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TRIBOLOGY IN ORTHOPAEDICS
DR UJJAL RAJBANGSHI
ORTHOPAEDICS,SMCH
LEARNING OBJECT
 History and introduction
 Friction
 Lubrication –mechanism and its different types
 Wear- mechanism and its different types
 Biological effects of wear particles
 Ideal implant
History
 David Tabor (23 October 1913 - 26 November 2005)
 A British Physicist ,was an pioneer of tribology
 Dr H Peter Jost (25th January 1921- 7th June 2016)
 Coined the term Tribology
Introduction
 Science of interacting surfaces in relative motion
 Tribos (Greek) meaning rubbing
 includes study of Friction, Lubrication, Wear
Friction
 Resistance to sliding motion between two bodies in contact
 Friction Force (F) ∝ Applied Load (W)
 F = μW (μ is the coeffificient of friction)
 F is independent of the apparent contact area
 Friction causes wear and generates heat which can lead to premature failure of the functioning implants.
Lubrication
 Synovial fluid:
 produced by Type B fibroblast-like cells (Type A cells help phagocytosis).
 clear viscous liquid , made up of proteinase, collagenase, hyaluronic acid, lubricin and prostaglandins.
 It is a dialysate of blood plasma without clotting factors or erythrocytes .
 Exhibits non-newtonian flow properties
 Pseudoplasticity = fall in viscosity as shear rate increases
 Thixotropy = time-dependent decrease in viscosity under constant shearing
Sommerfeld Number (S)
 S ∝ viscosity × velocity / stress
 Lambda value λ = fluid thickness / surface roughness
 Critical lambda value for reduced friction is ≈3
Stribeck Curve
 The relationship of coefficient of friction and lubricant film thickness is commonly shown in a Stribeck curve
that relates the friction to the Sommerfeld number.
 If the film thickness is much smaller than the combined roughness
of the articulating surfaces then surface asperity interaction cannot
be avoided and a boundary lubrication regime exists.
 If the lubricant film thickness is of a similar magnitude
to the combined surface roughness then a mixed lubrication
regime will exist with variable amounts of asperity contact.
 If the film thickness is sufficiently large compared to the surface
roughness it will prevent surface asperity interaction leading to low
friction and theoretically no wear. Seen in hydrodynamic lubrication
Types of Lubrication
 1. Boundary
 2. Fluid film
 2.1 Hydrodynamic
 2.2 Elastohydrodynamic
Boundary Lubrication
 Contact-bearing surfaces separated only by lubricant of molecular thickness
 Occurs when fluid film has been depleted
 Involves single monolayer of lubricant adsorption on each surface
 Independent of physical properties of lubricant(eg., viscosity) and
bearing material(stiffness)
 Primarily dependent on chemical properties of lubricant
fluid film Lubrication
 Separation of surfaces by a fluid film
 minimum thickness exceeds the surface roughness of the bearing surface
 prevents asperity contact
Hydrodynamic
 Non parallel rigid bearing surfaces
 Separated by a fluid film slide tangentially
 Converging wedge fluid forms
 Viscosity within this wedge produces a lifting pressure
 No contact between surfaces and hence no wear
 May occur during the swing phase of gait
Elastohydrodynamic Lubrication
 Occurs in non rigid bearing surfaces
 Macroscopic deformation serves to trap pressurized fluid
 This increase surface area which decreases the shear rate
 This increases the viscosity of synovial fluid
Microelastohydrodynamic Lubrication
 Assumes asperities of articular cartilage are deformed under high loads
 This smoothens out the bearing surface
 Which creates a film thickness of 0.5–1 μm, sufficient for fluid film lubrication
Squeeze film
 Occurs when there is no relative sliding motion
 Pressure builds up as viscous fluid offers resistance to being
squeezed
 Lubricant layer becomes thinner and the joint surfaces come
into contact
 This mechanism is capable of carrying high loads for short lengths of time
Schematic of squeeze film formation for a
cylinder on a soft flat
layer.
