how to improve your technique with ... - rowing ireland · 6 the highest amount of energy 93% is...
TRANSCRIPT
1
www.biorow.com
1
How to improve your technique
with biomechanics
Dr. Valery Kleshnev
Rowing Science Consultant
BioRow Ltd.
www.BioRow.com
Joy of Sculling 21st Annual Conference
Saratoga, December 12-15th, 2013
www.thejoyofsculling.com
2
www.biorow.com
Basic chart of Rowing Biomechanics
Medal
Work capacity
(Physiology)
Technique
(Biomechanics)
Motivation
(Psychology)
Life Style
(Management)
Efficiency = Pout / PinputEffectiveness = Pmax - Wmin
Rowing Style /
Rower’s Efficiency
Blade
Efficiency
Dynamics of
the system
Boat
EfficiencyRowing
Power
Segments’
Velocities RiggingForce
Curve
Boat Velocity
& Acceleration
Standards(Stroke Rate,
Length, Force)
Performance Level
Analysis Level
Measurement Level
Vertical Oar
Angle
From: Kleshnev V. Rowing Biomechanics Newsletter 2011/10 &
2011. Rowing Biomechanics. In: Rowing Faster, the 2nd ed., ed. Nolte V. Human
Kinetics
4
How we define rowing technique efficiency?
The three main parts of rowing as a process of
energy transformation
Propulsive PowerBlade
Propulsive
Efficiency
Minimal required Power
Boat Velocity
Efficiency
Mechanical Power
Internal
(muscle)
Efficiency
5
Efficiencies of the components of energy
transformation process during rowing
Internal Muscle
Efficiency 24±4%
O2
Handle power
Blade Propulsive
Efficiency 82±5%
Handle power
Propulsive power
Boat Velocity
Efficiency 94.5±1%
Boat Velocity
Drag Power
0%
10%
20%
30%
40%
50%
60%
70%
80%
90%
100%
Efficiency (%)
6
The highest amount of energy 93% is lost in the
rower’s body.
The Rower is the main area to improve rowing
efficiency.
1667
Total energy
consuming
400
Handle Power
328
Propulsive
Power
310
Minimal
Required Power
93.4%
5.3% 1.3%
Internal LossesBlade Shift Losses
Velocity Fluctuation Losses0
400
800
1200
1600
2000
Power (W)
Amounts and Losses of
energy in rowing
(example values)
www.biorow.com
How can we increase the rower’s efficiency
and effectiveness?
Using of the most powerful muscle groups;
Optimisation muscles contraction velocities;
No energy absorption, single-motion movement;
Decreasing of muscles-antagonists activity;
Muscles relaxation during recovery phase.
8
What are Rowing Biomechanics “Gold Standards”?
Pprop = DF * V3
P = Pprop / Eblade
L = Inb. * A
WPS = P * (60 / Rate)
Fav = 0.83 * WPS / L
EventG.St.
TimeP (W) Inb. (m) Rate (1/min)
Angle
(deg)Fav (N) Fmax (N)
W1x 07:11.5 400 0.89 33.0 110 371 713
W2x 06:39.5 400 0.88 35.0 110 354 680
W4x 06:08.5 400 0.87 37.0 110 339 651
W2- 06:52.9 400 1.16 37.0 90 334 641
W8+ 05:53.1 400 1.15 39.0 92 313 601
M1x 06:32.5 550 0.89 35.0 114 464 892
M2x 06:02.1 550 0.88 37.0 114 444 854
M4x 05:33.2 550 0.87 39.0 114 426 820
M2- 06:08.5 550 1.16 38.0 90 447 859
M4- 05:41.0 550 1.15 40.0 92 419 806
M8+ 05:18.6 550 1.14 40.0 94 414 797
LW2x 06:47.0 330 0.88 35.0 106 303 583
LM2x 06:07.2 470 0.88 37.0 110 393 756
LM4- 05:46.2 470 1.15 40.0 90 366 704
Category W (kg) P (W) Erg Score (m:s)
Open Women 85 400 6:23
Open Men 95 550 5:44
LW Women 60 330 6:48
LW Men 70 470 6:03
9
Input of body segments into rowing power
Legs produce nearly half of
rowing power;
Trunk produces nearly one
third of rowing power;
Arms produce about one
fifth of rowing power;
Arms, 22.70%
Trunk, 30.90%
Legs, 46.40%
15%
20%
25%
30%
35%
40%
45%
50%
20 25 30 35 40
Legs
Trunk
Arms
Power Shares (%)
Stroke Rate (str/min)
Legs increase their
percentage of power with
increasing stroke rate;
Arms’ power share
decreases, when the
stroke rate increases.
