Effect of the Grip Angle on Off-Spin Bowling Performance Parameters, Analysed with a Smart Cricket Ball

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Proceedings Effect of the Grip Angle on Off-Spin Bowling Performance Parameters, Analysed with a Smart Cricket Ball Franz Konstantin Fuss 1, *, Batdelger Doljin 1 and René E. D. Ferdinands 2 1 Smart Equipment Engineering and Wearable Technologies Research Program, Centre for Design Innovation, Swinburne University of Technology, Melbourne, VIC 3122, Australia; bdoljm@swin.edu.au 2 Discipline of Exercise and Sports Science, University of Sydney, Sydney, NSW 2141, Australia; edouard.ferdinands@sydney.edu.au * Correspondence: fkfuss@swin.edu.au; Tel.: +61-3-9214-6882 Presented at the 12th Conference of the International Sports Engineering Association, Brisbane, Queensland, Australia, 26 28 March 2018. Published: 14 February 2018 Abstract: In the off-spin bowling grip, the ball is clamped between index and middle fingers. Spin bowlers attempt to select a spread angle between these two fingers that achieves comfort and optimises performance. The aim of this paper was to investigate whether the standard grip is superior to narrow and wide grips. The bowling performance parameters were obtained from a smart cricket ball. Smart ball data revealed that the performance parameters varied with grip type. The following parameters were optimum at the standard grip: spin rate, resultant torque, spin torque, peak angular acceleration, and peak power. The following parameters were optimum at standard and wide grips: efficiency. The following parameters were optimum at standard and narrow grips: pitch angle of spin axis. The following parameters were optimum at the wide grip: precession and the precession torque. In general, the data tended to show that the standard grip is most effective for spin bowling. However, more research is needed to confirm this result, because the precession and precession torque were optimum at the wide grip, suggesting that this may have a superior performance over the standard and narrow grips. Keywords: cricket; smart cricket ball; spin rate; torque; acceleration; precession; efficiency; performance; finger spread angle; spin bowling 1. Introduction In spin bowling, the fingers of the bowler are distributed around the seam of the ball in order to impart spin about an axis perpendicular to the seam. In off-spin bowling (fingerspin with a sidespin component), this is achieved by (i) combining the movement of forearm joints and wrist joint (supination + ulnar abduction); (ii) rotating the fingers that grip the ball (finger flexion and ulnar abduction; thumb reposition); and most importantly, (iii) ensuring that the last contact is between middle finger and ball immediately before release [1]. The angle between index and middle fingers varies with bowlers, the size of the angle depending on hand size, perception (which grip width is comfortable for the bowler), and coaching (which grip style the bowler was taught by the coach). For investigating whether there is an optimum grip width or finger spread angle (between index and middle fingers), the different grip-types have to be compared with hand dynamics and performance (such as, accuracy of hitting a spot on the pitch and the number of wickets taken in a season). A smart cricket ball [1 7] can be used to measure multiple parameters of hand dynamics during the period when the fingers apply spin to the ball. Proceedings 2018, 2, 204; doi:10.3390/proceedings2060204 www.mdpi.com/journal/proceedings

Proceedings 2018, 2, 204 2 of 6 The aim of this study is to use the smart ball to determine whether there is an optimal grip width for spin bowling based on hand dynamics. 2. Material and Methods 2.1. Smart Cricket Ball The smart cricket ball used in this study [1,2,7] samples the angular velocity data about the three axes of the ball s coordinate system at 815 Hz with three high-speed digital gyroscopes, which have a maximum measurement range of 50 rps. The data are transferred wirelessly to a Smartphone or computer via Bluetooth. The battery of the ball is charged wirelessly. 2.2. Participants A male off-spinner (amateur cricket club level) participated in the study. The participant bowled the ball 10 times each for three different grip widths. The seam sector angle between the fingertips of index and middle fingers was between 90 and 120 degrees for the standard grip, >130 for the wide grip, and <80 in the narrow grip (Figure 1). The Smart Cricket Ball study was approved by the RMIT University Human Ethics Committee (approval No. BSEHAPP 13-12). Figure 1. Three different grip width (angle between index and middle finger tips) investigated in this study: from left to right: narrow grip; standard grip; wide grip. 2.3. Performance Parameters A total of nine different performance parameters (Table 1) were calculated from the raw data: spin rate (ω), pitch of the spin axis (angular deviation of the spin axis from the pole of the ball, where the pitch is 90 degrees if the spin axis is exactly at the pole of the ball), angular