#4 - Material, Structural and Tissue Mechanics
Material, Structural and Tissue Mechanics
The study of mechanical properties of biological tissues relies on:
Material Properties:
How a material behaves under loading conditions.
Mass, density, stiffness, strength
Structural Properties:
How the gross geometric configuration affects loading behaviours
size, shape (length, diameter)
Stress
Stress (σ) = Force / Area
A measure of a material’s internal resistance to axial load (either compression or tensile)
Measured in Pascals (Pa) = 1 N / m2 or MegaPascals = 1N/mm2
[1 N = 0.225 lbs force; 1 Pa = 145x10-6 lb/sq in]
Material failure - Stress Risers
Stress Riser: Discontinuity leading to uneven distribution of stresses.
Increases chance of tissue failure
“Sisceptibility to tissue failure is directly related to distribution of forces through tissue.”
Even distribution is optimal
Examples of discontinuities/stress risers??
Fractures (existing, past)
Occult tissue/fibrosis
Screws (current, past)
Tumour, infection
Osteotendinous junctions
Material Failure
Strain
Strain (ε): a measure of deformation
Stress-Strain Curves: Material Property
Stress-Strain Considerations: Toughness
“Toughness”: total failure energy = area under curve
Characteristics of an Idealized Stress-Strain Curve for Biologic Tissues: Uniaxial Loading
Elastic Limit (“C”)
Permanent Set
What is the physiologic/biomechanical impact of permanent set?
Clinical Impact of permanent set and plastic deformation??
Length-Tension Relationship in Muscle
What are the clinical implications of this?
How might we identify this clinically?
Clinical Implications of Plastic Deformation
Load-Deformation Curve: Structural Property
Structural Stiffness ~ A/L
Clinical Implications: Strength training increases Cross-sectional area of patellar tendon in cyclists
Material Mechanics:
Comparison of Structural vs Material Properties
Biologic Stress Strain Curves are Direction-dependent
Isotropic = loading characteristics/properties of a material are the same in all direction.
Anisotropic = loading characteristics/properties of a material are directionally dependent.
Biological Tissues are ANISOTROPIC
Exhibit a preferred direction of loading.
Examples include tendons, ligament, bone.
Effect of Anisotropy on tendon biomechanical properties
Reduced strain-to-failure
Decreased stiffness
Smaller region of plastic deformation (more brittle)
What is the clinical relevance/application of this concept?
Clinical Application of Anisotropicity
Pronation (pes planus)
Calcaneovalgus
Leads to shear forces at achilles tendon insertion
Ductile vs. Brittle
Fluid Mechanics and Friction
Branch of mechanics dealing with the properties and behaviour of liquids (and gases)
Several branches of mechanics in biology rely on principles of Fluid Mechanics:
Performance biomechanics
Biotribology: study of wear and tear on joints
Tissue Mechanics (disc, tendon, bone)
****VERY IMPORTANT METHOD OF DISSIPATING ENERGY****
Friction:
Resistance at the interface of two bodies
Static Friction: from a standing position (v=0)
What is the clinical relevance/application of this equation?
Dynamic Friction:
Rheology - study of flow of matter
Viscosity
Resistance to flow of a liquid
Related to forces of attraction of particles within the liquid
Related to the material properties of the fluid
Fluid “internal” friction
Fluid “shear stiffness” or “shear stress”
What can alter the viscosity (internal friction) of a liquid?
Temperature
Rate of flow**
Inertia and Drag of Fluids
Fd = ½pv^2CdA
Fd = Drag force
P = density of fluid
V = velocity
C = Drag coefficient
A = X-sectional AREA body
Rate of Flow ~ Viscosity
Shear Stress: fluid ‘stiffness’, resistance to flow = slope of a stress-strain curve of a liquid
Viscosity vs Shear rate: Newtonian Vs Non-Newtonian
Clinical Conditions that alter interstitial fluid viscosity
Altered macromolecular structure/content (collagen, proteoglycans, glycosaminoglycans, elastin, glycation end products)
Age
Increased glycation (cross-links between collagen molecules)
Altered high-weight molecules in the extracellular matrix (GAG, PG)
Inflammation/Edema
Protein accumulation (fibrin, globulins)
Glucpsaminoglycans
Dehydration
Electrolyte imbalance - alters change density (hydophilic)
Concentration of remaining proteins
Pathological matrix remodelling
Fibrosis
Diabetic glycation
Degenerative diseases (cartilage, tendonosis)
What relevance does this slide have to injury prevention?
