First published online February 29, 2008
Journal of Experimental Biology 211, 945-956 (2008)
Published by The Company of Biologists 2008
doi: 10.1242/jeb.006692
High-speed gallop locomotion in the Thoroughbred racehorse. II. The effect of incline on centre of mass movement and mechanical energy fluctuation
K. J. Parsons*,
T. Pfau,
M. Ferrari and
A. M. Wilson
Structure and Motion Laboratory, The Royal Veterinary College, University
of London, North Mymms, Hatfield, Hertfordshire AL9 7TA, UK

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Fig. 1. Examples of experimental records at 10 m s–1 (A,C,E) and
12 m s–1 (B,D,F) for horse 1. Red represents incline data and
blue represents level data. Craniocaudal acceleration (A,B), craniocaudal
velocity (C,D) and craniocaudal displacement (E,F) of the trunk for strides
recorded at each speed are presented and the figure demonstrates the
integration procedure. Acceleration data is integrated to provide velocity
data and displacement data for each stride. LF=lead fore; NLF=non-lead fore;
LH=non-lead hind; NLH=non-lead hind.
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Fig. 2. Displacement range (A), minimum and maximum velocity (B) and minimum and
maximum acceleration (C) from 8 m s–1 to 12 m
s–1 for dorsoventral (left) and craniocaudal (right) movement
on the level (blue triangles) and incline (red circles) for the six horses.
For each speed category mean ± 1 s.e.m. (displacement) or median and
interquartile range (velocity and acceleration) are calculated from all
strides. A linear function was fitted to the data and is shown as a red solid
line (incline data) and a blue broken line (level data).
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Fig. 3. Displacement range (A), minimum and maximum velocity (B) and minimum and
maximum acceleration (C) from 8 m s–1 to 12 m
s–1 for pitch (left column) and heading (right column) on the
level (blue triangles) and incline (red circles) for the six horses. For each
speed category mean ±1 s.e.m. (displacement) or median and
interquartile range (velocity and acceleration) are calculated from all
strides. A linear function was fitted to the data and is shown as a red solid
line (incline data) and a blue broken line (level data).
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Fig. 4. Stride data (mean ± s.e.m. as shading, N=6) of the sum of
the vertical kinetic (KEdv) and linear potential energy
(PE) during level (blue broken line) and incline (red solid line)
galloping at a mean speed of (A) 10 m s–1 (n
level=56 and n incline=60) and (B) 12 m s–1
(n level=60 and n incline=28). Presented data are averages
of all strides from all horses within the speed range. Aerial phases (vertical
grey bar) were estimated to be during the time when the curve was
approximately constant. Stance phases of individual feet are presented for
illustrative purposes as black bars in the lower panels. LF=lead fore;
NLF=non-lead fore; LH=non-lead hind; NLH=non-lead hind.
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Fig. 5. Stride data (mean ± s.e.m. as shading, N=6) of changes in
craniocaudal kinetic (KEcc) energy during level (blue
broken line) and incline (red solid line) galloping at a mean speed of (A) 10
m s–1 (n level=56 and n incline=60) and (B)
12 m s–1 (n level=60 and n incline=28).
Presented data are averages of all strides from all horses within the speed
range. For illustrative purposes the minimum craniocaudal kinetic energy has
been subtracted from external mechanical energy. Estimated aerial phase
(vertical grey bar); stance phases of individual feet are presented for
illustrative purposes as black bars in the lower panels (LF=lead fore;
NLF=non-lead fore; LH=non-lead hind; NLH=non-lead hind).
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Fig. 6. Stride data (mean ± s.e.m. as shading) of changes in total potential
energy (PE) during level (blue broken line) and incline (red solid
line) galloping at a mean speed of (A) 10 m s–1 (n
level=56 and n incline=60) and (B) 12 m s–1
(n level=60 and n incline=28). Aerial phase (vertical grey
bar); stance phases of individual feet are presented for illustrative purposes
as black bars in the lower panels (LF=lead fore; NLF=non-lead fore;
LH=non-lead hind; NLH=non-lead hind). Note s.e.m. shading is not clearly
visible as the standard errors are small.
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Fig. 7. Stride data (mean ± s.e.m. as shading) of changes in total linear
mechanical energy MElin(CoM) during level (blue broken
line) and incline (red solid line) galloping at a mean speed of (A) 10 m
s–1 (n level=56 and n incline=60) and (B)
12 m s–1 (n level=60 and n incline=28). For
illustrative purposes the minimum total energy has been subtracted from
external mechanical energy. Estimated aerial phase (vertical grey bar); stance
phases of individual feet are presented for illustrative purposes as black
bars in the lower panels (LF=lead fore; NLF=non-lead fore; LH=non-lead hind;
NLH=non-lead hind).
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Fig. 8. Linear mechanical work Wlin(CoM) (A), Linear mechanical
cost MCTlin(CoM) (B), rotational mechanical work
Wrot (C), rotational mechanical cost MCTrot
(D), linear + rotational mechanical work Wlin(CoM)+rot (E)
and linear + rotational mechanical cost MCTlin(CoM)+rot (F) for six
galloping horses on the level (blue triangles) and incline (red circles) at a
speed range of 8 m s–1 to 12 m s–1. For each
speed category values are mean ±1 s.e.m. (N=6) for individual
horses. A linear function was fitted to the data and is shown as a red solid
line (incline data) and a blue broken line (level data).
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Fig. 9. Negative linear work ( )
(percentage of total linear work) as a function of gradient. A linear
regression line (red) has been fitted to the data.
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© The Company of Biologists Ltd 2008