation of the model outputs with the stability constraint

Glenohumeral stability constraint

Discussion

Evaluation of the model outputs with the stability constraint

Modeled glenohumeral stability and instability

Stabilisation function of the shoulder muscles

Conclusion

Supporting information

S1 Fig. Average (±1 standard deviation represented by the shaded envelop) joints torques obtained with inverse dynamics (red), and residuals torques obtained with static optimization (blue) for the 13 degrees of freedom actuated by the muscles model.

S2 Fig. Average (±1 standard deviation represented by the shaded envelop) muscle model activations obtained with static optimization (in red) and normalized EMG (in blue).

S1 File. Individual data used to perform the statistics.

Acknowledgments

References