Book contents
- Frontmatter
- Contents
- List of contributors
- Preface: shaping primate evolution
- 1 Charles Oxnard: an appreciation
- Part I Craniofacial form and variation
- Part II Organ structure, function, and behavior
- Part III In vivo organismal verification of functional models
- Part IV Theoretical models in evolutionary morphology
- 13 Becoming bipedal: how do theories of bipedalization stand up to anatomical scrutiny?
- 14 Modeling human walking as an inverted pendulum of varying length
- 15 Estimating the line of action of posteriorly inclined resultant jaw muscle forces in mammals using a model that minimizes functionally important distances in the skull
- Part V Primate diversity and evolution
- Index
- References
14 - Modeling human walking as an inverted pendulum of varying length
Published online by Cambridge University Press: 10 August 2009
- Frontmatter
- Contents
- List of contributors
- Preface: shaping primate evolution
- 1 Charles Oxnard: an appreciation
- Part I Craniofacial form and variation
- Part II Organ structure, function, and behavior
- Part III In vivo organismal verification of functional models
- Part IV Theoretical models in evolutionary morphology
- 13 Becoming bipedal: how do theories of bipedalization stand up to anatomical scrutiny?
- 14 Modeling human walking as an inverted pendulum of varying length
- 15 Estimating the line of action of posteriorly inclined resultant jaw muscle forces in mammals using a model that minimizes functionally important distances in the skull
- Part V Primate diversity and evolution
- Index
- References
Summary
Symbols and abbreviations
Ac axial (centripetal or centrifugal) acceleration of the mass
ΔC forward translation of the substrate contact point
COM center of mass
D instantaneous horizontal distance traveled by the mass since t = 0
Dh the total horizontal distance traveled by the mass during one swing of the inverted pendulum, i.e., the step length
f stride frequency
Fc centripetal force required to keep the mass on a circular path
GRFv vertical component of the ground reaction force
H instantaneous value of the height of the point mass (or COM)
H height of the point mass (or COM) at the middle of the first double-support phase
H height of the point mass (or COM) at the middle of the second double-support phase
H height of the point mass (or COM) at the middle of the single-support phase
ΔH maximum vertical excursion of the point mass (or COM) from MDS to MSS
I moment of inertia of the mass about the pivot point of the inverted pendulum
Lc the axially directed force exerted on the virtual stance limb (VSL) by the mass
-Lc the axially directed force exerted on the mass by the virtual stance limb (VSL)
M mass
MDS middle of double-support phase
MSS middle of single-support phase
R the length of the virtual stance limb (from substrate contact-point to the point mass or its surrogate) at any moment in time
R length of the virtual stance limb at MDS
R length of the virtual stance limb at MSS
S stature
t time
t half the duration of the swing of the inverted pendulum
V velocity of the mass
Vc axial (centripetal or centrifugal) velocity of the mass
Vo orbital (tangential) velocity of the mass
[…]
- Type
- Chapter
- Information
- Shaping Primate EvolutionForm, Function, and Behavior, pp. 297 - 333Publisher: Cambridge University PressPrint publication year: 2004
References
- 1
- Cited by