Journal of Cellular Immunotherapy 4 (2018) 44–47
Contents lists available at ScienceDirect
Journal of Cellular Immunotherapy journal homepage: www.elsevier.com/locate/jocit
Theoretical numerical modeling of the oxygen diffusion effects within the periodontal ligament for orthodontic tooth displacement Camille Spingarna, Delphine Wagnerb, Yves Rémonda, Daniel Georgea,∗ a b
ICUBE Laboratory, University of Strasbourg, CNRS, 67000, Strasbourg, France Dental Faculty, 8, rue Sainte Elisabeth, 67000, Strasbourg, France
ARTICLE INFO
ABSTRACT
Keywords: Oxygen concentration Osteoblast Orthodontics Bone remodelling Tooth movement
Orthodontic tooth movement results from alveolar bone remodelling around the tooth. With applied mechanical forces, the periodontal ligament and its vascularization are deformed, the blood flow changes and so the amount of oxygen import, provoking, through cell density variation, bone remodelling and tooth movement. A numerical finite element (FE) model is presented in which the amount of oxygen and the cells densities of osteoclasts and osteoblasts are deduced from the oxygen variation inside the deformed periodontal ligament, leading to bone remodelling. Predicting this evolution will help the orthodontists in their decision making for patient dependent treatments.
1. Introduction Bone is a living material in continual renewal. Trying to model its evolution has been going on for a long time at continuous and microstructural levels [1,2]. Although lately sophisticated theoretical numerical models were developed [3–13], precise understandings of the coupled multiphysical multiscale underlying physics are still difficult to comprehend [14–17]. During orthodontic treatment, the bone adapts to the applied mechanical forces [18,19] on the teeth. While in orthopaedics, mechanical unloading is usually related to boneresorption and mechanical loading with bone remodelling, in orthodontics, a compressed bone shows boneresorption in front of the tooth, while tension shows bone reconstruction at the back, allowing the displacement of the tooth [20]. The exact process of bone remodelling for orthodontic tooth movement is still unknown but it is usually accepted that the periodontal ligament (PDL) plays a crucial role as it is highly vascularized (about 10%) and impacts directly on the cell differentiation processes through the oxygen concentration variation. The important blood supply involves a significant turnover of cells [21]. Under low amplitude forces, the ligament's vascularization is partially deformed resulting in a cell density change and differentiation, and bone remodelling leading to the tooth motion. When the PDL is completely compressed (above a given force level) and no longer vascularized, necrosis of the surrounding tissue occurs [22]. Deformation of the ligament is therefore the key factor for a good orthodontic movement
[23]. It is known that angiogenesis plays a key role in osteogenesis, but it also influences the multiplication of osteoblasts (responsible of bone construction) and osteoclasts (responsible of bone resorption). Two studies [24,25] extracted osteoblastic and osteoclastic cells from rats and analysed their evolutions at different level of oxygen. They concluded that osteoclasts multiply in hypoxia [24] and osteoblasts multiply with increase of oxygen [25]. This can be linked to the oxygen concentration variation in the vascularized PDL and play a role in the cells differentiation leading to the bone remodelling process in orthodontics. Here, a theoretical numerical model is developed to predict cell multiplication in the PDL and predict bone remodelling initiation for orthodontic application. 2. Material and methods The developed model is implemented within the software ABAQUS [26] through a UMAT subroutine encoded in FORTRAN. The bone, the teeth and the ligament are considered homogeneous and isotropic with a linear elastic mechanical behaviour. Their material properties are extracted from the literature [27,28]. The vascularization of the ligament is considered homogeneously distributed throughout the volume leading to an oxygen concentration variation equal to the relative volume variation of the ligament as:
cO 2 = f
Vvasc (t ) Vinit
= f {Tr [ (t )]}
Peer review under responsibilfity of Shanghai Hengrun Biomedical Technology Research Institute. ∗ Corresponding author. E-mail address:
[email protected] (D. George). https://doi.org/10.1016/j.jocit.2018.09.011
Available online 12 September 2018 2352-1775/ © 2018 Shanghai Hengrun Biomedical Technology Research Institute. Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/BY-NC-ND/4.0/).
