finite element representation of muscles...node 179 node 204 node 205 node 206 node 227 node 228...

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Finite Element Representation of Muscles Peter James Nugent, Supervisor: Dr. Andrew Phillips Department of Civil and Environmental Engineering, Imperial College London S16 Figure 1: Conversion from tetrahedral to truss elements Figure 2: Mesh of the muscle Final Muscle Model • Utilised a hyper elastic material that accurately captured the passive response of the muscle (Figure 4) • The model could be subject to both compressive and tensile forces (Figures 3 & 4) • Eight connector elements around the exterior of the muscle induced the compressive force • The wires that followed the geometry were similar to those found in the literature (Böl and Reese, 2008) ϵ [-] ×10 -3 -4 -3 -2 -1 0 1 2 3 4 Force [kN] -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Node 1 Node 4 Node 12 Node 19 Node 20 Node 27 Node 28 Node 35 Node 64 Node 65 Node 66 Node 89 Node 90 Node 91 Node 140 Node 141 Node 142 Node 177 Node 178 Node 179 Node 204 Node 205 Node 206 Node 227 Node 228 Node 229 Node 264 Node 265 Node 266 Node 277 Node 278 Node 279 Figure 3: Force-strain graph in the X direction ϵ [-] -0.25 -0.2 -0.15 -0.1 -0.05 0 0.05 0.1 0.15 0.2 Force [kN] -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Node 13 Node 14 Node 17 Node 18 Node 32 Node 34 Node 41 Node 43 Node 101 Figure 4: Force strain graph in the Y direction Figure 5: Anatomical model of the elbow system Biceps brachii Brachialis Brachioradialis Humerus Radius Ulna Figure 6: Elbow system in Abaqus CPRESS +0.000e+00 +6.415e01 +1.283e+00 +1.924e+00 +2.566e+00 +3.207e+00 +3.849e+00 +4.490e+00 +5.132e+00 +5.773e+00 +6.415e+00 +7.056e+00 +7.698e+00 X Y Z CPRESS +0.000e+00 +6.415e01 +1.283e+00 +1.924e+00 +2.566e+00 +3.207e+00 +3.849e+00 +4.490e+00 +5.132e+00 +5.773e+00 +6.415e+00 +7.056e+00 +7.698e+00 X Y Z CPRESS +0.000e+00 +6.415e01 +1.283e+00 +1.924e+00 +2.566e+00 +3.207e+00 +3.849e+00 +4.490e+00 +5.132e+00 +5.773e+00 +6.415e+00 +7.056e+00 +7.698e+00 X Y Z CPRESS +0.000e+00 +6.415e01 +1.283e+00 +1.924e+00 +2.566e+00 +3.207e+00 +3.849e+00 +4.490e+00 +5.132e+00 +5.773e+00 +6.415e+00 +7.056e+00 +7.698e+00 X Y Z Figure 7: Contact pressure on the humerus Aims • Create a generalised muscle model capable of being subject to compressive and tensile loads • Implement the muscle model in to an elbow system and capture the interaction between the deformed muscle and the bone Current Models • Existing muscle models use complex material sub routines that are computationally expensive • Some focus on the microscopic and mesoscopic scale of muscles such as the binding between actin and myosin proteins (Gielen et al., 2000) • Some also utilise MRI and CT scans that render the models subject specific Mesh & Geometry • A mesh was created using tetrahedral elements, which were then converted to truss elements (Figure 1) • This reduced the computational cost because truss elements have a single degree of freedom and hence can only deform axially, this is synonymous with the behaviour of a muscle 3D Elbow Mechanism • The biceps brachii was chosen as the muscle to model in three dimensions because it makes contact with the humerus in the system that was adapted from the literature (Siemienski, 1992; Rasmussen et al., 2001) • The brachialis and brachioradialas were modelled as wires • The ulna and radius were combined to model the forearm (Figures 5 & 6) • The contact between the biceps brachii and the humerus was modelled using a node to surface contact Conclusions • The muscle model correctly captured the passive behaviour of the muscle and leaves scope for further work to manipulate the active response of the muscle • The elbow mechanism accurately modelled the contact pressure between the humerus and biceps brachii (Figure 7) • A musculoskeletal model can be used to obtain muscle forces, implemented in to the elbow mechanism model and the resulting contact pressures can be applied to finite element models of bones References Böl, M. and Reese, S. (2008). Micromechanical modelling of skeletal muscles based on the finite element method. Computer methods in biomechanics and biomedical engineering, 11(5):489–504. Gielen, A. W. J., Oomens, C. W. J., Oomens, C. W. J., Arts, T., and Janssen, J. D. (2000). A finite element approach for skeletal muscle using a distributed moment model of contraction. Computer methods in biomechanics and biomedical engineering, 3(3):231– 244. Rasmussen, J., Damsgaard, M., and Voigt, M. (2001). Muscle recruitment by the min/max criteriona comparative numerical study. Journal of Biomechanics, 34(3):409–415. Siemienski, A. (1992). Soft saturationan idea for load sharing between muscles. application to the study of human locomotion. In Cappozzo, A., Marchetti, M., and Virgilio, T., editors, Biolocomotion: A Century of Research Using Moving Pictures, pages 293–303. Acknowledgements I would like to thank Dr Phillips and his research team for their support and guidance throughout this project

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Page 1: Finite Element Representation of Muscles...Node 179 Node 204 Node 205 Node 206 Node 227 Node 228 Node 229 Node 264 Node 265 Node 266 Node 277 Node 278 Node 279 Figure 3: Force-strain