10
This tells us that the largest
capacity for increasing
rowing power can be found
from utilization of the trunk
work-capacity.
Utilisation of work-capacity of the body
segments Legs use up to 95% of their
power.
Trunk muscles utilize only
about 55%;
Arms’ utilization is about
75%;
(Kleshnev V. 1991)
Legs,
95%Trunk,
55%
Arms,
75%
0%
10%
20%
30%
40%
50%
60%
70%
80%
90%
100%
Utilisation (%)
11
Velocity-Force dependence for isolated
muscle (Hill principle)
Hyperbolic relationship between velocity and force was discovered in the 1920s by Archibald Vivian Hill from a study of frog muscles.
A number of recent researches confirmed that it can be valid for complex multi-joint movements.
The highest power can be achieved at 1/3 of max. static force and 1/3 of max. voluntary velocity.
0%
50%
100%
150%
-40% -20% 0% 20% 40% 60% 80% 100%
0%
25%
50%
75%
100%
F
P
Force (%)
Velocity(%)
Power (%)
F = b1 / (b0 + V)
P = F VMax.
Power
Lengthening<->Shortening
www.biorow.com
Utilisation of the Hill principle in rowing
Negative power is the most inefficient unless it happens during very short
time.
Too heavy or too light gearing can affect the force/velocity relationship and
thus efficiency.
An optimal body sequence, (i.e. rowing style) matched to the rower’s
characteristics and boat speed plays the most significant role in
rowing efficiency.
-2
-1
0
1
2
3
-60 -45 -30 -15 0 15 30 45
Total
Legs
Trunck
Arms
V (m/s)
-2
-1
0
1
2
3
-60 -45 -30 -15 0 15 30 45
Total
Legs
Trunck
Arms
V (m/s)
13
How we measure velocities of body segments?
Cable position transducers are attached to the seat and top of the trunk (at the level L7-Th1 vertebra or sternum-clavicle joints);
Arms velocity is calculated as a difference between handle velocity (derived from oar angle and inboard) and trunk velocity.
14
What effective dynamics means?
Front-loaded drive, trampoline effect;
Quick acceleration of the rower’s mass first, then
taking the load;
Emphasis on the stretcher push, “catch through
the stretcher”;
Smooth “fat” force curve, control through
suspension from the seat;
Using rower’s inertia for propulsion at finish, “finish
through the handle”.
15
www.biorow.com
How the front-loaded drive looks like? It is important to
increase force
quickly up to 70% of
maximum;
“Trampolining”
effect?
1. Front-loaded 1. Middle-loaded
1
2
Drive
Force/Body mass (N/kg)
R3-D1 D2 D3 D41
2
Boat
Acceleration
1
2
Boat Velocity
16
www.biorow.com
Why the front loaded-drive is more effective?
Front-loaded drive (F1):
Gives 47% higher average
velocity and distance
travelled during the drive;
Creates much more even
distribution of the power;
Provide better utilization of
the most powerful muscle
groups
Hydro-lift force on the blade
can be used better.
0
2
4
6 F1F2F3
Force (N)
0
5
10
15
V1
V2
V3
Velocity (m/s)
0
20
40
60
80P1P2P3
Power (W)
0
20
40
60 P1P2P3
Distance
travelled (m)
FA
17
How can we analyse the Force Curve?
Catch gradient defines how quickly the force increases;
Position of the Peak Force defines emphasis of force
application;
Finish gradient defines how long the force maintained.
0%
20%
40%
60%
80%
100%
0% 20% 40% 60% 80% 100%
Norm.Oar Angle (% to total)
Normalized Force (% of Max.)
70% of Max.
Catch
Gradient Finish
Gradient
Position of
Peak Force
18
How the Target Force Curve looks like?
Solid, front-loaded, full, no “humps” or glitches.
Catch gradient 10% of the Total Angle (11 deg in sculling, 9 deg in rowing);
Position of the Peak Force 33% of Total Angle (down to 30% in 8+ and 4x, up to 38% in 1x);
Finish gradient 32% (up to 36% in big boats, down to 26% in small boats).