(1)
Journal of Cellular Immunotherapy 4 (2018) 44–47
C. Spingarn et al.
Table 1 Variation of cells percentage over oxygen concentration variation according to oxygen concentration calculated from experiments [24,25]. Oxygen concentration c O2 (%)
Variation of percentage of cells over variation of oxygen concentration osteoclasts variation (%) oxygen concentration variation
osteoblasts variation (%) oxygen concentration variation
0.2 to 1 1 to 2 2 to 5 5 to 12 12 to 20
0.075 0.40 −0.30 −0.31 −0.38
4.65 −2.16 3.32 0.21 0.88
0
0.2
sr
dosteoblasts (t0)
dosteoclasts (t0)
1.15
4.6
1.8/100 μm2
0.45/100 μm2
th tens
0.5
Tr ( ) th tens
th comp th comp
Tr ( ) <
th comp
if
Tr ( ) >
th tens
else
(2)
The threshold and are hypothesised with being the threshold compressive strain of the PDL below which no more oxygen variation is set, with a limit of oxygen concentration of 0%, and th tens being the threshold tensile strain of the PDL above which no more oxygen variation is set, and with a limit oxygen concentration of 20% [24,25]. In addition, we hypothesise that the oxygen concentration, and the cells concentration, varies proportionally with blood volume variation through the variable Tr ( ) . The cell density variations as a function of oxygen concentration are calculated from available experimental data [24,25]. These variations are presented in Table 1. Also, as defined by Arnett et al. and Utting et al. [24,25], assumption is made in the current work that there is equilibrium between osteoblasts and osteoclasts activity at the average oxygen concentration of 10% in the blood (normal physiological level). The bone remodelling process leading to the tooth displacement occurs at the interface between the bone and the PDL. Hence, only the cells located at this interface are considered active. An algorithm is developed (similar to the one developed in Ref. [29] for detecting the bone trabecular surface) to localize the cells close to the bone/PDL interface that enables to track its moving in space. To carry out the bone density evolution analysis, input data are required. Histology experiments were carried out on pig's PDL teeth to quantify the initial cells density distribution. An average density of 1.8 ( ± 3) osteoblasts per 100 μm2 was determined into the ligament. As it is defined that bone kinetic resorption is about four times faster than bone kinetic reconstruction [30], we assumed that the osteoclasts density is four times smaller than the osteoblasts one at 10% oxygen concentration. This leads to an average density of 0.45 osteoclasts per 100 μm2. Finally, the percentage of bone density variation at the interface is calculated from the given cells density and associated kinetics as: th comp (≤0)
Table 2 Definition of the parameters used in the current model. ss
0.2
cO 2 =
if
th comp
−0.5
d Fig. 1. Simplified 3D model of tooth within PDL and bone.
bone
dt
= ss . dosteoblasts
th tens
sr . dosteoclasts
th comp
(3)
where dosteoblasts and dosteoclasts are the number of active cells, ss and sr are respectively the velocity of forming and resorbing the bone density percentage per unit cell. The data used in the current model are resumed in Table 2. Tooth movement in orthodontics requires the application of both forces and moments to get the proper tooth displacement. This is a rather complex scenario to implement. Hence, a simpler analysis is developed with only a uniaxial force leading to a simple rotation of the tooth. To highlight the effects of oxygen impact on the bone remodelling process, a simplified 3D geometry model is developed (see Fig. 1)
Where cO2 is the oxygen concentration into the PDL, Vvasc is the variation of the volume of the PDL, Vinit its initial volume and Tr ( ) , the trace of the strain tensor. The function f is assumed to be with a linear variation and defined such that no deformation is set for an oxygen concentration of 10% (as the normal average concentration in the blood). The function f provides the oxygen concentration with:
Fig. 2. (a) PDL strain distribution, (b) variation of oxygen concentration, (c) variation of active osteoblasts density, and (d) variation of active osteoclasts density into the PDL with an applied force of 1.5 N on the teeth. 45
Journal of Cellular Immunotherapy 4 (2018) 44–47
C. Spingarn et al.
Fig. 3. Time evolution of bone density around the teeth with an orthodontic force of 1.5N (x100%).
characterize the oxygen variation within the PDL, hence the bone cells multiplication/activation process. From these, bone density evolution could be predicted for a simplified geometry through coupled mechanobiological parameters. These could, at term, be applied on real patients’ cases, to help the orthodontist procedures.
including bone, tooth and PDL. The thickness of the PDL is set as 0.2 mm as reported in the literature [31]. The orthodontic force is set at 1.5 N [18–20] as a surface tension. The external surface of the bone is fixed. The model is meshed with 8 noded linear bricks (C3D8 element of Abaqus). The model includes 9856 hexahedral elements and 10566 nodes.
