Study record
Arrow flexing in free flight: Park 2011 study
Arrow behaviour in free flight
Citation
Park, J. L. (2011). Arrow behaviour in free flight. Proceedings of the Institution of Mechanical Engineers, Part P: Journal of Sports Engineering and Technology, 225(4), 241-252. https://doi.org/10.1177/1754337111398542
Cite the study
Park, J. L. (2011). Arrow behaviour in free flight. Proceedings of the Institution of Mechanical Engineers, Part P: Journal of Sports Engineering and Technology, 225(4), 241-252. https://doi.org/10.1177/1754337111398542
@article{park2011freeflight,
author = {Park, J L},
title = {Arrow behaviour in free flight},
year = {2011},
journal = {Proceedings of the Institution of Mechanical Engineers, Part P: Journal of Sports Engineering and Technology},
volume = {225},
number = {4},
pages = {241--252},
doi = {10.1177/1754337111398542}
}
Technical details
- Design
- Laboratory test
- Population
- Equipment tests, no archers
- What was tested
- Equipment, no participants
- Level
- Not stated
- Discipline
- Compound
- Type
- Journal article
- Language
- English
- Peer review
- Yes
- Published in
- Proceedings of the Institution of Mechanical Engineers, Part P: Journal of Sports Engineering and Technology
What it measured and what it found
Park modelled an arrow's flight in the horizontal plane as that of a flexible beam and compared it with real shots from a compound bow fired by a shooting machine. A Protour 470 with X vanes, leaving the bow at 78.9 m/s with an angle of -0.6 degrees and a rotation of -45 degrees per second about its centre of mass (the bow was set up on purpose to exaggerate the effect), swung about its centre of mass with a period of about 21.8 metres, or 0.28 seconds. The swing died away with a time constant of 0.34 seconds, about 25.8 metres of flight. Meanwhile the arrow flexed at 77.1 Hz, roughly once per arrow length travelled, and the heavy point strayed less than 3 mm from a straight line.
With Titeflight vanes 24% larger the period was 12% shorter, at 19.4 metres, and damping was stronger; even with the largest vanes in common use, 125 mm long, the model predicts that the arrow still swings before settling. Without vanes the arrow stayed stable but swung with a period of about 80 metres: at 15 metres the model placed it 44 mm right of the fletched version, and the machine put it 45 mm across. The accuracy test is the most interesting part: with the bow set to give a large lateral swing, or one of half that size, the machine's groups at 35 metres were the same, with every arrow inside a 15 mm circle.
How it was measured
The arrow is treated as an Euler-Bernoulli beam, flexible but inextensible, divided into 16 segments, with mass and stiffness varying along the shaft and the masses of nock, vanes and point lumped at the right places; the equations are solved by finite differences in steps of 0.05 ms. Lift and drag are calculated for point, shaft and vanes with coefficients from the aerodynamics literature (for the vanes, from a study of rowing blades). The initial conditions, meaning speed, angle, rotation and flex as the arrow leaves the bow, come from measurements; the measured initial drag was 0.93 times the arrow's weight.
For comparison the arrow was shot by a machine from an Archery Research AR34 through sheets of paper at several distances up to 35 metres, measuring the tear between point and vanes to about 2 mm; successive shots gave the same tear within 2 mm. Some compound archers from the Australian national team repeated the paper test at short range. Accuracy was assessed with machine groups at 35 metres at two different swing amplitudes.
The method explained: Shooting machines and robots in archery research
Limitations
The model is compared with a single arrow, in two vane configurations, and a single compound bow; what the author says about the recurve is a reasoned extension, not a test. Only the horizontal plane is covered, with no wind. The comparison with measurements is graphical, on paper tears, with no measure of agreement, and with the larger vanes the measured damping was a little stronger than calculated. The number of arrows in the groups is not given, and the finding of no difference holds within the machine's aiming precision and for swings repeated identically: it says nothing about an archer, whose error changes from one arrow to the next.
The tests with national team archers are described as broadly in agreement, without data, and the author himself does not rule out that they were twisting the bow. The estimate of errors of about 0.1 metres at 50 metres when the archer twists the bow comes from another paper by the same author.
What it means for archers
For anyone setting up a bow the study has two consequences. The first concerns paper tuning: since the arrow almost always leaves with a little rotation about its centre of mass and then swings with a period of about 20 metres, a tear read at a single distance can mislead. The author suggests looking at it at no fewer than two distances, about a quarter of a period apart, for example 1 and 6 metres. The second is that a lateral swing that is always the same, on a compound shot with a mechanical release, did not enlarge the machine's groups: in the author's view the lateral position of the rest is not critical, provided the arrow behaves the same way on every shot.
The focus therefore moves from the arrow to the archer: what opens up groups is variability, such as twisting the bow differently from shot to shot or the string touching the face, rather than a swing that repeats itself exactly. For the recurve the author notes that bare-shaft tuning works when the initial angle and rotation are small, but presents this as a question still to be studied.
In the registry
The claims this study is evidence for, with its position and the current status.
- ReportedVane type changes how quickly the arrow settles in flight (for)
- ContradictedAn arrow that oscillates less in flight groups more tightly (against, context)
- ReportedBeyond its first bending mode the arrow vibrates in higher modes, the second at about three times the first (context)
- ReportedIn flight the arrow oscillates in pitch, one cycle every fourteen to twenty-two metres, and the waviness shows mostly over the first stretch (for)
- CorroboratedAlong its flight the arrow loses an appreciable part of its launch speed (context)
- ReportedMeasured in a wind tunnel, the aerodynamic damping of the arrow's oscillation is negligible (context)
Articles that use it
Research line
Same research line
- 2011A miniaturised arrow ballistic measurement system
- 2011A10 Aerodynamic Properties of an Archery Arrow : JAXA's 60cm MSBS Experiments
- 2011Aerodynamic properties of an arrow: Influence of point shape on the boundary layer transition
- 2011Air flow around the point of an arrow
- 2011Minimizing wind drift of an arrow
- 2011The aerodynamic drag and axial rotation of an arrow
Cite this record
Campagna, M. (2026). Study record: Arrow behaviour in free flight. In Evidence Registry. matteocampagna.com. Retrieved 16 October 2026, from https://matteocampagna.com/en/evidence/park-2011-free-flight
@misc{campagna2026_enevidencepark2011freeflight,
author = {Campagna, Matteo},
title = {Study record: Arrow behaviour in free flight},
year = {2026},
howpublished = {Evidence Registry, matteocampagna.com},
url = {https://matteocampagna.com/en/evidence/park-2011-free-flight},
note = {accessed 2026-10-16}
}
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