2
Tukey’s test
Distance (m) 2.61
(0.22)
2.62
(0.29)
2.71
(0.28)
2.85
(0.30)
3.26* .214
SLJ > 1st, 2nd
Takeoff V
x
(m/s) 3.28
(0.13)
3.54
(0.31)
3.81
(0.20)
3.36
(0.17)
23.52* .662
3rd > 2nd > 1st, SLJ
Takeoff V
y
(m/s) 1.75
(0.19)
2.18
(0.27)
2.04
(0.32)
1.83
(0.28)
10.25* .461
2nd > 1st, SLJ;
3rd > 1st
Angle of takeoff (deg) 28.08
(3.08)
31.68
(3.76)
28.01
(3.84)
28.53
(3.62)
5.08* .298
2nd > 1st, 3rd, SLJ
Peak active GRF
x
(N) 778.7
(140.3)
611.6
(130.5)
615.9
(91.7)
789.3
(146.7)
48.46* .802
1st, SLJ > 2nd, 3rd
Peak active GRF
y
(N) 1431.7
(301.2)
2159.3
(391.2)
2137.7
(556.1)
1427.5
(311.5)
49.41* .805
2nd, 3rd > 1st, SLJ
*p < .05. Note: x - horizontal, y – vertical
The first and the second landing positions of
standing triple long jump were estimated by the
center of pressure of force platforms. The total
distance of standing triple long jump was decided by
the center of pressure of force platform 1 plus the
distance from tape measure. The distance of
standing long jump was quantified from the distance
of the center of pressure of force platform 1 and the
center of pressure of force platform 2-3. The vertical
and horizontal center of mass velocities were
estimated using the impulse method.
Repeated measures one way ANOVA with
Tukey’s post-hoc test were applied to examine the
differences in the kinetics and kinematics data
between jumps and landings (α = .05).
3 RESULTS
The analysis of reliability across trials showed the
distances of the first jump, the second jump, the
third jump, and the standing long jump were ICC
= .766, .628, .373, and .876, respectively. The ICCs
across trials of peak active vertical GRFs for each
jump were .889-.991, but the ICCs of peak active
horizontal GRFs for the first jump, the second jump,
the third jump, and the standing long jump
were .970, .884, .726, and .991, respectively.
There were significant differences in the jump
distances, F(3, 36) = 3.26, p = .032, η
2
= .214. The
Tukey’s post-hoc test showed the SLJ was longer
than the first and second jump of standing triple long
jump (table 1). The results of takeoff velocity
showed that the angle of takeoff at the second jump
was the greatest, F(3, 36) = 5.08, p = .005, η
2
= .298.
The statistical results of biomechanical parameters
are showed as Table 1.
4 DISCUSSION
The analysis of reliability showed the distances of
two jump trials of SLJ and the first jump of standing
triple long jump were consistency highly. But the
jump distance of consistencies were reduced during
the second and the third jumps of standing triple
long jump. It indicated that the standing triple long
jump is asked the utmost jumping movement
following two feet landing. The performer had to
adapt the landing impact following the process of
quite long flight, and it increased the variability of
movement to perform the takeoff movement
continually.
The distance of each jump of standing triple long
jump was 92-95% of the maximal SLJ. Although the
statistical analysis showed that the first and second
jumps were less than SLJ, and the distances of three
jumps were no differences. These indicated that the
most performers did not jump longer than the
maximal SLJ during every jump of standing triple
long jump. The initial impact peak in vertical GRFs
were 3.47 BW and 4.49 BW at the second (the first
landing) and third (the second landing) jumps,
respectively. Such higher load of impact force could
inhibit the mechanism of pre-stretch for leg
extensors; as a result, it explained the cause that the
consistency was decreased during the second and
third jump of standing triple long jump.
In conclusion, the results showed that the every
jump distance of standing triple long jump was only
the 0.92-0.95 times as the maximal standing long
jump. The performance of the third jump was less
consistent, because the continuous jump movement
of task constraint and the larger impact force during
landing.