0%
20%
40%
60%
80%
100%
0% 20% 40% 60% 80% 100%
Norm.Oar Angle (deg)
Normalized Force (% of Max.)
70% of Max.Force
19
How can we present the Force Curve?
Force vs. time (s) is good for
synchronisation with other
variables, but difficult to
compare at various stroke
rates;
Force vs. time (% of stroke
cycle) is another option;
Force vs. Oar Angle allows
easy comparison at various
stroke rates and useful for
defining position of specific
points (peaks, gaps).
-100
0
100
200
300
400
500
600
700
800
0.0 0.5 1.0 1.5 2.0 2.5
212529333739
Time (s)
Handle Force (N) Stroke Rate (1/min)
-100
0
100
200
300
400
500
600
700
800
0% 20% 40% 60% 80% 100%
212529333739
Time (% of cycle)
Handle Force (N) Stroke Rate (1/min)
-100
0
100
200
300
400
500
600
700
800
-75 -50 -25 0 25 50
21
25
29
33
37
39
Oar Angle (deg)
Handle Force (N) Stroke Rate (1/min)
20
Why the stretcher force is positive?
1. Drive phase must be emphasised, because
the system velocity increases only during the
drive;
2. During the drive, acceleration of the rower’s
mass must be emphasised, because it is the
main “accumulator” of the kinetic energy;
3. The stretcher force must be emphasised,
because this is the only force, which
accelerated the rower’s centre of mass;
21
Why accelerate the rower’s mass during the drive?
Kinetic energy of the system
increases ONLY during the
drive phase;
Kinetic energy of the system
decreases during the recovery
phase and we can not change
it;
Amount of kinetic energy, which
the system gained during the
drive phase, determines
average velocity of the system;
Rower’s mass is the main
“accumulator” of the kinetic
energy;
0
500
1000
1500
2000
2500
3000
Rowers
Boat
System
Drive
Kinetic Energy (J)
T (s)
D boat
D rowers
Ek = (m v2) / 2
Steve Fairbairn (1930):
“Find out how to use your
weight and you will have
solved the problem of how
to move the boat”
22
Power transfer though the stretcher
In rowing the power is transferred through BOTH
handle and stretcher in the proportion about
60/40%
Squat: power transfer through upper body only
Legs press: power transfer through the foot-stretcher only
P = F * v
23Analogy with canoeing makes it easier to
understand why the stretcher force is important
Action Forces
Reaction Forces
Centre
of Mass
Force
Transfer
1. Athlete apply
action forces
2. Action forces
create opposite
reaction forces
3. Reaction forces
move centres of mass
24
How blade propulsive efficiency is defined?
Propulsive Power
P propulsive = F V mass centre
F
Vm.c.Vm.c.
F
Eblade = P propulsive / P total = (P - P waste) / P
Waste Power
F
V
P waste = F V
F V
25
Handle
Pin
Blade
DriveRecoveryRecovery
Oar Track during stroke cycle
26
What we need to know about blade efficiency?
Hydro-lift force works at sharp angles of attack and contributes 56% of the blade propulsive force;
Drag force works at the middle of the drive and contributes 44% of the blade propulsive force.
How can we increase the blade propulsive efficiency?
Use bigger blade area;
Use heavier gearing;
Utilise hydro-lift effect -> apply more
force at sharp oar angles at catch;
Place the blade at the optimal depth
under the water (4-6 deg).70%
80%
90%
100%
-75 -50 -25 0 25 50
Blade
Efficiency (%)
Oar Angle (deg)
50
100
150
Flift
Fdrag
Fblade total
Force (N)
30
60
90
Angle of attack (deg)
1
2
3
4
5
Vblade
Vboat
Velocity (m/s)
27
Oar blade as a jet engine? At the start of runway, the
efficiency of a jet plane is zero, because its velocity is zero, but the thrust and specific impulse are maximal.
As the plane accelerates, its efficiency increases, and became 100%, if the plane speed is equal to the speed of exhaust gasesExhaust Speed
Propulsion
Isp = (Vg – V) m / t
E= 2 / (1 + Vg / V)
28Specific Impulse as a measure of the blade
performance?
The specific impulse can be used together with blade efficiency for evaluation of the blade work.
