RELATIONSHIP BETWEEN KINETICS OF COUNTERMOVEMENT JUMP AND PROXIMAL MECHANICS OF COLLEGIATE BASEBALL PITCHING �Motoki Sakurai, Mu Qiao, David J. Szymanski, & Ryan L. Crotin
Department of Kinesiology, Louisiana Tech University, Ruston, LA
INTRODUCTION
METHODS
RESULTS
Nineteen collegiate baseball pitchers (age = 19.9 ± 1.5 yr, height = 186.5 ± 5.9 cm, body mass = 90.7 ± 13.8 kg, % body fat = 14.6 ± 5.2%) volunteered for this study. Signed informed consent was obtained from all participants. The research study was approved by the university’s IRB.
Two data collections took place that included pitching motion capture and recording bilateral CMJ kinetics. Twelve motion capture cameras tracked the whole-body movement and 2 force plates recorded ground reaction force (GRF) from each leg in both tests. In the pitching test, participants were asked to throw 5 fastballs for strikes on a custom-made mound from the stretch position. In the CMJ test, participants performed at least 3 CMJs or until they failed to achieve a greater jump height after the third trial. Jump kinetics and pitching kinematics data were compared based on the differences in throwing velocity and total linear momentum in the anterior-posterior (AP) direction, respectively. The medians for throwing velocity (fast and slow) and AP linear momentum (high and low) of participants were identified to divide them into two groups in each analysis.
CONCLUSIONS
Inefficient proximal mechanics (pelvis and trunk) in baseball pitching encourages greater throwing arm effort in achieving high ball velocities where very few studies have evaluated the influence of leg power on pelvis and trunk motion (2). Powerful lower body mechanics may enable more efficient trunk mechanics and momentum transfer to provide optimal force transfer to throw at high velocity. With effective force transfer generated from the legs to the throwing arm via proximal segments, throwing arm effort may be lowered (1, 4). The countermovement jump (CMJ) is a valid and reliable test that assesses an athlete’s ability to develop force and power output from lower body (3, 4). Pitchers who demonstrate powerful CMJ ability may be able to produce greater force in their lower body to provide efficient proximal mechanics and momentum transfer while pitching that encourage high ball velocity outcomes. However, the relationship between force/power output in the CMJ and pitching mechanics remains unclear. The purpose of this study was to identify how CMJ kinetics influence proximal mechanics in the baseball pitching motion with a focus on momentum transfer.
REFERENCES
PRACTICAL APPLICATION
Variable Name | p value | d | Fast | Slow |
Throwing velocity (m∙s-1) | <0.001* | 0.41 | 37.7 ± 0.8 | 35.6 ± 0.5 |
Peak trunk angular velocity (deg∙s-1) | 0.19 | 0.09 | 812±93 | 877±118 |
Peak pelvis angular velocity (deg∙s-1) | 0.79 | 0.004 | 589±267 | 560±217 |
Separation time (ms) | 0.32 | 0.05 | 26±20 | 18±17 |
Separation angle at SFC (deg) | 0.42 | 0.03 | 36±11 | 44±28 |
AP linear momentum (kg∙m·s-1) | 0.06 | 0.16 | 99±15 | 82±20 |
ML linear momentum (kg∙m·s-1) | < 0.001* | 0.33 | 16±5 | 7±5 |
Transverse angular momentum (kg∙m2∙rad·s-1) | 0.01* | 0.22 | 7±1 | 5±2 |
Absolute peak vertical GRF (N) | 0.01* | 0.22 | 2450±254 | 2080±352 |
Normalized peak vertical GRF (BW) | 0.99 | <0.001 | 2.56±0.261 | 2.56±0.443 |
Absolute peak power (W) | < 0.001* | 0.34 | 7690±731 | 5840±1120 |
Normalized Peak power (W∙N-1) | 0.15 | 0.10 | 8.06±1.13 | 7.2±1.41 |
Eccentric RFD (N·s-1) | 0.79 | 0.004 | 750±428 | 796±339 |
Concentric impulse (N·s) | 0.54 | 0.02 | 617±233 | 563±134 |
Take off velocity (m∙s-1) | 0.30 | 0.06 | 2.35±0.43 | 2.56±0.46 |
RSImod (m∙s-1) | 0.37 | 0.04 | 1.1±0.40 | 1.26±0.39 |
Stride leg peak force compensation | 0.77 | 0.01 | 0.009±0.04 | 0.01±0.04 |
Variable Name | p value | Fast | Slow |
Height (m) | 0.288 | 1.88±0.05 | 1.85±0.06 |
Body mass (kg) | 0.01* | 98.08±9.07 | 83.86±13.91 |
Lean body mass (kg) | 0.005* | 82.4±82.0 | 71.8±70.6 |
Table 1. Differences in kinematics and momentum profiles in pitching and kinetics in CMJ across throwing velocity groups.
Table 2. Height, body mass, and lean body mass differences across fast velocity and slow velocity groups.
Figure 1. Pitching motion capture
Figure 2. CMJ evaluation
Variable Name | p value | d | High M | Low M |
AP linear momentum (kg∙ m·s-1) | <0.001* | 0.39 | 105±11.4 | 76.6±10.4 |
Throwing velocity (m∙s-1) | 0.27 | 0.06 | 37.1±1.11 | 36.5±1.38 |
Peak trunk angular velocity (deg∙s-1) | 0.07 | 0.14 | 796±80 | 880±112 |
Peak pelvis angular velocity (deg∙s-1) | 0.47 | 0.03 | 608±312 | 530±125 |
Separation time (ms) | 0.75 | 0.006 | 24±22 | 22±14 |
Separation angle at SFC (deg) | 0.36 | 0.05 | 44±29 | 35±10 |
ML linear momentum (kg∙m·s-1) | 0.3 | 0.06 | 14±8 | 10±4 |
Transverse angular momentum (kg∙m2∙rad·s-1) | 0.04* | 0.28 | 7±1 | 5±2 |
Absolute peak vertical GRF (N) | 0.045* | 0.17 | 2420±292 | 2100±355 |
Normalized peak vertical GRF (BW) | 0.35 | 0.05 | 2.47±0.317 | 2.63±0.406 |
Absolute peak power (W) | 0.12 | 0.11 | 7340±1070 | 6370±1530 |
Normalized peak power (W∙kg-1) | 0.53 | 0.02 | 7.53±1.24 | 7.92±1.46 |
Eccentric RFD (N·s-1) | 0.73 | 0.007 | 809±459 | 750±290 |
Concentric impulse (N·s) | 0.02* | 0.22 | 684±226 | 487±54.4 |
Take off velocity (m∙s-1) | 0.43 | 0.03 | 2.43±0.42 | 2.57±0.42 |
RSImod (m∙s-1) | 0.10 | 0.12 | 1.05±0.45 | 1.34±0.30 |
Stride leg peak force compensation | 0.70 | 0.01 | 0.01±0.04 | 0.003±0.04 |
Table 3. Differences in kinematics and momentum profiles in pitching and kinetics in CMJ across high and low anterior-posterior linear momentum.
Table 4. Height, body mass, and lean body mass differences across high and low anterior-posterior linear momentum (M) related to throwing velocity.
Variable Name | p value | High M | Low M |
Height (m) | 0.04* | 1.89±0.05 | 1.84±0.56 |
Body mass (kg) | 0.001* | 100.18±8.18 | 82.29±12.15 |
Lean body mass (kg) | <0.001* | 83.8±8.6 | 70.8±7.6 |
Results are shown in the tables. Significant p-value was set below 0.05 for all the variables examined in this study. Table 1 and 3 presents Cohen’s d effect size calculations.