References
3. Results and discussion
[1] Weinans H, Huiskes R, Grootenboer HJ. The behavior of adaptative bone remodeling simulation models. J Biomech 1992;25:1425–41. [2] Ruimerman R, Hilbers P, van Rietbergen B, Huiskes R. A theoretical framework for strain-related trabecular bone maintenance and adaptation. J Biomech 2005;38:931–41. [3] Madeo A, Lekszycki T, Dell'Isola F. A continuum model for the bio-mechanical interactions between living tissue and bio-resorbable graft after bone reconstructive surgery. C R Mécanique 2011;339:625–40. [4] Madeo A, George D, Lekszycki T, Nierenberger M, Rémond Y. A second gradient continuum model accounting for some effects of micro-structure on reconstructed bone remodeling. C R Mécanique 2012;340:575–89. [5] Madeo A, George D, Rémond Y. Second gradient models for some effects of microstructure on reconstructed bone remodeling. Comp Meth Biom Biomed Eng 2013;16:S260–1. [6] Andreaus U, Giorgio I, Lekszycki T. A 2-D continuum model of a mixture of bone tissue and bio-resorbable material for simulating mass density redistribution under load slowly variable in time. ZAMM 2014;94:978–1000. [7] Scala I, Spingarn C, Rémond Y, Madeo A, George D. Mechanically-driven bone remodeling simulation: application to LIPUS treated rat calvarial defects. Math Mech Sol 2016;22(10):1976–88. [8] George D, Spingarn S, Dissaux C, Nierenberger M, Abdel Rahman R, Rémond Y. Examples of multiscale and multiphysics numerical modeling of biological tissues. Bio Med Mater Eng 2017;28:S15–27. [9] Bednarczyk E, Lekszycki E. A novel mathematical model for growth of capillaries and nutrient supply with application to prediction of osteophyte onset. ZAMP 2016;67:94. [10] Lu Y, Lekszycki T. A novel coupled system of non-local integro-differential equations modelling Young's modulus evolution, nutrients' supply and consumption during bone fracture healing. ZAMP 2016;67:111. [11] George D, Allena R, Rémond Y. Mechanobiological stimuli for bone remodeling: mechanical energy, cell nutriments and mobility. Comp Meth Biomech Biomed Eng 2017;20:S91–2. [12] Goda I, Ganghoffer JF, Czarnecki S, Wawruch P, Lewinski T. Optimal internal architecture of femoral bone based on relaxation by homogenization and isotropic material design. Mech Res Com 2016;76:64–71. [13] Rémond Y, Ahzi S, Baniassadi M, Garmestani M. Applied RVE reconstruction and homogenization of heterogeneous materials. Wiley-ISTE; 2016. ISBN: 978-1-84821901-4. [14] Lemaire T, Capiez-Lernout E, Kaiser J, Naili S, Sansalone V. What is the importance of multiphysical phenomena in bone remodelling signals expression? A multiscale perspective. J Mech Behav Biom Mat 2011;4(6):909–20. [15] Lemaire T, Kaiser J, Sansalone V. Three-scale multiphysics modeling of transport phenomena within cortical bone. Math Prob Eng 2015;2015:398970. [16] Sansalone V, Gagliardi D, Descelier C, Haiat G, Naili S. On the uncertainty propagation in multiscale modeling of cortical bone elasticity. Comp Meth Biom Biomed Eng 2015;18:2054–5.