acceleration (α), resultant torque (TR), spin torque (Tω), precession torque (Tp), power (P), precession (p; speed of the moving spin axis), normalised precession (pn; angle between spin and torque vectors [2]), and efficiency (η) of bowling (ratio of actual to ideal energy expressed as a percentage). All performance data used in this study are expressed as peak data (maxima) with the exception of efficiency (which is an energy ratio). The bowling performance is improved when spin rate, acceleration, resultant and spin torque, power, and efficiency increase significantly, with concomitant decreases in precession torque, precession, and normalized precession [2,4,5]. As the spin rate depends on the torque data, the torques were normalised to the spin rate (TR/ω, Tω/ω, Tp/ω). A bowling delivery is more effective the smaller the torque required per resultant spin rate. 2.4. Data Analysis and Statistics The performance parameters as detailed above were calculated with the Smart Cricket Ball software. The raw gyro data were filtered by a Butterworth low-pass filter of the 3rd order with a cut-off frequency of 30 Hz. The vectors obtained from the software are aligned to the coordinate system of the ball. The numeric performance data were correlated with grip width, which was treated as an ordinal variable (narrow = 1, standard = 2, wide = 3). The data were subjected to a non-linear regression

Proceedings 2018, 2, 204 3 of 6 analysis with a 2nd order polynomial for trend analysis. This analysis was used to verify whether the data showed a real trend for a p-value of the regression (p < 0.05). The 2nd order polynomial fit is able to detect a bidirectional trend, required for defining an optimum point. The distribution of the performance parameters within the 3 different grip widths was assumed to be Gaussian in theory. The performance parameters of the 3 different grip widths were compared with an ANOVA test followed by 4 posthoc tests (Tukey, Scheffe, Bonferroni and Holm). The ANOVA test strengthened the case for detecting a trend in the regression analysis. A significant difference was established if the p-value was smaller than 0.05 for the ANOVA test and the posthoc tests. 3. Results The participant generated the following smart ball data: spin rate of 18.3 rps on average for his standard grip; 0.2 Nm resultant torque; 12.3 W peak power; and 53.7 pitch on average (the angle between the spin axis at release and the perpendicular to the plane of the seam was 36.3 ). These data were below average for off-spinners [8]. However, the following data were above average [8]: bowling efficiency was 60.6%, precession 34 rad/s, and normalised precession 58.2 on average. The trend analysis revealed 6 different parameters (Figure 2). In the first 5 trend patterns (below), the regression p and the ANOVA p were smaller than 0.05. The posthoc tests showed the same significance or non-significance levels (p was either larger or smaller 0.05) across all 4 posthoc tests within each trend patterns. 1. Optimum point (highest performance) at the standard grip and less performance at wide and narrow grips: standard grip performance was significantly higher compared to narrow and wide grips, with insignificant difference between wide and narrow grips. This trend was seen in the spin rate, resultant torque, spin torque, Tω/ω, peak angular acceleration, and peak power. 2. Optimum point (highest performance) at the standard and narrow grips and less performance at the wide grip: standard and narrow grip performance was significantly higher compared to the wide grip, with insignificant difference between standard and narrow grips. This trend was seen in pitch and TR/ω. 3. Optimum point (highest performance) at the standard and wide grips and less performance at the narrow grip: standard and wide grip performance was significantly higher compared to the narrow grip, with insignificant difference between standard and wide grips. This trend was seen in the efficiency. 4. Optimum point (highest performance) at the wide grip and less performance at standard and narrow grips: the wide grip performance was significantly higher compared to standard and narrow grips, with insignificant difference between standard and narrow grips). This trend was seen in the precession and the precession torque. 5. Optimum point (highest performance) at the wide grip and decreasing performance over standard to narrow grip: all 3 grip performances were significantly different. This trend was seen in Tp/ω. 6. No trend at all (regression p > 0.05; ANOVA p > 0.05), seen in the normalized precession. With the exception of normalized precession, precession torque and Tp/ω, there was an optimum performance value at the standard grip in the remaining 10 performance parameters. In 4 of these 10 performance parameters, there was a further optimum, in addition to the standard grip, either at the narrow or at the wide grip. The latter two grips, however, did not achieve a consistent optimum. Precession torque and its normalized Tp/ω did not follow the overall trend and showed an optimum at the wide grip.