Boosted Lubrication
 Under squeeze film conditions
 Water and synovial fluid are pressurized(compressed) into cartilage
 Leaving behind a concentrated pool of hyaluronic acid protein
 This lubricates the surfaces
Weeping Lubrication
 Occurs when cartilage is compressed
 Articular cartilage is fluid filled, porous and permeable
 It is capable of exuding and imbibing lubrication fluid
 Cartilage generates tears of lubricant fluid by compression of the bearing surface
 The process is thought to contribute to nutrition of the chondrocytes
Lubrication Mechanisms - Synovial Joints
 Intact synovial joints have a very low coefficient of friction (~0.02)
 Articular cartilage surface is not flat and has numerous asperities
 Kind of lubrication occurring at one time in a synovial joint varies according to the loading conditions
Wear
 Progressive loss of material from the surface due to relative motion.
 Simply the removal of material from a solid surface by the action of another surface.
 Generates further “third body” wear particles .
 Softest material is worn first
Wear Mechanism
 Wear is either chemical (usually corrosive) or mechanical
 Types of mechanical wear include:
 Adhesive
 Abrasive
 Fatigue
Adhesive Wear
 Occurs when junction is formed between two opposing surfaces
 Junction is held by inter-molecular bonds
 This force is responsible for friction
 This junction is responsible for spot welding / transfer
 Steady low wear rate
Abrasive Wear (ploughing)
 Occurs when softer material comes into contact with significantly harder material
 Microscopic counterface aspirates on the harder surface cut and plough through the softer material
 This produces grooves and detaches material to form wear debris
 This is the main mechanism in metal / polymer prostheses
Abrasive Wear (ploughing)
 Abrasive wear (cont.):
 Third body abrasive wear occurs when extraneous material enters the interfacial region
 Trapped wear debris produces a very high local stress
 This quickly leads to localized fatigue failure and a rapid,
varying wear rate.
Fatigue Wear
 Caused by accumulation of microscopic damage within the bearing material
 Depends on the frequency and magnitude of the applied loads and on the intrinsic properties of the
bulk material
 Also dependent on contact stress Fatigue wear :
 Decreased by:
 Conformity of surfaces
 Thicker bearing surface
 Increased by:
 Higher stiffness of material
 Misaligned or unbalanced implants
Corrosive wear
 Mechanical wear may remove the passivation layer
 This allows chemical corrosion to occur
Wear sources in Joint Arthroplasty
 Primary articulation surface
 Secondary articulation surface
 backside of modular poly insert with metal
 screw fretting with the metal shell of acetabular liners
 Cement - prosthesis micromotion
 Cement - bone or prosthesis - bone micromotion
 Third body wear
Linear wear :
 Loss of height of the bearing surface
 Expressed in mm / year
Volumetric wear :
 Total volume of material that has been worn away
 Expressed in mm3 / year
Wear rate
 Debris volume; highest in the first year – “wearing in”
 Steady state then achieved (debris volume related to load and sliding distance)
 Accelerated wear occurs at the end of a prosthesis’ life
Head size
 Volume of wear debris = πPr2 (P is penetration and r is radius of femoral head)
 Larger the femoral head the greater the sliding distance and volumetric wear
 Smaller head size decreases the sliding distance and reduces volumetric wear
 Smaller the femoral head the greater the penetration
Laws of wear
 The volume of material (V) removed by wear increases with load (L) and sliding distance (X) but decreases
as the hardness of the softer material (H) increases:
 V ∝ LX / H
 V = kLX
 k = a wear factor for a given combination of materials
Factors that determine wear
Patient factors
 Weight (applied load)
 Age and activity level (rate of applied rate load)
Factors that determine wear
Implant factors
 Coefficient of friction (lubrication)
 Roughness (surface finish)
 Toughness (abrasive wear)
 Hardness (scratch resistance, adhesive wear)
 Surface damage
 Presence of third bodies (abrasive wear)
Wear in prosthetic hips
 There is a combination of wear and creep
 Creep usually dominates the initial penetration rate
 Majority of the linear penetration after the first year is due to wear
 Direction of creep is superomedial
 Direction of wear is superolateral
Wear in prosthetic hips
Wear in prosthetic hips:
 Cup penetration can be measured in the following ways:
 By comparison between initial and follow-up radiographs, corrected for magnification
 Shadowgraph technique
 Computer software scan imaging
Biological effects of wear particles
 Large (micron sized) particles have localized effects at the bone / implant / cement interfaces
 Small (nanometre sized) particles are thought to have the potential for systemic effects
Biological effects of wear particles
Local
 Particles 0.1–10 μm diameter .
