The creation of foot-running shoe FE models involves several key steps, beginning with the acquisition of reliable geometric data for model reconstruction. In early research, symmetrical geometric shapes were often used for model construction, representing only partial structures. For instance, Verdejo and Mills (2004) and Even-Tzur et al. (2006) employed simple geometric forms, such as cylinders and spheres, to represent different foot and shoe components. Specifically, the calcaneus was modeled as a combination of a cylinder and hemisphere to capture its overall shape and curvature, while the heel pad was approximated using a thicker cylinder with a spherical lower surface to simulate its cushioning properties. The midsole was represented as a vertical cylinder, emphasizing its height and radius to replicate cushioning and support functions. Although these simplifications allowed for quicker modeling and analysis, they failed to capture the complex anatomical structures and interactions during movement. This limitation affects the model's ability to accurately reflect the biomechanical behavior of different foot shapes and sizes, leading to potential inaccuracies in results. To address these issues, researchers have increasingly turned to data from CT and MRI scans to develop more detailed and individualized models, thereby enabling a finer exploration of running biomechanics. Medical DICOM images of the foot and shoe are usually obtained by scanning the participant's leg in a shod condition using CT or MRI. These images are then segmented using medical image segmentation software, such as MIMICS (Materialise, Leuven, Belgium), to delineate the boundaries of bones, soft tissues, and the shoe, and are then utilized to reconstruct the 3D geometry. The resulting geometric models of the foot and shoe can be imported into reverse engineering software, such as SOLIDWORKS (Dassault Systèmes, Paris, France), for surface smoothing and solid model creation, including cartilages. Finally, these models are aligned and assembled to establish the coupled foot-shoe FE models. Typically, foot modeling involves extracting only the bones and the outer layer of soft tissue from the acquired images, with some bones fused for simplification. Other structures, such as cartilage, muscles, and connective tissues (e.g., tendons and ligaments), are manually reconstructed based on anatomical features. In some cases, researchers also reconstruct the 3D physical geometry of the Achilles tendon, given its crucial role in force generation during running activities (Li et al., 2019). For running shoe modeling, nearly half of the included studies reconstructed the two primary components: the upper and the sole. In some cases, the sole was further divided into insole, midsole, and outsole, and additional elements, such as CFP and heel cups, were modeled to explore their effects on foot biomechanics (Chen and Lee, 2015; Li et al., 2019; Yang et al., 2022; Zhu et al., 2023; Zhou et al., 2024b; 2024a). Non-structural features like shoelaces were often excluded to simplify the model. Additionally, it is important to note that some studies focused solely on the sole structure, neglecting the upper (Verdejo and Mills, 2004; Even-Tzur et al., 2006; Hannah et al., 2016; Nonogawa et al., 2021; Zhou et al., 2024a; 2024b). This omission can significantly affect the results, as foot deformation occurs when wearing shoes during dynamic simulations. The interaction between the foot and the shoe upper plays a critical role in influencing internal stress and strain patterns (Yu et al., 2013). After creating the foot-running shoe model, the next step is to mesh the model components. Each component is meshed individually using appropriate element geometries. In general, researchers aim to develop an optimal mesh density that balances model accuracy with computational efficiency. Depending on the shape of each component, commonly reported element geometries include triangular or quadrilateral elements for 2D FE models and tetrahedral, hexahedral, and pentahedral elements for 3D models. Tetrahedral elements were found used in most studies probably due to the complexity of human bone geometry and running shoe structures. Hexahedral elements, however, are more accurate and efficient for dynamic simulations, while tetrahedrals are preferred for discretizing complex surfaces (Burkhart et al., 2013). Some studies using simplified geometric models opted for hexahedral elements to improve accuracy, particularly for shoe components (Verdejo and Mills, 2004; Even-Tzur et al., 2006; Chen and Lee, 2015; Nonogawa et al., 2021). Additionally, localized mesh refinement is often applied in contact regions between the running shoe and the ground, as well as in areas with intricate geometries, to enhance mesh quality. Before running the simulation, several beams or axial 1D elements are incorporated into the mesh to represent the ligaments connecting different bones. This approach is widely regarded as one of the most efficient methods for simulating ligament behavior in the foot-ankle complex (Wang et al., 2016). Finally, the foot-running shoe model’s mesh is typically refined through a detailed mesh convergence study, ensuring a balance between computational efficiency and solution accuracy. Criteria such as plantar pressure and maximum vertical GRF are used to assess convergence, with a tolerance of less than 5% set for the mesh sensitivity analysis. Once the mesh is generated, various properties must be assigned to