| Literature DB >> 28533757 |
Edoardo Borgiani1,2, Georg N Duda1,2, Sara Checa1,2.
Abstract
Bone is a living part of the body that can, in most situations, heal itself after fracture. However, in some situations, healing may fail. Compromised conditions, such as large bone defects, aging, immuno-deficiency, or genetic disorders, might lead to delayed or non-unions. Treatment strategies for those conditions remain a clinical challenge, emphasizing the need to better understand the mechanisms behind endogenous bone regeneration. Bone healing is a complex process that involves the coordination of multiple events at different length and time scales. Computer models have been able to provide great insights into the interactions occurring within and across the different scales (organ, tissue, cellular, intracellular) using different modeling approaches [partial differential equations (PDEs), agent-based models, and finite element techniques]. In this review, we summarize the latest advances in computer models of bone healing with a focus on multiscale approaches and how they have contributed to understand the emergence of tissue formation patterns as a result of processes taking place at the lower length scales.Entities:
Keywords: bone healing; computer modeling; multiscale modeling; systems biology; tissue regeneration
Year: 2017 PMID: 28533757 PMCID: PMC5420595 DOI: 10.3389/fphys.2017.00287
Source DB: PubMed Journal: Front Physiol ISSN: 1664-042X Impact factor: 4.566
Overview of the main properties of computer models of bone regeneration.
| Carter et al., | 2D | Tissue level | Finite element modeling | Identification of intermittent hydrostatic stress as an important stimulus in the regulation of tissue patterning during bone healing | |||
| Claes and Heigele, | 2D | Tissue level | Finite element modeling | Quantification of the levels of mechanical strain leading to intramembranous bone formation, endochondral ossification, and fibrocartilage formation. | |||
| Lacroix et al., | 2D | Tissue level | Finite element modeling | Coupled equations | The site of origin of the cells has an important influence on the healing pattern. | ||
| Cell population level | Partial differential equations | ||||||
| Bailon-Plaza and van der Meulen, | 2D | Tissue level | Partial differential equations + finite element modeling | Coupled equations | Demonstrated the dependence of successful healing on moderate mechanical loading, and the adverse effects of insufficient, delayed, or excessive mechanical stimulation | ||
| Cell population level | Partial differential equations | ||||||
| Gomez-Benito et al., | 3D | Tissue level | Partial differential equations + finite element modeling | Coupled equations | Low fixation stiffness delays fracture healing and causes a larger callus | ||
| Cell population level | Partial differential equations | ||||||
| Geris et al., | 2D | Tissue level | Partial differential equations | Coupled equations |
- The establishment of a vascular network in response to angiogenic growth factors as a key factor in the healing process. - A correct description of cell migration is essential to the prediction of realistic spatiotemporal tissue distribution patterns in the fracture callus. | ||
| Cell population level | Partial differential equations | ||||||
| Isaksson et al., | 2D | Tissue level | Partial differential equations + finite element modeling | Coupled equations | Identified matrix production rates of bone and cartilage, and cartilage replacement (degradation) as the most important parameters for the fracture healing process. | ||
| Cell population level | Partial differential equations | ||||||
| Nagel and Kelly, | 2D | Tissue level | Finite element modeling | Coupled equations | Collagen organization of the repair tissue is regulated by the local mechanical environment | ||
| Cell population level | Partial differential equations | ||||||
| Wehner et al., | 3D | Tissue level | Finite element modeling and fuzzy logic | Optimization of fixation stiffness for a reduced healing time. | |||
| Geris et al., | 2D | Tissue level | Partial differential equations+ finite element modeling | Coupled equations | The direct action of mechanics on both angiogenesis and osteogenesis was able to predict overload-induced non-union formation | ||
| Cell population level | Partial differential equations | ||||||
| Checa et al., | 3D | Tissue level | Finite element modeling +agent-based model | Coupled equations | Inter-species differences in the mechanical regulation of bone healing between sheep and rat | ||
| Cell level | Agent-based model | ||||||
| Byrne et al., | 3D | Tissue level | Finite element modeling+ agent-based model | Coupled equations | Prediction of tissue differentiation patterns in an human tibia under realistic muscle loads | ||
| Cell level | Agent-based model | ||||||
| Vetter et al., | 2D | Tissue level | Finite element modeling | Coupled equations | Fracture bridging of the periosteal side by cartilage was observed only (i) for a specific choice of the mechanical threshold values for tissue differentiation and (ii) when assuming a strong source of biological stimulation at the periosteum | ||
| Cell population level | Partial differential equations | ||||||
| Carlier et al., | 2D | Tissue level | Partial differential equations | Coupled equations |
- Increased tip cell density due to the loss of DII4 - Excessive number of tip cells in high VEGF environments - Absence of vascular network and fracture healing in very high VEGF environments | ||
| Cell population level | Partial differential equations | Passing of variables | |||||
| Cellular level | Agent-based model | Passing of variables | |||||
| Intracellular level | Set of equations | ||||||
| Steiner et al., | 3D | Tissue level | Finite element modeling and fuzzy logic | A fracture-healing model regulated by local distortional and dilatational strains was able to predict the course of IFM and tissue distribution of different healing situations under axial compression, torsion, shear loading, and bending. | |||
| Ribeiro et al., | 2D | Tissue level | Partial differential equations | Coupled equations | Bone healing in a large bone defect augmented with a BMP-2 soaked hydrogel as a result of the effect of BMP-2 on cellular activity | ||
| Cell population level | Partial differential equations | ||||||
Figure 1(A) Histological section (Safranin-O von Kossa staining) of sheep callus stabilized with an external fixator (9 weeks). (B) Map of elastic coefficient (GPa) of the same sample measured by quantitative acoustic scanning microscopy. (C) FEMs of callus region (black square B) under 10% compression showing the influence of callus tissue structure and heterogeneity on the mechanical strains within the healing region. High mechanical strains are induced in regions between the highly organized bone tissue, which cannot be predicted when describing the tissues as continuous and homogeneous materials.
Figure 2Although computer models of bone healing tend toward a multiscale approach to understand interactions between and within the different length and time scales, computer models at the intracellular level are still lacking.