The analysis included an investigation of the hip, shoulder and spine angular segments and a complete balance study using the COM as the reference. Initially, each golfer was asked to stay in a neutral upright standing position to initialize the marker position as the reference position. The estimated COM during upright position was assumed to be the most postural stable position. The beginning of the swing was defined by the first position change of the club head. A reflective ball was used to define the moment of impact. For the purpose of calculating the 3D kinematic data, the three best swings of the player were captured and reconstructed using VICON cameras and Nexus software. The player confirmed the swing was an adequate representation of their normal swing and the investigator confirmed adequate data capture. Each swing was assumed as an independent sample for the final data analysis. Following the 3D reconstruction, a quintic spline function (MATLAB, The MathWorks, Inc., Natick, MA) was applied to the raw coordinates in order to smooth the data and calculate kinematic quantities. The calculation of the different angles using the 3D location of each marker was done using a simple trigonometric model. Specifically, the hip angle was defined as the angle in the transverse plane between the lines connecting the two hip markers while standing in the neutral position and at any point in time. The same definition was applied for shoulder angles using the two shoulder’s markers. For both angles, a positive value was indicative of a rotation from the neutral position away from the imaginary target and a negative value represented a rotation towards the target as illustrated in Figure 2. The COM movement during the swing was estimated using a two-link biomechanical model. The details of this model and its accuracy compare to a full body model have been described in our previous publications. (Najafi et al., 2010b; Marclay et al., 2012) In summary, the position of COM was estimated using the subject’s anthropometry data (i.e. height and body mass) and measuring spine and ankle joint angles (respectively using back markers and leg markers). Our previous study demonstrated that this simplified model has a high agreement with the estimated values using the full body model during golf swing trials (r = 0.93 ± 0.05 for A-P and r = 0.95 ± 0.03 for M-L directions) (Marclay et al., 2012). In another study, we demonstrated that the range of COM motion estimated using this model has a high correlation (r > 0.95, p < 0.001) with the range of center of pressure (COP) motion measured using a pressure platform (Najafi et al., 2010a). Reducing the number of reflective markers from 36 (for full body model) to nine, allows us to reduce the time of measurement as well as minimizing the degree of inconvenience for players for performing more natural swing trials. We didn’t use COP measurement in this study, since our initial observations suggested that the natural base of support of our golfers exceed the measurable area of a standard pressure/force platform. The maximum speed of the arm during the downswing was determined with the markers located on the left arm of each player. For this purpose, the total arm distance from the top of the backswing to the impact of the ball is differentiated and multiplied by the frequency of the system. In a similar way, the speed and acceleration of the COM were also calculated and analyzed. Based on our initial observations and comparing with the Vicon data, we defined the top of the backswing as the minimum peak of the COM in A-P direction. As far as we know, this represents the first time the backswing has been defined by the COM rather than the club stopping or body rotation stopping (Mcteigue et al., 1994). This measure may be unbiased by different swing strategies based on skill level. This peak could be accurately detected using a peak detection algorithm and could objectively discriminate between the backswing and downswing. Therefore, the minimum position of COMA-P was used as the data point to separate these two phases. Figure 3A demonstrates the different phases of the golf swing, including the COM variability at the top of the backswing and at maximal arm speed during the swing. COM was estimated at the key instances during swing including the time of upright position (tUP), address (tAdd), top of backswing (tTBS), impact (tImpact), maximum arm’s speed (tMAS), and maximum COM acceleration (tAccMax). To characterize and analyze dynamic balance for each group, COM distances as well as areas between each two measured instances were calculated and compared. An example of COM distances (A-P and M-L) and COM area (Figure 3A, dashed surface) between tUP (Figure 3A, star point) and tTBS is illustrated in Figure 3A. In a second part of the study, we analyzed the influence of the arm speed during the swing. It stands to reason that arm movement can also influence the motion of the COM and challenge the postural control. For this purpose, the different COM distances and areas were normalized by the maximum arm speed of each golfer. Finally, a new measure was introduced as part of the balance control of the golfer: the COM’s linearity during the early downswing. This measure was intended to correspond to the teaching philosophy that there is a flat and straight trajectory into impact although this philosophy has some controversy. It is based on others work on center of pressure changes in the swing despite different strategies (Ball and Best, 2007) and the club following one plane in some despite the body moving in different planes (Coleman and Anderson, 2007). We assumed that we may achieve the best energy efficacy if the COM moves on a linear trajectory from the top of backswing toward the address point. Therefore, we calculated the non-linearity of the downswing COM trajectory and assumed it as an outcome to assess the skill level. Based on this definition, a lower non-linearity value indicates a better skill level. Figure 3B demonstrates the interpretation of the linearity for a typical trajectory of the COM. To estimate the non-linearity, first we projected in A-P direction, the position of COM at tAdd on the COM downswing curve: (Figure 3B, square point). Then, the maximum difference between the curve of the COM during downswing phase and the straight line joining the top of the backswing and the projected point was calculated. The estimated maximum distance was assumed as the maximum non-linearity of the downswing curve. We normalized this value by the range of motion of COM in A-P direction to estimate the percentage of non-linearity. |