Karajan N, Otto D, Oladyshkin S, Ehlers W
Institute of Applied Mechanics (Civil Engineering), University of Stuttgart, Pfaffenwaldring 7, Stuttgart, 70569, Germany,
Biomech Model Mechanobiol. 2014 Oct;13(5):1065-80. doi: 10.1007/s10237-014-0555-y. Epub 2014 Feb 20.
A possibility to simulate the mechanical behaviour of the human spine is given by modelling the stiffer structures, i.e. the vertebrae, as a discrete multi-body system (MBS), whereas the softer connecting tissue, i.e. the softer intervertebral discs (IVD), is represented in a continuum-mechanical sense using the finite-element method (FEM). From a modelling point of view, the mechanical behaviour of the IVD can be included into the MBS in two different ways. They can either be computed online in a so-called co-simulation of a MBS and a FEM or offline in a pre-computation step, where a representation of the discrete mechanical response of the IVD needs to be defined in terms of the applied degrees of freedom (DOF) of the MBS. For both methods, an appropriate homogenisation step needs to be applied to obtain the discrete mechanical response of the IVD, i.e. the resulting forces and moments. The goal of this paper was to present an efficient method to approximate the mechanical response of an IVD in an offline computation. In a previous paper (Karajan et al. in Biomech Model Mechanobiol 12(3):453-466, 2012), it was proven that a cubic polynomial for the homogenised forces and moments of the FE model is a suitable choice to approximate the purely elastic response as a coupled function of the DOF of the MBS. In this contribution, the polynomial chaos expansion (PCE) is applied to generate these high-dimensional polynomials. Following this, the main challenge is to determine suitable deformation states of the IVD for pre-computation, such that the polynomials can be constructed with high accuracy and low numerical cost. For the sake of a simple verification, the coupling method and the PCE are applied to the same simplified motion segment of the spine as was used in the previous paper, i.e. two cylindrical vertebrae and a cylindrical IVD in between. In a next step, the loading rates are included as variables in the polynomial response functions to account for a more realistic response of the overall viscoelastic intervertebral disc. Herein, an additive split into elastic and inelastic contributions to the homogenised forces and moments is applied.
通过将较硬的结构(即椎体)建模为离散多体系统(MBS),同时使用有限元方法(FEM)以连续介质力学的方式表示较软的连接组织(即较软的椎间盘(IVD)),可以实现对人体脊柱力学行为的模拟。从建模的角度来看,IVD的力学行为可以通过两种不同的方式纳入MBS。它们既可以在MBS和FEM的所谓联合仿真中在线计算,也可以在预计算步骤中离线计算,在预计算步骤中,需要根据MBS的应用自由度(DOF)定义IVD离散力学响应的表示。对于这两种方法,都需要应用适当的均匀化步骤来获得IVD的离散力学响应,即产生的力和力矩。本文的目标是提出一种在离线计算中近似IVD力学响应的有效方法。在之前的一篇论文(Karajan等人,《生物力学模型与分子生物力学》,2012年,第12卷第3期,第453 - 466页)中,已经证明FE模型的均匀化力和力矩的三次多项式是将纯弹性响应近似为MBS自由度耦合函数的合适选择。在本论文中,应用多项式混沌展开(PCE)来生成这些高维多项式。在此之后,主要挑战是确定IVD用于预计算的合适变形状态,以便能够以高精度和低数值成本构建多项式。为了进行简单验证,将耦合方法和PCE应用于与前一篇论文相同的简化脊柱运动节段,即两个圆柱形椎体和其间的一个圆柱形IVD。下一步,将加载速率作为变量纳入多项式响应函数中,以考虑整个粘弹性椎间盘更实际的响应。在此,对均匀化力和力矩进行弹性和非弹性贡献的加法分解。