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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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modulation models like the proposed by Stokes et al [7] and Carter et al [10]. Carter et<br />

al [10] described an isotropic growth tensor in terms of the hydrostatic and deviatoric<br />

stresses, while Stokes et al [7] described the longitudinal growth as a function of the<br />

tensile or compressive axial stresses. These models were compared by Lin et al [11],<br />

revealing that the model of Carter et al [10] is less able to predict the growth retardation<br />

under compressive loads than the model proposed by Stokes et al [7]. Both models<br />

describe the ‘baseline’ growth rate as its mechanical modulation from a<br />

phenomenological point of view; therefore the bone elongation is simulated using<br />

equivalent thermal deformations [11].<br />

The main objective of this work is to develop a finite element model that describes the<br />

growth plate behavior and its mechanical modulation from a biological point of view.<br />

We used a two-dimensional domain inspired on the quantitative histology of a human<br />

growth plate [1]. The model was implemented on an ABAQUS User Element<br />

subroutine (UEL) and it was used to simulate the growth for a 2-years old, male human<br />

distal femur.<br />

3. MATEMATHICAL MODEL<br />

The mathematical model is based on the following assumptions:<br />

a) Given that the PTHrP-Ihh regulatory loop is highly stable in time [9], it is assumed<br />

that its mechanism of expression is insensitive to mechanical loads [13]. This<br />

explains, to some extent, the “in vitro” results reported by Villemure et al [14].<br />

b) The mathematical description of the cell distribution and concentration in the<br />

growth plate is performed by second-order transversely isotropic tensors [12],<br />

defined as<br />

R PC<br />

R HC<br />

CPC<br />

= 3<br />

PC 1<br />

r<br />

PC<br />

( 1 + ( r − ) n ⊗ n)<br />

CHC<br />

= 3<br />

HC 1<br />

r<br />

HC<br />

( 1 + ( r − ) n ⊗ n)<br />

, (1)<br />

, (2)<br />

where R PC and R HC are the proliferative and hypertrophic distribution tensors,<br />

respectively, r PC and r HC are the ratios of the number of proliferative and<br />

hypertrophic cells in the growth preferential direction n to the number of cells in<br />

the orthogonal direction, C PC and C HC are the concentrations of proliferative and<br />

hypertrophic chondrocytes and 1 is the unit second order tensor.<br />

c) According to Stokes et al [7] it is assumed that, in the growth direction, no<br />

extracellular matrix exists between the hypertrophic chondrocytes. In addition, it is<br />

supposed that all the new cells produced complete their maduration from the<br />

proliferative to the hypertrophic state. Therefore, the growth per day can be<br />

expressed as<br />

G n p h × = , (3)<br />

max

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