A higher specific impulse is generated at a lighter gearing ratio, but at a lower handle velocity at the same time.
This could be achieved either by using bigger blade area, or by more effective thrust production using a better shape and/or utilisation of hydro lift effect.
Power (W)
0
500
1000
1500
0
100
200
300
Thrust
Force (N)
Oar Angle
(deg)
0.1
0.2
-75 -50 -25 0 50
Blade specific impulse
Isp (s/m)
25
1
2
3
-1
1
2
-5
0
5
10Handle
Velocity
Vert.angle
Isp = Ftrust / Prow
Isp = (Lin / Lout) cos(α) / Vh
29
How we analyze rower’s blade work?
Two-dimensional (2D) sensor measures oar angles horizontal and vertical planes, which allows to define a path of the blade relative to water.
Criterion -3 deg was chosen to indicate full immersion of the blade into the water.
- 6
0
3
- 50 - 25
Vertical Angle (deg)
Catch Slip
Release Slip
Water Level
Recovery
Effective Angle
Catch Finish
3
Drive
Target Curve
Horizontal Angle (deg)
30
Rotational motions of the oar.
Rotational motions of the oar were measured with BioRow 7Dwireless sensor;
The most understandable and informative measured variable appeared to be the roll Gx, which is clearly related to the squaring-feathering of the oar.
Angular
Velocities
+ -
Roll
Pitch
+-
Yaw
+
Gx
Gy
Gz+Ay
+Ax
+Az
Accelerations
-10
-5
0
5
Ax
Ay
Az
Oar Accelerations (m/s2)
Catch
Finish
-200
0
200
400
600
0.0 0.5 1.0 1.5 2.0
Gx
Gy
Gz
Oar Rotations
(deg/s)
Drive0
100
200
300
0.0 0.5 1.0 1.5
-5
0
5
Force
Vertical AngleForce (N)
Time (s)
2
1
3
31
When the blade squared – feathered?
The squaring takes 0.25-
0.35s and completed at the
catch, when the oar change
direction, but the blade is still
in the air.
The feathering began, when
the centre of the blade
crosses the water level and
completed in about 0.15-
0.25s – faster than squaring;
The higher the stroke rate,
the longer distance of
recovery is required to square
the blade.
-400
-200
0
200
400
600
-75 -50 -25 0 25 50
20.430.0
35.037.0
Oar Roll Velocity Gx (deg/s)
Stroke
Rate
Catch Finish
Drive
Recovery
0
20
40
60
80
-75 -50 -25 0 50Oar Angle (deg)
Oar Roll
Angle
(deg)
SquaringFeathering
-0.5
0.5
-2.0 -1.0 0.0 1.0
Horizontal Position (m)
Vertical
Position (m)Water level
Catch slipFinish slip
Squaring
With BioRowTel system, the oar roll
data in conjunction with horizontal and
vertical oar angles allows a full
reconstruction of the oar movements
relative to the water level.
32
Determination of “Boat velocity efficiency”
The main reasons for energy losses are:
•boat velocity fluctuation;
•non-linear dependence of drug power on velocity
Pdrag = k V3
Propulsive power
Drag Power
Boat Velocity
Drag Power
V
F
P = kV3
F = kV2
33
Boat speed during recovery The hull speed increases
through recovery at higher stroke rates.
The higher the rate, the closer the peak speed to the catch.
The reason for this is in interaction of the rower’s and the boat masses.
The transmission of the kinetic energy from the rower’s mass is to the hull occurs during recovery by means of pull through the foot-stretcher.
At the higher rating the pull force exceeds 200N and overcomes the drag force ≈100N at the hull.
-1.5
-1.0
-0.5
0.0
0.5
1.0
20
26
30
35
37
Angle
Hull velocity rel. average (m/s)
CatchDrive
Release
Recovery
-400
-200
0
200
400
600
800
1000
20
26
30
35
37
Foot-stretcher Force (N)
ReleaseCatch
Drive
Recovery
Angle
-2
-1
0
1
HullRower CMSystem CM
Velocity rel. Average (m/s) Rate 37
Release
Catch
Drive
RecoveryRecovery
34Variations of the boat velocity is NOT the
main reason of the energy losses in rowingThere are two main reasons
of the variation of the boat velocity:
Periodical production of the propulsive force;
Movement of the rower’s mass relative to the boat shell.