Viscoelastic Tissue Mechanics
Viscoelastic Tissue
Biological tissues are viscoelastic
Tendon, ligament, cartilage, bone
Interaction of fluid (viscous) and solid (elastic) phases
High friction forces at interface of fluid: elastic components
Friction and viscosity are important principles in understanding tissue mechanics and injury
***Integriy of solid/fluid phases critical to tissue function***
Ehlers-danlos syndrome, Marfan Syndrome
RATE IF LOADING of BIOLOGIC TISSUES significantly alters internal tissue stresses because it impacts viscosity
Viscoelasticity
Elastic Tissue
Viscoelastic Tissue
Viscoelasticity - hysteresis
Elastic vs Viscoelastic
Theological Models to study Viscoelastic Tissues
Rheology: Study of deformation and flow of matter
Used to model biological (viscoelastic) tissue
Interrelate stress, strain, and strain rate
Two model components:
Linear spring
Elastic component
Dashpot
Viscous component
Rheological Models: Linear spring
Elastic properties of tissue
Strain Rate INDEPENDENT
Rheological Models: Dashpot
Represents ‘viscous’ component of viscoelastic tissue
Loading response is strain rate development
Rate of Loading Increases internal tissue stress
Viscoelastic Tissues exhibit Unique Mechanical Behaviours:
Stress-Relaxation
Creep
Biologic Tissues demonstrate:
Stress-Relaxation: CONSTANT DEFORMATION
Viscoelastic Creep:
Increasing strain with CONSTANT STRESS
Clinical Applications of Creep
Initial-Cycles (First-Cycle) Effect
Loading history (history dependence) of biologic tissues has significant effect on mechanical properties
Repeart Loads lead to tissue ‘fatigue’ - reduced hysteresis effect
More pronounced with aging and OA
Decreased ‘stiffness’
Due to plastic deformation (permanent set)
Decreased ability to withstand further applied forces.
In load-time curve
Upward shift (less ‘stress-relaxation’) with increasing repetition (n)
Steady state = ‘preconditioned’
Continued loading to predisposes to tissue ‘ failure’.
Tissue Loading
Uniaxial Loading: Poisson Effect
Bending: Area Moment of Inertia:
= resistance of a beam to bending about its neutral axis
Solid Cylinder
Hollow Cylinder
What is the trade-off between Bone, Mass, Radius in a solid vs hollow bone with the same Area Moment of Inertia
If we keep the area moment of inertia the same, what is the difference in radius of a hollow bone vs a solid bone?
In keeping area moment of inertia the same, what is the difference in mass between a hollow bone vs solid bone?
What is the trade-off between Mass and Radius of a solid vs hollow bone?
Comparison of Solid vs Hollow Bone Strength vs Mass
Assume bone dimensions of:
Radius = 10cm
Length = 40cm
Density (cortical bone) p = 1.9 g/cm^3
Hollow Bone:
What outer radius is needed to maintain area moment of inertia for hollow bone?
Summary: for two bones with equal area moment of inertia….
Solid Bone:
Radius = 10cm
Length = 40cm
Weight = 23.9kg
I = 7850cm^4
Hollow Bone:
Inner Radius = 10cm
Outer Radius = 11.9cm
Cortical Thickness = 1.9cm
Length = 40cm
Weight = 9.9kg
I = 7859cm^4
Net Weight Difference = 14 kg
19% increase in radius
59% lighter
Bending
Long bones mechanically considered as ‘beams’
Stress (both tensile and compressive) are maximal the further from the neutral axis
Three Point Bending
Failure in 3 vs 4-point Bending
Torsion: Helical Stress
Cantilever Bending:
= compressive force offset from the longitudinal axis creating both bending moment and compression