Chapter 3 joint and materials mechanics
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Artificial hips. Chapter 3 - Joint and Materials Mechanics. Shoe impact tester. Joint Motion. Anatomical Position Planes Sagittal Frontal Transverse. Mobility and ROM. ROM joint & person specific Injuries: excessive ROM Factors affecting ROM:

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Chapter 3 joint and materials mechanics

Artificial hips

Chapter 3 - Joint and Materials Mechanics

Shoe impact tester


Joint motion
Joint Motion

  • Anatomical Position

  • Planes

    • Sagittal

    • Frontal

    • Transverse


Mobility and rom
Mobility and ROM

  • ROM joint & person specific

  • Injuries: excessive ROM

  • Factors affecting ROM:

    • Shape and geometry of articulating surfaces

    • Joint capsule and ligaments

    • Surrounding muscles

    • Apposition of body parts

  • Joint Stability


Lever systems
Lever Systems

R

F

  • Rigid rod fixed at point to which two forces are applied

  • 1st class

  • 2nd class

  • 3rd class

  • Functions

    •  applied force

    •  effective speed

F

R

R

F


Instantaneous joint center
Instantaneous Joint Center

  • Caused by asymmetries in the joint motion

  • Basic movements

    • rotation

    • sliding

    • rolling


Moment of force joint motion
Moment of Force & Joint Motion

  • Moment = F ·d

  • Moment = muscular activity, essential for controlling joint motion

  • Theory: actions at joints can be represented by the resultant joint force and the resultant joint moment


Resultant joint force vs bone on bone forces
Resultant Joint Force vs Bone-on-Bone Forces

  • RJF: Net force across the joint produced by bone, ligaments, muscle etc.

  • Bone-on-Bone: more complex calculation


Material mechanics
Material Mechanics

  • Rigid body mechanics: body segments are considered rigid structures (non-deformable)

    • fixed center of mass

    • homogeneous material

  • Used to analyze movements

  • Easier to model and provide a reasonable approximation


Deformable solids
Deformable solids

  • Segment or tissue analyzed undergoes deformation

  • More complicated analysis and difficult to model


Material properties
Material Properties

  • Basic properties

    • Size

    • Shape

    • Area

    • Volume

    • Mass

  • Derived

    • Density

    • Centroid


Stress
Stress

  • Stress (): internal resistance to an external load

    • Axial (compressive or tensile) =F/A

    • Shear  = F/A (parallel or tangential forces)

  • Units Pascal (Pa) = 1Nm2

Axial

Shear


Strain
Strain

  • Change in shape or deformation ()

  • Absolute strain

  • Relative strain

    • L/Lo


Stress strain
Stress &Strain

  • Stress-strain ratio: stiffness or compliance of the material

    • E = / 

  • Linear material

    • Hooke’ law:  = E· 

  • Biological material non-linear due to its tissue fluid component (viscoelastic properties)

A

B


Uniaxial loading
Uniaxial Loading

E

  • Simplest form: forces applied along single line typically the primary axis

    • compressive

    • tensile

    • shear

  • Stress-strain curve

    • Linear region (B)

    • elastic limit (C)

    • yield point (D)

    • ultimate stress (E)

    • Rupture (F)

    • Energy stored (area)

D

F

C

B


Poisson s effect
Poisson’s effect

Force

  • When a body experiences an uniaxial load its axial & transverse dimensions will change,

  • v = -(t/ a)


Multiaxial loading
Multiaxial Loading

  • Deformation in all three directions

  • Net effect of the strains

  • Shear stresses


Bending
Bending

  • Long bones: beams

  • Compressive stress: inner portion

  • Tensile stress: outer portion

  • Max stresses near the edges, less near the neutral axis

T

C

axis

axis

y

x=(Mb·y)/I


Bending moments
Bending Moments

  • Shear stresses max at neutral axis and zero at the surface

  •  = (Q·V)/(I ·b)

  • Q= area moment

  • V= vertical shear force

Q

y

h

b


Bending1
Bending

  • Three point bending

    • failure at middle

    • ski boot fracture

  • Four point bending

    • failure at the weakest point between two inside forces


Bending2
Bending

  • Cantilever bending

  • Compressive force acting off-center from long axis


Torsion
Torsion

  • Twisting action applied to a structure

  • Resistance about long axis determined by polar moment of inertia

  • J=[·(r4o-r4i)]/2

  • Shear stress along the shaft =(T·r)/J

  • Twist angle: =(T·l)/(G·J)


Torsion1
Torsion

  • Larger radius of the shaft, greater resistance

  • Stiffer the material harder to deform

  • In addition to shear stress, normal stress (tensile & compressive) are produced in a helical path (spiral fractures)

r


Viscoelasticity
Viscoelasticity

  • Provided by the fluid component in biological tissue

  • Resistance to flow

  • Affects stress-strain

  • Increase in strain rate produces-increases stiffness of the material


Viscoelasticity1
Viscoelasticity

  • Pure elastic material

    • strain energy returned

    • no energy loss

  • Viscoelastic tissues

    • lose energy due to heat

    • energy is not returned immediately

    • Resilient

    • Dampened

  • Hysteresis: area representing energy lost

Elastic

Load

Non

unload


Viscoelasticity2
Viscoelasticity

creep

  • Creep response

  • Stress-relaxation response

  • Effects of strain-rate on stress relaxation

Time


Material fatigue failure
Material Fatigue & Failure

Initial cycle effect

  • Fatigue: repeated loads above a certain threshold

  • Continued loading: failure

  • First cycle effect: shift in mechanical response

1

2

3

n


Material failure
Material failure

  • Distribution of stresses

    • Discontinuity (stress risers)

      • fractures sites

      • screws

      • osteotendinous junctions

  • Ductile vs Brittle materials

  • Failure theories

    • maximal normal stress

    • maximal shear stress

    • maximal energy distortion


Biomechanical modeling simulation
Biomechanical Modeling & Simulation

  • Model: representation of one or more of an object’s or system’s characteristics using mathematical equations

  • Goal

    • improve understanding of a system

  • Simulation:process of using validated model


Biomechanical modeling simulation1
Biomechanical Modeling & Simulation

  • Physical model: simulates actual conditions, crash test dummies

  • Mathematical or computer model: conditions are represented using mathematical equations


Why use a model
Why use a model?

  • Easy to duplicate

  • Easy to make change in the system

  • Time

  • Economic factor


How to select a model

What questions is being posed?

Type: molecular, tissue, organ etc.

Deformable or rigid

finite or continuoum

static, quasi static or dynamic

Linear or nonlinear

2D or 3D

Determined or stochastic

kinematics or kinetics

inverse or direct

How to select a model?


Model simulations
Model & Simulations

  • Models are simplifications of actual situations

  • Model and simulation are as good as the data use as input

  • Stability of the model (range of values)


Finite element modeling
Finite-element modeling

  • Structures are represented as simple blocks assembled to form complex geometrical structures

  • Connected at poinst (nodes) forming a mathetical representation of the structure

  • Forces are applied at the structure and stress and strain are predicted

  • Complex and requires a great deal of computing power



Rheological models
Rheological Models

  • Study of deformation and flow of matter

  • Use to model biological tissue

  • Interrelate stress, strain, and strain rate

  • Three types

    • Linear spring

    • dashpot

    • frictional

  • Linear spring

    • elastic properties of tissue


Rheological models1
Rheological Models

  • Dashpot

    • loading response that is strain rate dependent

    • fluid viscosity (newtonian fluid)

    •  = ·

  • Frictional element

  • Combinations of models

Strain rate


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