Proceedings 2018, 2, 204 4 of 6 22 70 45 20 60 40 spin rate (rps) 18 16 14 12 pitch (deg) 50 40 30 20 precession (rad/s) 35 30 25 10 10 8 0 20 85 0.24 0.22 80 0.22 0.2 normalised precession (deg) 75 70 65 60 55 resultant torque T R (Nm) 0.2 0.18 0.16 0.14 spin torque Tω (Nm) 0.18 0.16 0.14 0.12 0.1 50 0.12 0.08 45 0.1 0.06 0.14 3000 17.5 precession torque T p (Nm) 0.12 0.1 0.08 0.06 angular acceleration α (rad/s 2 ) 2500 2000 1500 1000 power P (W) 15 12.5 10 7.5 5 0.04 500 2.5 80 0.013 0.009 75 70 0.012 0.008 efficiency ϕ (-) 65 60 55 50 T R /ω (Nm/rps) 0.011 0.01 Tp/ω (Nm/rps) 0.007 0.006 0.005 0.004 45 40 0.009 0.003 35 0.008 0.002 Figure 2. Box plots (red) and parabolic fit functions (blue) of performance parameters against narrow, standard and wide grips; from left to right and top to bottom: spin rate ω (rps), pitch (deg), precession (rad/s), normalized precession (deg), resultant torque TR (Nm), spin torque Tω (Nm), precession torque Tp (Nm), acceleration α (rad/s 2 ), power P (W), efficiency η ( ), TR/ω (Nm/rps), Tp/ω (Nm/rps).

Proceedings 2018, 2, 204 Table 1. Performance parameters and their statistics; bold font: p < 0.05 (significant difference); italic font: p > 0.05 (insign precession; pn = normalised precession; TR = resultant torque; Tω = spin torque; Tp = precession torque; α = angular acceleration Statistics Regression R 2 Regression p ANOVA p Max Posthoc p: Narrow vs. Standard Max Posthoc p: Narrow vs. Wide Max Posthoc p: Standard vs. Wide Narrow (Mean ± S ω (rps) 0.4162 0.0001 0.0007 0.0010 0.4373 0.0305 14.16 ± pitch ( ) 0.6450 <0.0001 <0.0001 1.0000 0.0010 0.0010 55.26 ± max p (rad/s) 0.2999 0.0017 0.0081 1.0000 0.0193 0.0284 34.39 ± pn ( ) 0.0536 0.2182 0.4751 1.0000 0.9775 0.8051 58.82 ± 1 max TR (Nm) 0.3462 0.0006 0.0032 0.0157 1.0000 0.0079 0.156 ± 0 max Tωω (Nm) 0.4445 0.0001 0.0004 0.0010 1.0000 0.0042 0.125 ± 0 max Tp (Nm) 0.5628 <0.0001 <0.0001 1.0000 0.0010 0.0010 0.100 ± 0 max α (rad/s 2 ) 0.4445 0.0001 0.0004 0.0010 1.0000 0.0042 1602.9 ± max P (W) 0.4352 0.0001 0.0004 0.0010 1.0000 0.0078 7.30 ± 3 η (%) 0.3468 0.0006 0.0032 0.0220 0.0061 1.0000 51.67 ± TR/ω (Nm/rps) 0.4424 0.0001 0.0004 1.0000 0.0019 0.0018 0.0109 ± 0 Tω/ω (Nm/rps) 0.3745 0.0003 0.0018 0.0115 1.0000 0.0042 0.0086 ± 0 Tp/ω (Nm/rps) 0.8222 <0.0001 <0.0001 0.0010 0.0010 0.0010 0.0071 ± 0

Proceedings 2018, 2, 204 6 of 6 4. Discussion The smart ball data showed that the performance parameters of the standard grip generally outweighed the parameters of the two other grips. This suggests that experienced spin bowlers had over time adopted a grip with a finger spread that they could perform effectively. The ideal finger spread angle, according to the general coaches recommendation, is as wide as comfortably possible. However, this experimental protocol cannot determine conclusively that the finger-spread (gripwidth) used by the bowler was biomechanically optimal, since the bowler had less experience using the narrow and wide grips. The problem here is the