 Phagocytosed by macrophages .
 Stimulate the release of soluble pro-inflammatory mediators (tumour necrosis factor (TNF), interleukin
(IL)-1, IL-6, PGE2, matrix metaloproteinases) .
 Mediators released stimulate bone resorption by osteoclasts and impair the function of osteoblasts.
Biological effects of wear particles
Local (cont.):
 Major factors that affect extent of osteolysis are:
 Volume of wear debris >150 mm3 per annum is thought to be the “critical” level
 Total number of wear particles
 Morphology of particles
 Size of particles
 Immune response to the particles
Biological effects of wear particles
Systemic
 Metal ion release is increased five-fold by metal-on-metal bearing surfaces
 Metal ions are not phagocytosed
 Immune sensitization and neoplastic transformation are concerns
 Pseudotumours and metal hypersensitivity leads to early hip revision
Corrosion
Corrosion is reaction of a metal with its environment
 resulting in continuous degradation to
 oxides, hydroxides or other compounds Passivation
 Oxide layer forms on the alloy surface
 Strongly adherent
 Acts as a barrier to prevent corrosion
 Can be jeopardized by mechanical wear
Corrosion
 Types of corrosion
 Uniform attack
 Galvanic
 Crevice
 Pitting
 Fretting (combination of wear and crevice corrosion)
 Intergranular
 Inclusion corrosion
 Leaching corrosion
 Stress corrosion
Ideal implant
 Biocompatibility: inert, non-immunogenic, nontoxic, non-carcinogenic
 Strength: sufficient tensile, compressive and torsional strength, stiffness and fatigue resistance
 Workability: easy to manufacture and implant
 Inexpensive
 No effect on radiological imaging
 Corrosion free
THANK YOU

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Tribology in orthopaedics seminar

  • 1. TRIBOLOGY IN ORTHOPAEDICS DR UJJAL RAJBANGSHI ORTHOPAEDICS,SMCH
  • 2. LEARNING OBJECT  History and introduction  Friction  Lubrication –mechanism and its different types  Wear- mechanism and its different types  Biological effects of wear particles  Ideal implant
  • 3. History  David Tabor (23 October 1913 - 26 November 2005)  A British Physicist ,was an pioneer of tribology  Dr H Peter Jost (25th January 1921- 7th June 2016)  Coined the term Tribology
  • 4. Introduction  Science of interacting surfaces in relative motion  Tribos (Greek) meaning rubbing  includes study of Friction, Lubrication, Wear
  • 5. Friction  Resistance to sliding motion between two bodies in contact  Friction Force (F) ∝ Applied Load (W)  F = μW (μ is the coeffificient of friction)  F is independent of the apparent contact area  Friction causes wear and generates heat which can lead to premature failure of the functioning implants.
