BioMech - Biological Materials ch. 9

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47 Terms

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External Forces impose loads

External forces on a body affect motion

External forces also load a body and affect internal structures

  • Cartilage, ligaments, tendons, bones, muscle


Mechanical response of structures are related to injury


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Mechanics of Materials

Considers segment to be a deformable body, not rigid

External forces imposed are resisted by internal forces and cause deformation

  • external applied load: stress

  • Deformation caused: strain


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Mechanical Stress

How an applied force is distributed over the body it acts on

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Mechanical stress equation

σ=FA\sigma=\frac{F}{A}

σ\sigma = stress

F = Internal force (N)

A = Cross-sectional area of the internal surface (m²)

  • Units: N/m² (Pascal)


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Internal force (F)

The force is the resultant of the many intermolecular bond forces across the imaginary cut plane

  • F in the stress equation


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Key feature of Mechanical stress

The amount of area the force is applied to:

Larger muscle harder to tear

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Cross-Sectional Area

The cross-sectional area of the imaginary plane is the area over which the internal force is applied

  • A in the stress equation


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Types of Mechanical Stress

3 principal stresses depending on applied loading

  • Tension

  • Compression

  • Shear


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Axial Stress

external forces act perpendicular to the analysis plane

  • Also call normal or longitudinal stress


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Uniaxial load

external forces are colinear

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Tensile stress

  • an axial or normal stress

  • occurs at the analysis plane as a result of a force or load pulling the molecules apart at that plane

  • Tension causes body to deform by stretching (elongating)


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Tension: Bone cross section

Bone cross-sectional area depends on plane of analysis

  • Larger cross-sectional area: lower stress

  • Small cross-sectional area: higher stress


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Compression

Compressive stress

  • an axial or normal stress

  • occurs at the analysis plane as a result of a load squeezing the molecules together at that plane

  • compression causes body to deform by shortening


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Compression: Bone cross-section

Bone cross sectional area

  • larger cross-sectional area: lower stress

  • smaller cross-sectional area: higher stress


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Shear

Shear stress

  • a transverse stress

  • acts parallel to the analysis plane as a result of non-colinear forces sliding molecules at that plane

Shear causes body to deform by skewing
- changes orientation of the sides of the object

shear stress represented with τ\tau

  • τ\tau =shear force / area


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Tension Injury

Sprains (rupture) ligament and tendon

Strains (tear) muscle and cartilage

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Compression injury

Bruises soft tissue

crushing fracture of bone

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Shear injury

Blister on skin

Dislocation of a joint

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Mechanical Loading

When external forces are not uniaxial, more complex loading occurs

  • Bending

  • Torsion

  • Combined loads


Complexity of loading reflects

  • Number, direction & location of external forces

  • Shape of object


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Bending

Bending load

  • nonaxial loading

  • Tension and compression produced at the analysis plane from 3 or more forces create force couples at ends of object

    • tends to rotate ends of body in opposite direction

  • Bending loads cause body to deform by curve (bending)

    • One side squeezed

    • One side stretched


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Torsion

Torsion load

  • nonaxial loading

  • shear stress acts parallel to the analysis plane as a result of opposing torques applied about the long axis of the body

  • torsion causes body to deform by twisting

    • Shear stress from torsion load increases with greater distance from axis

Tubular and hollow cross-section of bones resists torsion

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Combined Loading

Human bones under complex loading from gravity, tendons, ligaments, other bones, contact forces

  • sustained loading a combination of

    • tension, compression, simple shear loads, bending, torsion


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Strain

Quantifies the material’s deformation

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Linear strain

change in an object’s length

  • deformation produced by tensile or compressive stress


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Shear Strain

change in orientation of an object’s molecules

  • Deformation produced by shear stress

Reported as change in angle of perpendicular plane

Δθ\Delta\theta
Unit: Radians

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Linear Strain mathematically

ε=(l−lo)lo\varepsilon=\frac{\left(l-l_{o}\right)}{l_{o}}

ε\varepsilon = linear strain

ll = stretched length

lol_{o} = original, undeformed length

l−lol-l_{o} = change in length

Units: dimensionless

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Poisson’s Ratio

Width of an object also changes as it lengthens or shortens
When lengthened = wide ; When shortened = narrow

Ratio = (Axial strain) / (Transverse strain)

range: 0.1 to 0.5

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Stress-Strain Relationship

Behavior of material under load

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Elastic Behavior

Material deforms and returns to original length when unloaded

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Plastic Behavior

Material deforms but doesn’t return to original length

  • permanent deformation


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Elastic Modulus (E)

Slope of the stress-strain curve

E=ΔσΔεE=\frac{\Delta\sigma}{\Delta\varepsilon}

Also known as Young’s modulus

  • Bulk modulus: slope describing compressive loading

  • Shear modulus: Slope describing shear loading


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Elastic Modulus & Materials

Stiff material: less strain per unit of stress (Large E)

Pilant material: more strain per unit of stress (low E)

  • Bone is stiffer than ligaments or tendons

  • Tendons and ligaments are more pilant than bone


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Mechanical strength of a material

Maximum stress a material can withstand before failure

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Elastic limit

The yield point for a material on the σε\frac{\sigma}{\varepsilon} curve

  • stress above this point causes permanent deformation of material


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Yield strength

Stress at the elastic limit

  • Disruption of internal organization, material does not regain shape


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Ultimate strength

maximum stress material can withstand

  • Material starts to give way


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Failure strength

Stress level where total failure occurs

  • Breakage or complete rupture of the material occurs


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Failure strain

Strain exhibited when a total failure occurs

  • Ductile material: exhibits large failure strain

    • Deforms a lot before giving way (ligament)

  • Brittle material: exhibits a low failure strain

    • Deforms minimally before giving way (bone)


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Toughness

The ability of a material to absorb energy before failure

  • ligaments and tendons are tougher than bone


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Connective Tissue

Components of the MS system exhibit different properties

  • Muscle: active element of connective tissue

  • passive elements of connective tissue

    • Bone, cartilage, ligament, tendon


Properties of collagen and elastin vary in connective tissue

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Connective Tissue components

Collagen: Fibrous protein

  • Very stiff

Elastin: Fibrous protein

  • Very pilant


Connective tissue composition affects loading response


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Isotropic

stiffness similar in different directions

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Ansiotropic

Stiffness dependent on load direction

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Mechanical properties of the MS: Bone

45% mineral, 30%—35% collagen, 20% water

Strongest and stiffest material in musculoskeletal system

  • Compression > Tension > Shear

Mechanical properties vary with bone health

Bone strength affected by rate of loading

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Mechanical properties of the MS: Cartilage

60%-80% water, 10%-30% collagen

  • Hyaline (articular): covers bone ends at joints

  • Fibrous: specialized in joints (invertebral disks, menisci)


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Mechanical properties of the MS: Tendons & Ligaments

70% water, 25% collagen

Ligaments have more elastin than tendons

collagen fibers in bundles aligned with functional axis

  • High stiffness to tensile loading


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Mechanical properties of the MS: Muscle

Active component (sarcomere) determines muscle stiffness

  • Passive component (connective tissue sheaths) create high failure strain