training effect. It is possible that the bowler chose a non-optimal finger spread angle, but just got used to it over time. When increasing his finger-spread to a more optimal angle, he was unable to execute it, because he simply did not develop the motor pattern to do so. This effect is more pronounced in amateur athletes, but also occurs elite athletes, who could be performing better with more efficient techniques. An immediate change to the technique, even if demonstrably better, would initially lead to a diminished performance. Sometimes, the diminished performance is permanent if the motion pattern is too hard-wired to accept the technical change and perform effectively. While there was no optimum in the normalized precession, the best performance in the wide grip was seen in the precession, precession torque and its normalized Tp/ω. It is feasible that these parameters are influenced by the forcing apart of the two fingers in the wide grip, which stabilizes the wrist and finger movements. Consequently, the TR-vector is close to the ω-vector which keeps the precession torque and thus the precession to a minimum. This would support the general coaches recommendation that the ideal finger spread angle is as wide as comfortably possible. Precession and the associated precession torque are technical skill parameters. The smaller the precession torque, the higher is the expected spin rate. Consequently, the wider grip may result in a higher spin rate after a significant training period with the wide grip. Conflicts of Interest: The authors declare no conflict of interest. References 1. Fuss, F.K.; Doljin, B.; Ferdinands, R.E.D. Case studies of the centre of pressure between hand and ball in off-spin bowling, analysed with a smart cricket ball. Proc. Eng. 2016, 147, 203 207, doi:10.1016/j.proeng.2016.06.214. 2. Fuss, F.K.; Doljin, B.; Ferdinands, R.E.D.; Beach, A. Dynamics of spin bowling: The normalized precession of the spin axis analysed with a smart cricket ball. Proc. Eng. 2015, 112, 196 201. 3. Fuss, F.K.; Lythgo, N.; Smith, R.M.; Benson, A.C.; Gordon, B. Identification of key performance parameters during off-spin bowling with a smart cricket ball. Sports Technol. 2011, 4, 159 163, doi:10.1080/19346182.2012.726225. 4. Fuss, F.K.; Smith, R.M. Should the finger pressure be well distributed across the seam in seam bowling? A problem of precession and torque. Proc. Eng. 2013, 60, 453 458. 5. Fuss, F.K.; Smith, R.M. Accuracy performance parameters of seam bowling, measured with a smart cricket ball. Proc. Eng. 2014, 72, 435 440. 6. Fuss, F.K.; Smith, R.M.; Subic, A. Determination of spin rate and axes with an instrumented cricket ball. Proc. Eng. 2012, 34, 128 133. 7. Doljin, B.; Fuss, F.K. Development of a smart cricket ball for advanced performance analysis of bowling. Proc. Technol. 2015, 20, 133 137. 8. Fuss, F.K.; Doljin, B.; Ferdinands, R.E.D. Unpublished data, 2017. 2018 by the authors; Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).