Download presentation

Presentation is loading. Please wait.

1
**Hill model of force production**

Three element model Contractile Component Series Elastic Component Parallel Elastic Component Viscoelastic behavior Describe the three element model of force production Describe the behavior of each component during dynamic force production Implement a Hill-style model to predict force production

2
**Release experiments Two-phase response Elastic decline in tension**

Monotonic recovery Increasing length of release

3
Temperature Both development and recovery of tension are slower when cold

4
**Activation increases damping**

Set muscle vibrating on a spring Activate (b) Amplitude of vibration decreases

5
**Viscoelasticity Elasticity Viscosity Voigt-Kelvin (parallel)**

Force depends on length (F = k x) Viscosity Force depends on velocity (F= b v = b dx/dt) Voigt-Kelvin (parallel) Equal displacement; forces sum Maxwell (series) Equal forces; displacements sum

6
**Instantaneous response**

Length step dx/dt∞ viscous force ∞ Voigt (parallel) model fails Maxwell (series) model looks elastic Force step Voigt model looks viscous Maxwell model looks elastic

7
**Adaptation Creep Relaxation**

Under persistent force, viscous element lengthens Voigt: countered by rising elastic tension Relaxation Voigt model fails Maxwell spring pulls damper until force 0

8
**Length Step Maxwell Model Instantly elastic Relaxation Voigt Model**

Instantly immobile Steady-state elasticity dLd/dt = k(x-Ld)/b; F=k(x-Ld) F = kx + b(dx/dt)

9
**Force step Maxwell Model Instantly elastic Creep Voigt Model**

Instantly immobile Finite creep dL/dt = (dF/dt)/k+F/b dL/dt = (F-kL)/b

10
**Dynamic Response Maxwell Model: Length control**

Voigt Model: Force control First one is different Does not return to initial condition Out of phase

11
Standard Linear Solid Series spring isolates the Voigt construct from incompatible length changes “Best of both worlds” Viscous creep/relaxation Persistent force

12
**Three element model A.V. Hill (1922) H.S. Gasser & Hill (1924)**

Fibers as elastic tube Elastic myosin gel Viscous cytoplasm Elastic cell membrane/ECM Active state Contractile “stuff” with two rest lengths Time-dependent behavior from internal mechanics

13
**Hill’s activation & release**

Release resets CE balance Active state starts, CE reference length changes Instantaneous CE force resisted by damper Tension recovers to a lower level: force-length relationship Time course of tension rise and recovery don’t actually match in real muscle

14
**Cyclic stretches Viscoelastic model has short-range stiffness**

ie, matches Rack & Westbury’s nonlinear result

15
**Conceptual revisions There’s no actual viscous structure**

Phenomenological contractile element i.e.: curve fitting F = FL(x) * FV(v) Series elasticity: tendon (?) Parallel elasticity Epi-/peri-mysium? Titin? You can’t really match physical structures with a phenomenological model

16
**Application of Hill model**

Series & Parallel elastic elements Contractile element Activation, force-length, force-velocity F = a(t) * FL(x) * FV(v) 1.8 1.6 1.4 1.2 Force 1 Po 0.8 0.6 0.4 0.2 -0.5 0.5 1 Vmax Shortening Velocity

17
**Modeling Simulink Matlab Mathematica Excel 1 Force f(u) Sarcomere F-L**

Product SL*u/ML ML->SL F-V 3 Activation 2 Velocity Length Simulink Matlab Mathematica Excel

18
**Experimental measures**

Raw, isokinetic data Force-velocity/length curve Sandercock & Heckman 1997

19
**What is a modern “Hill model”?**

Phenomenological: curve fitting Extrapolation from Isometric force-length Isotonic force-velocity Extra features Activation dynamics (ECC) Short-range stiffness Nonlinearities

20
**Hill model + architecture**

Muscle is one big sarcomere Scaling LfVmax, L0 PCSAP0

21
**Complex simulation platforms**

SIMM (Musculographics) SimTK (NIH) Animatlab (GSU) Neuromechanic DADS (LMS) SimMechanics (Matlab)

22
**Model accuracy? One big sarcomere assumption**

Simulation of continuously changing velocity not so good One big sarcomere assumption Steady-state to dynamic assumption Estimation of force-length pretty good Winters et al., 2011 Perreault & al., 2003

23
**Summary 3-Element model Descriptive but practical**

Contractile element (active forces) Isometric force-length Isotonic force-velocity Series elastic element (transient dynamics) Parallel elastic element (passive forces) Descriptive but practical

Similar presentations

OK

PHYSIOLOGY 1 LECTURE 18 SKELETAL MUSCLE MECHANICS - MODEL.

PHYSIOLOGY 1 LECTURE 18 SKELETAL MUSCLE MECHANICS - MODEL.

© 2017 SlidePlayer.com Inc.

All rights reserved.

Ads by Google