Fig. 2 shows, in the ligament and for an applied force of 1.5N, the developed strain, the oxygen concentration, active osteoclasts density, and active osteoblasts density. As expected, the largest variations are located at places where the PDL deformations are highest (compression and tension sides). Due to the low force applied and the defined hypotheses, the oxygen concentration shows a small variation, which is followed by corresponding variations of cell densities. It is possible that the oxygen concentration variation due to small strains may be more important in particular through the porosity of the vascular network. This needs to be addressed experimentally in future works. Nevertheless, the variations of cell densities generate, through the applied mechanical force, a variation in the cell activation process leading to the bone remodelling. Following equation [3], the results for the bone density evolution are presented in Fig. 3. As described previously, the bone density is resorbed in the compressed area (at the front). On the contrary, the bone is constructed in the area under tension (at the back). Although the experimental quantification of the model parameters need be extracted, results show the bone density variations with very small applied mechanical forces through oxygen variations. Here, the bone remodelling simulation is based not on strain energy density as in the usual bone remodelling numerical models [1–8], but only on biological quantities being determined via the applied mechanical forces. These could help in more detailed definition of multiphysics coupled mechanobiological theoretical-numerical models as for example in Ref. [11], and integrating more realistic load cases to help the orthodontists in the prediction of patient specific tooth movement. 4. Conclusion Orthodontists require predictive models to decide on optimum procedure to correct patients' malocclusions. The teeth realignment being oxygen PDL dependent, a theoretical numerical model was developed and implemented within a finite element numerical model to 46
Journal of Cellular Immunotherapy 4 (2018) 44–47
C. Spingarn et al. [17] Martin M, Lemaire T, Haiat G, Pivonka P, Sansalone V. A thermodynamically consistent model of bone rotary remodeling: a 2D study. Comp Meth Biomech Biomed Eng 2017;20(S1):127–8. [18] Wagner D, Bolender Y, Rémond Y, George D. Mechanical equilibrium of forces and moments applied on orthodontic brackets of a dental arch: correlation with literature data on two and three adjacent teeth. Bio Med Mater Eng 2017;28:S169–77. [19] Wagner D, Bolender Y, Rémond Y, George D. Experimental quantification of the mechanical forces and moments applied on three adjacent orthodontic brackets. Bio Med Mater Eng 2017;28(S1):S179–84. [20] Cattaneo PM, Dalstra M, Melsen B. Strains in periodontal ligament and alveolar bone associated with orthodontic tooth movement analyzed by finite element. Orthod Craniofac Res 2009;12(2):120–8. [21] Tuncay OC, Daphne Ho BS, Melissa K, Barker BS. Oxygen tension regulates osteoblast function. Am J Orthod Dent Orthop 1994;105(5):457–63. [22] Liao Z, Chen J, Li W, Darendeliler MA, Swain M, Li Q. Biomechanical investigation into the role of the periodontal ligament in optimising orthodontic force: a finite element case study. Arch Oral Biol 2016;66:98–107. [23] Toms SR, Lemons JE, Bartolucci AA, Eberhardt AW. Nonlinear stress-strain behavior of periodontal ligament under orthodontic loading. Am J Orthod Dentofacial Orthop 2002;122(2):174–9.
[24] Arnett TR, Gibbons DC, Utting JC, Orriss IR, Hoebertz A, Rosendaal M, et al. Hypoxia is a major stimulator of osteoclast formation and bone resorption. J Cell Physiol 2003;196(1):2–8. [25] Utting JC, Robins SP, Brandao-Burch A, Orriss IR, Behar J, Arnett TR. Hypoxia inhibits the growth, differentiation and bone-forming capacity of rat osteoblasts. Exp Cell Res 2006;312:1693–702. [26] ABAQUS v6.12 [Computer software]. SIMULIA. [27] Zargham A, Geramy A, Rouhi G. Evaluation of long-term orthodontic tooth movement considering bone remodeling process and in the presence of alveolar bone loss using finite element method. Orth Waves 2016;75:85–96. [28] Fongsamootr T, Suttakul P. Effect of periodontal ligament on stress distribution and displacement of tooth and bone structure using finite element simulation. Eng J 2014;19:99–108. [29] Yi W, Wang C, Liu X. A microscale bone remodeling simulation method considering the influence of medicine and the impact of strain on osteoblast cells. Finite Elem Anal Des 2015;104:16–25. [30] Burr DB, Allen MR. Basic and applied bone biology. Academic Press; 2013. p. 390. ISBN: 9780123914590. [31] Bourauel C, Vollmer D, Jäger A. Application of bone remodeling theories in the simulation of orthodontic tooth movements. J Orofac Orthop 2000;61:266–79.
47