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Saturday, June 27th, 2009<br />

Scheiber P, Krautgasser S, Von Duvillard SP et al (2009) Physiological responses <strong>of</strong> older recreational alpine skiers to different skiing<br />

modes. Europ Journal <strong>of</strong> Applied Physiology, 105(4), 551 - 558.<br />

Seifert J, Kroell J, Mueller E (2008) The Relationship <strong>of</strong> Heart Rate and Lactate to Cumulative Muscle Fatigue during Recreational Alpine<br />

Skiing. Journal <strong>of</strong> Strength & Conditioning Research. In Press.<br />

THE RELATIONSHIP BETWEEN THE TIMING OF TAKE-OFF ACTION AND FLIGHT LENGTH BY USING TWO DIFFERENT<br />

TYPES OF JUMP-DOLLS<br />

SASAKI, T., TSUNODA, K., HOSHINO, H., MIYAKE, S.<br />

HOKUSEI GAKUEN UNIVERSITY<br />

Introduction: The purpose <strong>of</strong> this study is to detect the optimal timing <strong>of</strong> jump action in ski jumping. Assuming a jumper could always<br />

produce same motions, the timing <strong>of</strong> jump action would be the most important variable for the flight distance. In this study, the jump <strong>of</strong><br />

the two different jump-dolls were observed on the hill model (1/100). Dolls always produce same power during jump action. Thus, the<br />

flight distance solely depends on the timing <strong>of</strong> initiating the action. Therefore, it is possible to clarify the relationship between the timing<br />

and the flight distance.<br />

Methodology: Two different types <strong>of</strong> jump-dolls were developed. First doll was used two springs for producing s<strong>of</strong>ter power. Four springs<br />

were set in respective joints (knees and hips) <strong>of</strong> the second types <strong>of</strong> the doll. The jump doll can reproduce the same hopping action on<br />

the take-<strong>of</strong>f platform. The critical point (K) in the model <strong>of</strong> jumping hill is 160 cm. The dolls are able to jump on this model hill. The position<br />

<strong>of</strong> start on in-run is 150 cm away from the edge <strong>of</strong> platform. The peg, which releases the strength <strong>of</strong> the jump doll, was put on six places<br />

every 4 cm away from the edge <strong>of</strong> platform. Five times trials in two jump dolls were executed for every peg point. All the jump actions<br />

were recorded by the NAC video camera with 500 fps.<br />

Results: The elapsed time for jump actions from squat position to full extension and speed <strong>of</strong> take-<strong>of</strong>f were almost the same in both types.<br />

Using the same release point, the maximum flight distance was occurred in each doll. The release point is 4 cm before the edge <strong>of</strong><br />

platform. The flight distance is 125 cm in type 1, and 166 cm in type 2. On the other hand, the minimum flight distance was observed in<br />

initiating jump action at the 12 cm before the edge. The flight distance is 88 cm in type 1, and 128 cm in type 2.<br />

Discussion: Smooth action on each joint is achieved by a bearing devices, although the doll is made by wood, The doll-model produces<br />

the same strength at take-<strong>of</strong>f actions, because, it is possible to take the same squat position anytime. Therefore, the jump -doll can be<br />

used in the experiment <strong>of</strong> ski-jump. In this study, the difference in the flight distance is only attributed by the difference <strong>of</strong> the timing <strong>of</strong> the<br />

jump action. As an evidence <strong>of</strong> the transition <strong>of</strong> the power, the oscillation <strong>of</strong> skis was exactly observed during the initial flight phase. This<br />

phenomenon already pointed out even in the human action (Sasaki et al., 2005). In the flight distance, the most effective timing for beginning<br />

the action is clarified in this experiment by the jump-doll.<br />

Conclusion: Until the 4 cm from the edge <strong>of</strong> platform, the later the timing <strong>of</strong> beginning the action is, the larger the flight distance is. The<br />