  • 6. Lubrication  Synovial fluid:  produced by Type B fibroblast-like cells (Type A cells help phagocytosis).  clear viscous liquid , made up of proteinase, collagenase, hyaluronic acid, lubricin and prostaglandins.  It is a dialysate of blood plasma without clotting factors or erythrocytes .  Exhibits non-newtonian flow properties  Pseudoplasticity = fall in viscosity as shear rate increases  Thixotropy = time-dependent decrease in viscosity under constant shearing
  • 7. Sommerfeld Number (S)  S ∝ viscosity × velocity / stress  Lambda value λ = fluid thickness / surface roughness  Critical lambda value for reduced friction is ≈3
  • 8. Stribeck Curve  The relationship of coefficient of friction and lubricant film thickness is commonly shown in a Stribeck curve that relates the friction to the Sommerfeld number.  If the film thickness is much smaller than the combined roughness of the articulating surfaces then surface asperity interaction cannot be avoided and a boundary lubrication regime exists.  If the lubricant film thickness is of a similar magnitude to the combined surface roughness then a mixed lubrication regime will exist with variable amounts of asperity contact.  If the film thickness is sufficiently large compared to the surface roughness it will prevent surface asperity interaction leading to low friction and theoretically no wear. Seen in hydrodynamic lubrication
  • 9. Types of Lubrication  1. Boundary  2. Fluid film  2.1 Hydrodynamic  2.2 Elastohydrodynamic
  • 10. Boundary Lubrication  Contact-bearing surfaces separated only by lubricant of molecular thickness  Occurs when fluid film has been depleted  Involves single monolayer of lubricant adsorption on each surface  Independent of physical properties of lubricant(eg., viscosity) and bearing material(stiffness)  Primarily dependent on chemical properties of lubricant
  • 11. fluid film Lubrication  Separation of surfaces by a fluid film  minimum thickness exceeds the surface roughness of the bearing surface  prevents asperity contact
  • 12. Hydrodynamic  Non parallel rigid bearing surfaces  Separated by a fluid film slide tangentially  Converging wedge fluid forms  Viscosity within this wedge produces a lifting pressure  No contact between surfaces and hence no wear  May occur during the swing phase of gait
  • 13. Elastohydrodynamic Lubrication  Occurs in non rigid bearing surfaces  Macroscopic deformation serves to trap pressurized fluid  This increase surface area which decreases the shear rate  This increases the viscosity of synovial fluid
  • 14. Microelastohydrodynamic Lubrication  Assumes asperities of articular cartilage are deformed under high loads  This smoothens out the bearing surface  Which creates a film thickness of 0.5–1 μm, sufficient for fluid film lubrication
  • 15. Squeeze film  Occurs when there is no relative sliding motion  Pressure builds up as viscous fluid offers resistance to being squeezed  Lubricant layer becomes thinner and the joint surfaces come into contact  This mechanism is capable of carrying high loads for short lengths of time Schematic of squeeze film formation for a cylinder on a soft flat layer.
  • 16. Boosted Lubrication  Under squeeze film conditions  Water and synovial fluid are pressurized(compressed) into cartilage  Leaving behind a concentrated pool of hyaluronic acid protein  This lubricates the surfaces
  • 17. Weeping Lubrication  Occurs when cartilage is compressed  Articular cartilage is fluid filled, porous and permeable  It is capable of exuding and imbibing lubrication fluid  Cartilage generates tears of lubricant fluid by compression of the bearing surface  The process is thought to contribute to nutrition of the chondrocytes
  • 18. Lubrication Mechanisms - Synovial Joints  Intact synovial joints have a very low coefficient of friction (~0.02)  Articular cartilage surface is not flat and has numerous asperities  Kind of lubrication occurring at one time in a synovial joint varies according to the loading conditions
  • 19. Wear  Progressive loss of material from the surface due to relative motion.  Simply the removal of material from a solid surface by the action of another surface.  Generates further “third body” wear particles .  Softest material is worn first
  • 20. Wear Mechanism  Wear is either chemical (usually corrosive) or mechanical  Types of mechanical wear include:  Adhesive  Abrasive  Fatigue
  • 21. Adhesive Wear  Occurs when junction is formed between two opposing surfaces  Junction is held by inter-molecular bonds  This force is responsible for friction  This junction is responsible for spot welding / transfer  Steady low wear rate
  • 22. Abrasive Wear (ploughing)  Occurs when softer material comes into contact with significantly harder material  Microscopic counterface aspirates on the harder surface cut and plough through the softer material  This produces grooves and detaches material to form wear debris  This is the main mechanism in metal / polymer prostheses
  • 23. Abrasive Wear (ploughing)  Abrasive wear (cont.):  Third body abrasive wear occurs when extraneous material enters the interfacial region  Trapped wear debris produces a very high local stress  This quickly leads to localized fatigue failure and a rapid, varying wear rate.
