Delphine Perie1, Mehdi Ghafari1, and Daniel Curnier2
1Mechanical Engineering, Polytechnique Montreal, Montreal, QC, Canada, 2Kinesiology, University of Montreal, Montreal, QC, Canada
Synopsis
Due to the
complexity of the heart’s geometry, the characterization of the material
properties of the myocardium remains challenging. Using kinematically
admissible hyperboloid virtual fields and a finite element mesh of the left
ventricle, we successfully solved the virtual field method equations to
determine the stiffness of the myocardium from a reverse identification
approach. The distribution of the elastic stiffness presented
same patterns between the 3 volunteers. However, the standard risk volunteer
presented higher stiffness within the mobile wall than the high risk volunteers.
This approach
would be an efficient tool to characterize early cardiac dysfunction.
Introduction
Due to the
complexity of the heart’s geometry, the characterization of the material
properties of the myocardium remains challenging. Modelling the mechanical behavior of soft tissues requires the knowledge of
the structure and mechanical properties of
the constitutive elements [1,2]. Finite elements models of the left ventricle,
associated to reverse identification methods are memory and time consuming. The objective of this study was to calculate
material properties of the left ventricle over the cardiac cycle using a
reverse identification method based on the 3D virtual field method [3,4] and
full-field data from cine-CMR.Methods
The data used in this study comes from the PETALE study [5]
in which the leukemia survivors were divided
into 3 groups according to their exposition risk to doxorubicin: standard risk
(SR), high risk (HR) and high-risk group who received dexrazoxane, a
cardioprotective agent (HRdex). The CMR acquisitions
were performed on a Siemens Skyra 3T MR system using a 18-channel phased array
body matrix coil and included an ECG-gated cine TruFISP sequence (14 slices in
short axis and 5 slices in long axis, slice thickness 8mm, repetition time
34.6ms, effective echo time 1.2ms, flip angle 38°, iPAT factor 3, matrix
208x210 and in-plane pixel size 1.25x1.25 mm). The data points of the epicardial
and endocardial left ventricle surfaces were semi-automatically extracted using
CIM (v8.1, University of
Auckland, [6]). These data points were imported in the 3D environment of CATIA
(Dassault Systems) to create curves for the geometrical reconstruction of the endocardial
and epicardial surfaces of the left ventricle. The volume delimited by these
surfaces was then meshed into 10,000 hexahedral linear elements in a prolate
spheroidal coordinate system (Figure 1). The displacement
field of left ventricle was calculated from the differences in data points coordinates
between each phase of the cardiac cycle (Figure 2). Intraventricular pressure,
estimated from electrophysiological data (arterial pressure, cardiac ouput and
heart rate), was applied to the endocardial
surface. The finite element mesh was then used to discretize the equations
of the principle of the virtual work. Using the theory of piecewise virtual
fields applied to the data, we identified two kinematically admissible hyperboloid
virtual fields (Figure 3) that allowed determining two unknown parameters, the global
hyperelasticity (C) and the elastic stiffness (Q11) of the left
ventricular myocardium. The data from one subject from each risk group of the
PETALE study were used to build the models and solve the equations of the
virtual field method.Results
The
equations of the virtual field method were successfully solved for each of the
3 data-sets. The elastic stiffness (Q11) of the left ventricular
myocardium varied from 1 to 15 kPa over the diastole cycle. It’s distribution
within the myocardium at end-diastole presented same patterns between the 3
volunteers (Figure 4). However, the SR volunteer presented higher stiffness
within the mobile wall than the HRdex and HR volunteers (maximum value of 14.5,
12 and 12.5 kPa for the SR, HR, and HRdex volunteers respectively).
The
hyperelastic parameter C increased almost linearly up to 11, 8 and 6 kPa in the
SR, HRdex and HR volunteers respectively (Figure 5).Discussion
The stiffness found using this reverse
identification technique based on the 3D virtual field method is in the same
range as reported data in the literature from finite element models [1,2]. The
convergence analysis showed the results sensitivity to the mesh size. The
results were also sensitive to the chosen virtual field. A small size of the
mesh and virtual fields defined in prolate spherical systems were found more
suitable for measuring the material parameters than those defined in spherical
coordinates. The quasi-static
hypothesis simplifies the complexity of the virtual field approach
developed in 3D. Incorporating the forces
of acceleration and virtual speeds instead of virtual displacements
would help estimate the distribution of the left ventricular mass and quantify inertial parameters. Higher stiffness
in the SR group on the mobile wall may suggest less interstitial fluid in diastole than
in the HR and HRdex groups.Conclusion
The
identification of the mechanical properties of the myocardium from a reverse identification technique based
on the 3D virtual field method would be an efficient tool to
characterize early cardiac dysfunction. The technique has the potential to be
easily implemented in the software of medical imaging equipments.Acknowledgements
NSERC and Polytechnique Montreal for
the financial support, researchers from the PETALE study for the opportunity to
do this complementary analyses on the cancer survivors.References
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