We can not change these factors without changing the nature of rowing
Increase of the boat velocity during recovery caused by transfer of KINETIC ENERGY from the rower’s mass to the boat.
-6
-4
-2
0
2
4
RowerBoatSystem
Accelerations (m/sTime
0
200
400
600
Force (N)
Catch Release
Recovery Drive Recovery
-2
-1
0
1
BoatRower CMSystem CM
Velocity rel. Average (m/s)
Release
Catch
Drive
RecoveryRecovery
Time
Time
35
How can we help to optimize rigging?
Rigging Calculator www.biorow.com/RigChart.aspx
www.biorow.com
35
Thanks to Ian Wilson of Concept2 UK for the idea and
Dick & Peter Dreissigacker of Concept 2 for support.
36
What we can measure in rigging?Why rigging is important?
Oar dimensions define
gearing, which determines
force/velocity ratio of
rower’s muscles
contraction;
Stretcher position is
related to ratio of
catch/finish angles;
Gate height and blade
pitch defines vertical oar
angles;
Stretcher angle and
height defines lift force and
kinetics of the drive.www.biorow.com
36
Spread (sweep)
Gate Height
Height from water
Heels Depth
Span (sculling)
Overlap (sculling)
Overlap (Sweep)
Stretcher
Angle
Work through
Pitch
Seat Travel
Gate Height
Stretcher position
SlidesAngle
37
What is correct definition of the Gearing?
The standard definition of the
gearing is the ratio of
velocities (or displacements,
travels) of output to input;
In rowing, velocity of the
output is defined by actual
outboard, input – by actual
inboard;
The span/spread does NOT
affect gearing;
Blade efficiency or “slippage”
DOES affect Gearing.
www.biorow.com
37
Gearing = Actual Outboard / Actual Inboard
= (Out.-SL/2- SW/2) / (Inb.-Hnd/2+SW/2)
Blade Travel
Handle Travel
Oar LengthInboard
PinActual Inboard
Oar LengthInboard
Actual OutboardPin
38
Is gearing constant during the drive?
At sharp oar angles only part of
blade velocity is parallel to the
boat velocity;
Effect of the oar angle is small
until 45deg;
Gearing ratio became twice
heavier at the oar angle 60deg;
Gearing ratio became three
times heavier at the oar angle
70deg;
Gearing ratio became six times
heavier at the oar angle 80deg;
The most common catch angles
are between 55deg (sweep)
and 70deg (sculling).
0
1
2
3
4
5
6
7
8
9
10
11
12
0 10 20 30 40 50 60 70 80
Dynamic Gearing Ratio
(Outboard/Inboard)
Oar Angle (deg)
G(a) = G/cos(a)
Handle Velocity
Blade Velocity
Boat Velocity
39
1987
1988
1992
2001
2011
Our history force measurements in rowing
1998
Instrumented gates
Oar bend sensors
Handle
Oar Shaft Insert
Strain Gauges
“+” “-“
2002
2005
Stretcher
Force
sensors
2001
2005
Seat Force
sensor 2002
2005
2012
2011 Wireless
40
What is measured with force transducers?
Handle Force gives the most accurate power measures, but require calibration of every oar.
Gate force require inboard for power calculation, which could vary during the drive ±5%;
Pin Force is affected by oar angle and axial force, so power could me measured with ±20% accuracy.
Peach Inn. Ltd.
Our gates,
WEBA gate
Handle
Force
Our sensors, FES sensor
Pin Force Gate
Force
Axial Force
41
What Biomechanical Tools we use? BioRowTel v4.5 telemetry system
was created by rowing scientist
for research purposes. It is
accurate, flexible, scalable, based
on “screening” concept, quick to
setup, light;
Scalable design: one “Master”
unit + up to 8 “Slaves”;
Master unit contains:
GPS and impeller input for boat
speed;
3D accelerometer, 3D gyro;
Wind speed & direction input;
Sampling frequency 25-100 Hz;
Resolution 14 bit;
Works >8 hours;
Weight 300g.www.biorow.com
41
“Master” unit “Slave” unit
42
www.biorow.com
42
Thank you for attention
Dr. Valery Kleshnev
Rowing Scientist
e-mail: [email protected]
Rowing Biomechanics Newsletter www.biorow.com
www.biorow.org