| Literature DB >> 30719007 |
Daniel Link1, Marcus Weber1, Daniel Linke1, Martin Lames1.
Abstract
This study explores whether positioning systems are a viable alternative to timing gates when it comes to measuring sprint times in ice hockey. We compared the results of a single-beam timing gate (Brower Timing) with the results of the Iceberg optical positioning system (Optical) and two radio-based positioning systems provided by InMotio (Radio 1) and Kinexon (Radio 2). The testing protocol consisted of two 40 m linear sprints, where we measured sprint times for a 11 m subsection (Linear Sprint 11), and a shuttle run (Shuttle Total), including five 14 m sprints. The exercises were performed by six top-level U19 field players in regular ice hockey equipment on ice. We quantified the difference between measured sprint times e.g., by Mean Absolute Error (MAE) (s) and Intra Class Correlation (ICC). The usefulness of positioning systems was evaluated by using a Coefficient of Usefulness (CU), which was defined as the quotient of the Smallest Worthwhile Change (SWC) divided by the Typical Error (both in s). Results showed that radio-based systems had a higher accuracy compared to the optical system. This concerned Linear Sprint 11 (MAEOptical = 0.16, MAERadio1 = 0.01, MAERadio2 = 0.01, ICCOptical = 0.38, ICCRadio1 = 0.98, ICCRadio2 = 0.99) as well as Shuttle Total (MAEOptical = 0.07, MAERadio1 = 0.02, MAERadio2 = 0.02, ICCOptical = 0.99; ICCRadio1 = 1.0, ICCRadio2 = 1.0). In Shuttle Total, all systems were able to measure a SWC of 0.10 s with a probability of >99% in a single trial (CUOptical = 4.6, CURadio1 = 6.5, CURadio2 = 5.1). In Linear Sprint 11 an SWC of 0.01 s might have been masked or erroneously detected where there were none due to measurement noise (CUOptical = 0.6, CURadio1 = 1.0, CURadio2 = 1.0). Similar results were found for the turning subsection of the shuttle run (CUOptical = 0.6, CURadio1 = 0.5, CURadio2 = 0.5). All systems were able to detect an SWC higher than 0.04 s with a probability of at least 75%. We conclude that the tested positioning systems may in fact offer a workable alternative to timing gates for measuring sprints times in ice hockey over long distances like shuttle runs. Limitations occur when testing changes/differences in performance over very short distances like an 11 m sprint, or when intermediate times are taken immediately after considerable changes of direction or speed.Entities:
Keywords: on-ice test; performance analysis; positioning systems; smallest worthwhile change; sports analytics; timing gates; validation
Year: 2019 PMID: 30719007 PMCID: PMC6349073 DOI: 10.3389/fphys.2018.01882
Source DB: PubMed Journal: Front Physiol ISSN: 1664-042X Impact factor: 4.566
FIGURE 1Visualization of test setting and segments Linear Sprint 11 (A), Linear Sprint 21 (B), Shuttle Sprint (C), and Shuttle Turn (D). Shuttle Run Total is given as the concatenation of all Shuttle Sprints and Shuttle Turns. The Figure shows the original trajectory of one athlete measured simultaneously by each EPTS.
Results of accuracy testing for each RUN and EPTS.
| RUN × EPTS | N | ME | MAE | MXE | TE | CV | LOA | ICC | R |
|---|---|---|---|---|---|---|---|---|---|
| Optical | 12 | −0.16 | 0.16 | −0.19 | 0.01 | 1.2 | [−0.2 to −0.12] | 0.38 | 0.97 |
| Radio 1 | 12 | ∼0 | 0.01 | −0.03 | 0.01 | 0.7 | [−0.04 to 0.03] | 0.96 | 0.98 |
| Radio 2 | 12 | −0.01 | 0.01 | −0.02 | 0.01 | 0.7 | [−0.03 to 0.02] | 0.96 | 0.99 |
| Optical | 6 | −0.07 | 0.07 | −0.12 | 0.02 | 0.1 | [−0.13 to −0.01] | 0.99 | 0.97 |
| Radio 1 | 6 | 0.01 | 0.02 | 0.04 | 0.01 | 0.1 | [−0.03 to 0.05] | 1.0 | 0.97 |
| Radio 2 | 6 | ∼0 | 0.02 | 0.05 | 0.02 | 0.1 | [−0.05 to 0.06] | 1.0 | 0.96 |
| Optical | 29 | −0.12 | 0.12 | −0.16 | 0.02 | 0.8 | [−0.16 to −0.07] | 0.55 | 0.99 |
| Radio 1 | 29 | 0.05 | 0.05 | 0.1 | 0.02 | 1.2 | [−0.01 to 0.11] | 0.86 | 0.99 |
| Radio 2 | 29 | −0.04 | 0.04 | −0.12 | 0.02 | 1.2 | [−0.1 to 0.02] | 0.89 | 0.99 |
| Optical | 23 | 0.12 | 0.12 | 0.17 | 0.02 | 0.7 | [0.08 to 0.17] | 0.80 | 1.0 |
| Radio 1 | 23 | −0.06 | 0.06 | −0.11 | 0.02 | 0.7 | [−0.11 to −0.02] | 0.94 | 1.0 |
| Radio 2 | 23 | 0.05 | 0.05 | 0.09 | 0.02 | 0.8 | [−0.01 to 0.1] | 0.96 | 1.0 |
FIGURE 2Visualization of accuracy for each trial and each EPTS according to Bland-Altman. The plots show Measurement Error (E) over SPRINT TIMEMean (mean of sprint time measured by EPTS and timing gate) as well as Mean Error (ME, solid colored line) and Lines of Agreement (LOA, dashed colored line) (all in s). Negative values indicate shorter EPTS sprint times compared to the timing gate.
Indicators for evaluating the usefulness of tested EPTS.
| RUN | SPRINT TIME | SWC | CUOptical | CURadio1 | CURadio2 |
|---|---|---|---|---|---|
| Linear Sprint 11 | 1.45 ± 0.05 | 0.01 | 0.6− | 1.0# | 1.0# |
| Linear Sprint 21 | 2.63 ± 0.08 | 0.02 | 1.1# | 2.0+ | 2.0+ |
| Shuttle Total | 19.15 ± 0.48 | 0.10 | 4.6+ | 6.5+ | 5.1+ |
| Shuttle Sprint | 1.90 ± 0.10 | 0.01 | 0.6− | 0.5− | 0.5− |
| Shuttle Turn | 2.41 ± 0.18 | 0.01 | 0.6− | 0.6− | 0.5− |
FIGURE 3Course of players x-coordinate (in m) over time (in s) during Shuttle Run measured simultaneously by each EPTS. The enlarged segments show when the player passes the measurement line of the timing gates at the end of the Shuttle Turn (A), the end of the Shuttle Sprint (B), and when reaching the turnover moment in the third Shuttle Turn (C). Total SPRINT TIME for this Shuttle Run measured by the timing gates was 19.41 s (SPRINT TIME Optical = 19.30 s, SPRINT TIME Radio 1 = 19.43 s, SPRINT TIME Radio 2 = 19.37 s).