models of terrestrial locomotion: from mice to men… to elephants? justus d. ortega dept. of...
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Models of Terrestrial Locomotion:Models of Terrestrial Locomotion:From Mice to Men…From Mice to Men…
to Elephants?to Elephants?
Justus D. Ortega
Dept. of KinesiologyHumboldt State University
What do all these animals have in
common?
Locomotion• Complex interaction of the neuromuscular and
musculoskeletal systems• Comes in many forms:
oBipedal: oWalkoRunoSprinto Hop
oQuadipedaloWalkoTrotoGallop
• How do we study something so complex?
Today we’ll discuss models of locomotion
for walking and running/hopping
•Whole body level- mechanics1. Ground reaction force2. Movement and mechanical energy of
CoM3. Behavioral models of walking and
running
Basic patterns in walking and running
Walking- Double support: two feet on ground- Single support: One foot on ground
Running-Stance phase: one foot on ground-Aerial phase: no ground contact
Ground reaction force
•Force exerted by the ground on the feet
•Greatly affect energetics of motion
Ground reaction force in walking
Running Ground Reaction Force
Center of MassMotion
Center of mass- balance point of body
Center of MassMotion
Walking Running
WalkVelocity decreasesHeight increases
Velocity increasesHeight decreases
RunVelocity decreases Height decreases
Velocity increasesHeight increases
Mechanical Energy of Center of Mass
Mechanical Energy- Energy of an object related to its motion
Two primary forms: Kinetic: energy in motion
Potential: stored energy-Gravitational- elastic
Kinetic energy (Ek,t)
m = massv = velocityk = kinetic, t = translational
m
Ek,t = 0.5 mv2
v
Gravitational potential energy (Ep,g)
mg = weight of object
ry = vertical position of object
Ep,g = mgry
ry
mg
Elastic energy: energy stored when a spring is stretched or
compressed
Stretched(Energy stored)
Rest length(no energy stored)
Compressed(Energy stored)
Spring
Mechanical energy in walking
Some kinetic energySome gravitational potential energyLittle work done against aerodynamic dragUnless slipping, no work done against friction
Not much bouncing (elastic energy)
Mechanical energy fluctuations in level walking
Average Ek,t constant (average vx constant)
Average Ep,g constant (average ry constant)
HOWEVEREk,t and Ep,g fluctuate within each stance
Mechanical Energy in Walking
Mid-stance
KE minimized at mid-stanceand GPE maximized at mid-
stance
Walking and Mechanical energy
•1st half of stance: decrease Velocity & increase HeightoKE converted to GPE
•2nd half of stance: increase Velocity & decrease HeightoGPE converted to KE
•KE and GPE are out of phase
Alexander (1992)
Vertical motion allows mechanical energy
exchange
Walking as Inverted Pendulum
Kineticenergy
Gravitational Potential
Energy
Totalenergy
Time (s)
Single support phase
Perfect Inverted Pendulum
Total
GPE
KE
Time (s)0.0 0.2 0.4 0.6
DS SS
0.2 J/kg
Work
(Ortega and Farley, J. Applied Physiology, 2005)
60-70% of mechanical energy is conserved
Mechanical energy exchange and the cost of
walking
Metabolic Cost of Transport (mlO2/kg/km)
Speed (m/s)1.00.5 1.5 2.0
80
120
160
200
Mechanical Energy
Exchange (%)
70
60
40
50
30
Effect of body size on mechanical
energy recovery
As increase size, greatest recovery at faster speeds, but similar amount
11-12 years
3-4 years
Cavagna, 1983
Mechanical Energy in Running
KE and GPE minimized at mid-stance
Mid-stance
KE (J)
GPE (J)
TotalEnergy (J)
Time (s)
Stance phase of running
But what about EE?
Running: Spring mechanism
•Ek,t & Ep,g are in phase. Elastic energy is stored in leg.
Leg stiffness
•Ratio of peak force to maximum displacement
Blickhan, 1989
Animals maintain same leg stiffness across many
speeds
Farley et al., 1993
How do we do it?
Effect of speed on leg spring
As speed increases….-Peak force increases-Compensate with greater angular excursion = CoM disp.
Leg stiffness
and speed in variety of
running animal
Leg Angle Stiffness
Speed (m/s) Speed (m/s)Farley et al., 1993
Leg stiffness is proportional to body mass
Animals can adjust leg stiffness for different
surface stiffnesses
Animal adjust leg stiffness so CoM
movement is same
Ferris & Farley, 1983
Running Robots ?
Using spring mass model to improve
performance
Alt video
Why is it so hard to walk on the moon?
How did dinosaurs walk and run?
Thank you