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Simulation Study on Mechanical Adaptation in Cancellous Bone by Trabecular Surface Remodeling Taiji ADACHI, Ken-ichi TSUBOTA and Yoshihiro TOMITA Kobe University / RIKEN May 24 May 24 May 24 May 24- - -25, 2000, Suzuki Umetaro Hall, RIKEN 25, 2000, Suzuki Umetaro Hall, RIKEN 25, 2000, Suzuki Umetaro Hall, RIKEN 25, 2000, Suzuki Umetaro Hall, RIKEN RIKEN Symposium RIKEN Symposium RIKEN Symposium RIKEN Symposium Computational Biomechanics Computational Biomechanics Computational Biomechanics Computational Biomechanics

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Simulation Study on Mechanical Adaptation in Cancellous Bone by Trabecular Surface Remodeling

Taiji ADACHI, Ken-ichi TSUBOTA and Yoshihiro TOMITA

Kobe University / RIKEN

May 24May 24May 24May 24----25, 2000, Suzuki Umetaro Hall, RIKEN25, 2000, Suzuki Umetaro Hall, RIKEN25, 2000, Suzuki Umetaro Hall, RIKEN25, 2000, Suzuki Umetaro Hall, RIKEN

RIKEN Symposium RIKEN Symposium RIKEN Symposium RIKEN Symposium – Computational Biomechanics Computational Biomechanics Computational Biomechanics Computational Biomechanics –

Bone Functional Adaptation by Remodeling

Mechanical Environment Bone Structure

Introduction

Hierarchical Structure of Bone

MicroTanaka

Mechanical Stimuli

Cellular Activities

Formation / Resorption

Structural Changes

• Trabecular microstructure of cancellous bone– changing / maintained by remodeling under mech. influence

• Adaptation to mechanical environment– regulated by Oc / Ob activities on trabecular surface

• Surface movement by cellular activities lead to– macroscopic changes of trabecular architecture

Trabecular Surface Remodeling

(Parfitt94)

Theoretical models & Computational simulations

Computational Simulation for Bone Remodeling

Microscopic MechanismCowin92, Sadegh93,

Mullender94

Macroscopic PhenomenaCowin76, Carter87, Huiskes87,

Beaupre90, Weinans92

- Self Optimization Model (Carter87)- Adaptive Elasticity (Cowin76)

(Carter87)

Trabecular Level Remodeling

Trabecular Remodeling

• Microscopic resorption / formation by osteoclasts / osteoblasts on trabecular surface (e. g. Parfitt84)

• Local mechanical signals play an important role(e.g. Guldberg97)

• Trabecular level mechanical stimulus related to morphological changes of trabecular architecture

Outline

Simulation for Trabecular Surface Remodeling

• Remodeling Rate Equation• Method of Pixel-based Simulation• Computational Simulation for Proximal Femur

• A Remodeling Rate Equation: based on Uniform Stress Hypothesis

as an optimality condition for remodeling equilibrium (Adachi98)

• Nonuniformity in local stress distribution on trabecular surface as driving force of remodeling

• Related to local morphological changes of trabecular architecture

Uniform Stress Hypothesis

A Remodeling Rate Equation

∫∫=SS rd dSlwdSlw )()( σσ

)/(ln dc σσΓ =

<Γ>Γ

=

Γ=

Resorption:0Formation:0

)(FM&

Representative stress

Stress nonuniformity

Driving force of remodeling

A Remodeling Rate Equation

Microstructural Finite Element ModelTrabecular Bone- Microstructural voxel/pixel finite element models- Resorption/formation by removing/adding elements- Generated by using digital images, µµµµCT

Stress Analysis by EBE/PCG FEM

EquilibriumNo

Yes

Surface Movement

Calculation of Remodeling Driving Force ΓΓΓΓ

End

1 step

Remodeling Simulation

2

- Bone part: 0.67 Million Elements- Pixel size: 70µm

Lat. Med.

10mm

Cancellousbone

Cortical bone

140m

m (2

000

pixe

ls)

Hip abductionforce

Joint reactionforce

*Model parameters(1) Threshold values: Γ u = 1.0, Γ l = -2.0(2) Sensing distance: lL = 1.0mm (~14 pixels)

H1 = 714µm, H2 = 713µmH1/H2 = 1.00

Fabric ellipse4mm×4mm region

1mm

Large-Scale FE Pixel Model of Proximal Femur

- Trabecular bone remodeling at 12th StepOne-legged stance Abduction

* Boundary condition (Beaupré90)

703N, 28°

2317N, 24°

351N, -8°

1158N, -15°

Region 1

Region 2

10mm

Trabecular Structural Changes

Trabecular microstructure Apparent principal stress

- Region 1: Uniaxial Compression

Fabric ellipse

- Region 2: Compression-Tension

1

2

1000µm

1000µm

10MPa

10MPa

ΘH = 48° Θσ = -59°

σ1 = -2.3MPaσ2 = 2.2MPa

|σ1/σ2 | = 1.04

1 2

1

2

1000µm

1000µm

10MPa

10MPa

CompressionTension

ΘH = 30° Θσ = 24°

H1 = 794µmH2 = 583µmH1/H2 = 1.36

σ1 = -9.5MPaσ2 = 0.66MPa

|σ1/σ2 | = 14.3

1

2

1mm

1mm

H1 = 645µmH2 = 625µmH1/H2 = 1.03

Trabecular Structure & Mechanical Environment

Remodeling under Multiple Loading

Structural Changes under Multiple Loading

Structural Changes under Multiple Loading

703N28° 2317N

24°

351N-8°

1158N-15°

468N35° 1548N

56°

(1) One-legged stance: 6000/day

(2) Abduction: 2000/day

(3) Adduction: 2000/day

Trabecular bone remodeling at 10th step* B.C.: Beaupré et al. (1990)

10mm

Fine Element

70µm/pixel(Tanaka92)

Comparison

One-legged stance Abduction Adduction

Trabecular microstructure for multiple loading condition

Equivalent stress distribution*Single loading condition:

One-legged stance

1mm

1mm

At Microstructural Level

Discussion and Conclusion

- Trabecular surface remodeling in cancellous bone- Large-scale pixel FE model of proximal femur- Trabeculae adapt to mechanical environment- Direct evaluation of micro-macro relationships- Insight into microscopic mechanism

Proposed simulation method using microstructural voxel FE models could be applicable to predict the

trabecular remodeling

Future Works3D remodeling simulationusing digital-image based

FE model (µCT)

Guldberg97

Comparison with experiment

Application to orthopaedic research area: Remodeling at bone-implant interface