jump-doll always transmits almost same power.<br />

OPTIMIZATION OF AERODYNAMIC STABILITY IN SKI JUMPING: THE TUG-OF-WAR BETWEEN SAFETY AND PERFORM-<br />

ANCE<br />

MARQUES-BRUNA, P., GRIMSHAW, P.<br />

EDGE HILL UNIVERSITY<br />

Introduction: Past research in ski jumping has aimed to increase jump length and modify ski length and hill design to make the <strong>sport</strong><br />

safer (Schwameder, 2008). However, the assessment <strong>of</strong> aerodynamic stability (Anderson, 2007) for improved safety has received less<br />

attention (Seo et al., 2004). Thus, this study aimed to model aerodynamic efficiency and stability in pitch in ski jumping as a function <strong>of</strong><br />

athlete’s posture. The findings may be used to optimise flight posture and warrant safer training and competition.<br />

Methods: Mathematical modelling was carried out using a hypothetical ski jumper with a typical mass <strong>of</strong> 70 kg, height <strong>of</strong> 1.76 m and ski<br />

length <strong>of</strong> 2.57 m (Seo et al., 2004). Lift (FL), drag (FD), lift/drag ratio (FL/FD), dPitching-moment/dAngle-<strong>of</strong>-attack slope (dM/dAA) at the trim<br />

AA and oscillatory frequency (FREQ) (Anderson, 2007) were calculated as a function <strong>of</strong> AA, ski opening angle (SOA; at 20°, 25° and 30°)<br />

and forward-leaning angle (FLA; at 0°, 10°, 20°, 30° and 40°) (Seo et al., 2004). Air density was set at 1.18 kg/m3, and air speed at 25 m/s<br />

to simulate competition at a large jumping hill (Schwameder, 2008).<br />

Results: FL was largest with SOA = 30° & FLA = 0°-10°. FD increased monotonically from AA = 10°. FL/FD peaked at AA = 2°-12°, at which<br />

FL was rather low. dM/dAA became steeper with increased SOA and FLA, ranging from – 0.82 Nm/° for SOA = 20° & FLA = 0° to – 2.67<br />

Nm/° for SOA = 30° & FLA = 40°. FREQ increased as a function <strong>of</strong> SOA and FLA, showing about half a cycle per second (0.51 Hz) for SOA =<br />

30° & FLA = 10°.<br />

Discussion/Conclusion<br />

An optimised flight posture <strong>of</strong> SOA = 30° & FLA = 10° is suggested. This is a high-lift configuration that yields steep dM/dAA and high<br />

oscillatory frequency upon sudden deviations from trimmed flight. The high frequency may initiate transitory dynamic oscillations (Anderson,<br />

2007). The findings add to the current priority to warrant safety in the <strong>sport</strong> (Schwameder, 2008).<br />

References<br />

Anderson, J.D. (2007). Fundamentals <strong>of</strong> aerodynamics. (4th ed.). McGraw-Hill. London.<br />

Schwameder, H. (2008). Biomechanics research in ski jumping, 1991-2006. Sports Biomechanics. 7 (1): 114-136.<br />

Seo, K., Watanabe, I. and Murakami, M. (2004). Aerodynamic force data for a V-style ski jumping flight. Sports Engineering. 7: 31-39.<br />

PHYSIOLOGIC RESPONSES OF LOW AND HIGH STRESS RESPONDING RECREATIONAL ALPINE SKIERS TO DIFFERENT<br />

SKIING PACES<br />

SEIFERT, J., SCHEIBER, P., MÜLLER, E.<br />

MONTANA STATE UNIVERSITY, BOZEMAN, MONTANA; UNIVERSITY OF SALZBURG, SALZBURG, AUSTRIA<br />

Introduction: Previous studies have demonstrated that there are skiers who demonstrate a low physiological response (LO; low lactate<br />

and HR), while others have a high physiological response (HI; high lactate and HR) when skiing at similar velocities. However, it is unknown<br />

how LO and HI respond to different skiing paces when compared to their individual self-paced skiing. It is important to understand<br />

OSLO/NORWAY, JUNE 24-27, 2009 499

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