Finite Element Representation of MusclesPeter James Nugent, Supervisor: Dr. Andrew Phillips

Department of Civil and Environmental Engineering, Imperial College London

S16

Figure 1: Conversion from tetrahedral to truss elements Figure 2: Mesh of the muscle

Final Muscle Model• Utilised a hyper elastic material that accurately captured the passive response of the muscle (Figure 4)

• The model could be subject to both compressive and tensile forces (Figures 3 & 4)

• Eight connector elements around the exterior of the muscle induced the compressive force

• The wires that followed the geometry were similar to those found in the literature (Böl and Reese, 2008)

ϵ [-] ×10-3-4 -3 -2 -1 0 1 2 3 4

Forc

e [k

N]

-0.8

-0.6

-0.4

-0.2

0

0.2

0.4

0.6

0.8

1

Node 1Node 4Node 12Node 19Node 20Node 27Node 28Node 35Node 64Node 65Node 66Node 89Node 90Node 91Node 140Node 141Node 142Node 177Node 178Node 179Node 204Node 205Node 206Node 227Node 228Node 229Node 264Node 265Node 266Node 277Node 278Node 279

Figure 3: Force-strain graph in the X directionϵ [-]

-0.25 -0.2 -0.15 -0.1 -0.05 0 0.05 0.1 0.15 0.2

Forc

e [k

N]

-0.8

-0.6

-0.4

-0.2

0

0.2

0.4

0.6

0.8

1Node 13Node 14Node 17Node 18Node 32Node 34Node 41Node 43Node 101

Figure 4: Force strain graph in the Y direction

Figure 5: Anatomical model of the elbow system

Biceps brachii

Brachialis

Brachioradialis

Humerus

RadiusUlna

Figure 6: Elbow system in Abaqus

CPRESS

+0.000e+00+6.415e−01+1.283e+00+1.924e+00+2.566e+00+3.207e+00+3.849e+00+4.490e+00+5.132e+00+5.773e+00+6.415e+00+7.056e+00+7.698e+00

X

Y

Z

CPRESS

+0.000e+00+6.415e−01+1.283e+00+1.924e+00+2.566e+00+3.207e+00+3.849e+00+4.490e+00+5.132e+00+5.773e+00+6.415e+00+7.056e+00+7.698e+00

X

Y

Z

CPRESS

+0.000e+00+6.415e−01+1.283e+00+1.924e+00+2.566e+00+3.207e+00+3.849e+00+4.490e+00+5.132e+00+5.773e+00+6.415e+00+7.056e+00+7.698e+00

X

Y

Z

CPRESS

+0.000e+00+6.415e−01+1.283e+00+1.924e+00+2.566e+00+3.207e+00+3.849e+00+4.490e+00+5.132e+00+5.773e+00+6.415e+00+7.056e+00+7.698e+00

X

Y

Z

Figure 7: Contact pressure on the humerus

Aims• Create a generalised muscle model capable of being subject to compressive and tensile loads

• Implement the muscle model in to an elbow system and capture the interaction between the deformed muscle and the bone

Current Models• Existing muscle models use complex material sub routines that are computationally expensive

• Some focus on the microscopic and mesoscopic scale of muscles such as the binding between actin and myosin proteins (Gielen et al., 2000)

• Some also utilise MRI and CT scans that render the models subject specific

Mesh & Geometry• A mesh was created using tetrahedral elements, which were then converted to truss elements (Figure 1)

• This reduced the computational cost because truss elements have a single degree of freedom and hence can only deform axially, this is synonymous with the behaviour of a muscle

3D Elbow Mechanism• The biceps brachii was chosen as the muscle to model in three

dimensions because it makes contact with the humerus in the system that was adapted from the literature (Siemienski, 1992; Rasmussen et al., 2001)

• The brachialis and brachioradialas were modelled as wires

• The ulna and radius were combined to model the forearm (Figures 5 & 6)

• The contact between the biceps brachii and the humerus was modelled using a node to surface contact

Conclusions• The muscle model correctly captured the passive behaviour of the muscle and leaves scope for further

work to manipulate the active response of the muscle

• The elbow mechanism accurately modelled the contact pressure between the humerus and biceps brachii (Figure 7)

• A musculoskeletal model can be used to obtain muscle forces, implemented in to the elbow mechanism model and the resulting contact pressures can be applied to finite element models of bones

ReferencesBöl, M. and Reese, S. (2008). Micromechanical modelling of skeletal muscles based on the finite element method. Computer methods in biomechanics and biomedical engineering, 11(5):489–504. Gielen, A. W. J., Oomens, C. W. J., Oomens, C. W. J., Arts, T., and Janssen, J. D. (2000). A finite element approach for skeletal muscle using a distributed moment model of contraction. Computer methods in biomechanics and biomedical engineering, 3(3):231– 244. Rasmussen, J., Damsgaard, M., and Voigt, M. (2001). Muscle recruitment by the min/max criteriona comparative numerical study. Journal of Biomechanics, 34(3):409–415. Siemienski, A. (1992). Soft saturationan idea for load sharing between muscles. application to the study of human locomotion. In Cappozzo, A., Marchetti, M., and Virgilio, T., editors, Biolocomotion: A Century of Research Using Moving Pictures, pages 293–303.

AcknowledgementsI would like to thank Dr Phillips and his research team for their support and guidance throughout this project