Download - Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

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Page 1: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits and jumpiness.• Recap: gaits and ballistic walking

• When the Froude Number (V2/g L) is greater than 1, simple ballistic walking is no longer possible.

• More aspects of jumping (energy and force)

• The jumper model accounts for an airborne phase of movement.

• Calculating optimal gaits for energy expenditure

Page 2: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits and jumpiness.

Page 3: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion
Page 4: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

Review of walking

Matthis & Fajen, 2013

How much energy input is needed for walking?

Page 5: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

Energy tradeoffs in walking and running

What’s different?

KE

PE

KE

PE

elastic potential energy

Page 6: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

A model for running:the spring-loaded inverted pendulum (SLIP)

BBC

tendons are springy!

Page 7: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

The jumper: for speeds greater than Fr = 1, gait must change with an airborne phase

Spring Loaded Inverted Pendulum

Page 8: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

Goal: compute the power (rate of energy expenditure) as a function of size (M,m) and gait (jumpiness)

M

m

h

d

VAssume constant Vno air resistanceno skidding

j = (1-β)/β

Maynard-Smith Mathematical Ideas in Biology

L

βL (1-β)L

Page 9: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

Goal: compute the power (rate of energy expenditure) as a function of size (M,m) and gait (jumpiness)

M

m

h

d

j = (1-β)/β

Maynard-Smith Mathematical Ideas in Biology

L

βL (1-β)L

V

Energy to launch? = (M +m)g (h+d) Energy to break the fall? Energy to move the foot?

γ= (M +m)g (h+d) {-1 < γ < 1}= mV2/2

Page 10: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

= (1+γ )(M +m) + mV2/2 g2 L2(1-β) 8V2

Goal: compute the power (rate of energy expenditure) as a function of size (M,m) and gait (jumpiness)

M

m

h

d

j = (1-β)/β

Maynard-Smith Mathematical Ideas in Biology

L

βL (1-β)L

V

Total Energy

Page 11: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

= (1+γ )(M +m) + mV3/ (2 L) g2 L(1-β) 8V

Goal: compute the power (rate of energy expenditure) as a function of size (M,m) and gait (jumpiness)

M

m

h

d

j = (1-β)/β

Maynard-Smith Mathematical Ideas in Biology

L

βL (1-β)L

V

Total Power

= (1+γ )(M +m) + mV3/ (2 Lβ(1+j)) g2 Lβj 8V

Page 12: Lecture 4. Terrestrial locomotion III: mechanical analysis of gaits …courses.washington.edu/biomechs/lectures/lecture04.pdf · 2016. 10. 4. · Lecture 4. Terrestrial locomotion

How does Power vary with foot mass (m)?body mass (M)?body velocity (V)?jumpiness (j)?

P

0 inf.

= (1+γ )(M +m) + mV3/ (2 Lβ(1+j)) g2 Lβj 8VTotal Power

dP/dj = 0 —> Max, Min, inflection….