  • 24. Fatigue Wear  Caused by accumulation of microscopic damage within the bearing material  Depends on the frequency and magnitude of the applied loads and on the intrinsic properties of the bulk material  Also dependent on contact stress Fatigue wear :  Decreased by:  Conformity of surfaces  Thicker bearing surface  Increased by:  Higher stiffness of material  Misaligned or unbalanced implants
  • 25. Corrosive wear  Mechanical wear may remove the passivation layer  This allows chemical corrosion to occur
  • 26. Wear sources in Joint Arthroplasty  Primary articulation surface  Secondary articulation surface  backside of modular poly insert with metal  screw fretting with the metal shell of acetabular liners  Cement - prosthesis micromotion  Cement - bone or prosthesis - bone micromotion  Third body wear
  • 27. Linear wear :  Loss of height of the bearing surface  Expressed in mm / year Volumetric wear :  Total volume of material that has been worn away  Expressed in mm3 / year
  • 28. Wear rate  Debris volume; highest in the first year – “wearing in”  Steady state then achieved (debris volume related to load and sliding distance)  Accelerated wear occurs at the end of a prosthesis’ life
  • 29. Head size  Volume of wear debris = πPr2 (P is penetration and r is radius of femoral head)  Larger the femoral head the greater the sliding distance and volumetric wear  Smaller head size decreases the sliding distance and reduces volumetric wear  Smaller the femoral head the greater the penetration
  • 30. Laws of wear  The volume of material (V) removed by wear increases with load (L) and sliding distance (X) but decreases as the hardness of the softer material (H) increases:  V ∝ LX / H  V = kLX  k = a wear factor for a given combination of materials
  • 31. Factors that determine wear Patient factors  Weight (applied load)  Age and activity level (rate of applied rate load)
  • 32. Factors that determine wear Implant factors  Coefficient of friction (lubrication)  Roughness (surface finish)  Toughness (abrasive wear)  Hardness (scratch resistance, adhesive wear)  Surface damage  Presence of third bodies (abrasive wear)
  • 33. Wear in prosthetic hips  There is a combination of wear and creep  Creep usually dominates the initial penetration rate  Majority of the linear penetration after the first year is due to wear  Direction of creep is superomedial  Direction of wear is superolateral
  • 34. Wear in prosthetic hips Wear in prosthetic hips:  Cup penetration can be measured in the following ways:  By comparison between initial and follow-up radiographs, corrected for magnification  Shadowgraph technique  Computer software scan imaging
  • 35. Biological effects of wear particles  Large (micron sized) particles have localized effects at the bone / implant / cement interfaces  Small (nanometre sized) particles are thought to have the potential for systemic effects
  • 36. Biological effects of wear particles Local  Particles 0.1–10 μm diameter .  Phagocytosed by macrophages .  Stimulate the release of soluble pro-inflammatory mediators (tumour necrosis factor (TNF), interleukin (IL)-1, IL-6, PGE2, matrix metaloproteinases) .  Mediators released stimulate bone resorption by osteoclasts and impair the function of osteoblasts.
  • 37. Biological effects of wear particles Local (cont.):  Major factors that affect extent of osteolysis are:  Volume of wear debris >150 mm3 per annum is thought to be the “critical” level  Total number of wear particles  Morphology of particles  Size of particles  Immune response to the particles
  • 38. Biological effects of wear particles Systemic  Metal ion release is increased five-fold by metal-on-metal bearing surfaces  Metal ions are not phagocytosed  Immune sensitization and neoplastic transformation are concerns  Pseudotumours and metal hypersensitivity leads to early hip revision
  • 39. Corrosion Corrosion is reaction of a metal with its environment  resulting in continuous degradation to  oxides, hydroxides or other compounds Passivation  Oxide layer forms on the alloy surface  Strongly adherent  Acts as a barrier to prevent corrosion  Can be jeopardized by mechanical wear
  • 40. Corrosion  Types of corrosion  Uniform attack  Galvanic  Crevice  Pitting  Fretting (combination of wear and crevice corrosion)  Intergranular  Inclusion corrosion  Leaching corrosion  Stress corrosion
  • 41. Ideal implant  Biocompatibility: inert, non-immunogenic, nontoxic, non-carcinogenic  Strength: sufficient tensile, compressive and torsional strength, stiffness and fatigue resistance  Workability: easy to manufacture and implant  Inexpensive  No effect on radiological imaging  Corrosion free