establish the simulation environment. These include material properties, contact interactions, constraints, boundary conditions, and loads. The accuracy of FE models for the foot-running shoe complex is highly dependent on the appropriate assignment of material properties to each component of the model, which mainly includes bones, muscles, ligaments, fascia, soft tissue, the shoe upper, and the shoe sole. These material properties would directly influence the model's response and, consequently, the validity of the simulation results (Phan et al., 2021). Typically, material parameters are derived from values reported in literature. For instance, bones are commonly represented as linear elastic materials, with a Young’s modulus of 0.73GPa (Cen et al. 2023). Similarly, muscles, fascia, and ligaments are often modeled as one-dimensional truss elements connecting anatomical insertion points, with varying lengths and cross-sectional dimensions, and assigned linear elastic properties with Young’s modulus of 0.45GPa, 0.35GPa, and 0.26GPa, respectively (Cen et al. 2023). Soft tissue and shoe soles, on the other hand, are frequently represented using non-linear hyperelastic models, such as the five-term Mooney-Rivlin model, to more accurately capture their rubber-like mechanical behavior (Li et al., 2019; Zhou et al., 2024a; 2024b). While many studies rely on literature-based material properties, some incorporate personalized material properties obtained from in vivo experiments (for foot tissues) and mechanical testing (for running shoes) into the models. For example, Yang et al. (2022) determined the mechanical properties of shoe midsoles and insoles through material testing of custom-sized EVA and Latex samples using a MicroTester and a push-pull tester, respectively. In general, despite the availability of more complex material models, linear elastic assumptions remain a common choice in FE modeling of the foot-shoe interaction due to their computational efficiency and feasibility for parametric studies. This simplification allows researchers to systematically examine variations in running mechanics, such as changes in contact angles and footwear features, without incurring excessive computational costs or significantly compromising result reliability. However, it is important to recognize that most studies employing this approach use a quasi-static modeling framework, either analyzing discrete time points within the stance phase or conducting multiple simulations at different instances of the stance phase (Verdejo and Mills, 2004; Even-Tzur et al., 2006; Li et al., 2019; Nonogawa et al., 2021; Yang et al., 2022; Zhu et al., 2023; Song et al., 2023; 2024; Zhou et al., 2024a; 2024b). Under dynamic loading conditions, where deformations and stress distributions evolve continuously, non-linear hyperelastic material models would be required to capture the complex mechanical behavior of both foot tissues and shoe components, given the substantial deformations relative to their geometric dimensions. Following the assignment of material properties, appropriate boundary and loading conditions must be applied to the model. Most simulations in this review utilized data derived from motion analysis and musculoskeletal modeling of the subject (Hannah et al., 2016; Nonogawa et al., 2021; Yang et al., 2022; Song et al., 2023; 2024; Zhu et al., 2023; Zhou et al., 2024a; 2024b). Common constraints and loads include running kinematics and kinetics, such as foot-ground angle, joint moments, joint contact forces, foot muscle forces, and GRF. In these simulations, a stiff plate is often attached to the outsole of the shoe model to simulate ground support. The proximal surfaces of the soft tissue, tibia, fibula, and the shoe tongue loop are typically fixed in all directions. Various running postures are replicated by adjusting the plate angle. For load applications, researchers either apply direct loads to the dorsal surface or use force vectors connected to specific bone insertion points to simulate the forces exerted by relevant joints and muscles. To simulate the running stance phase, a quasi-static approach is commonly preferred. However, some studies have explored dynamic modeling to analyze the mechanical response of human structures under varying running conditions and footwear designs. For example, Chen and Lee, (2015) developed a computational model of a body-heel-shoe system to investigate the mechanical behavior of the heel pad under realistic impact loads during running. By applying different touchdown velocities of the foot prior to landing, they examined how these variations influenced internal deformations and stress distribution within the heel pad. Beyond boundary and loading conditions, a crucial factor in ensuring realistic simulation outcomes is the proper definition of contact interactions within the model. The accuracy of force transmission and mechanical behavior depends on how material properties interact and transfer loads across contact surfaces. Most studies in this review define the interactions between the foot, shoe, and ground plate as frictional surface-to-surface contact using the isotropic Coulomb friction model. The coefficient of friction, originally determined by Zhang and Mak, (1999), generally ranges from 0.5 to 0.6. For interactions within the shoe-such as between the insole, midsole, and outsole-a surface-to-surface tying method is commonly employed to ensure structural cohesion. Some studies adjust the friction coefficient between the shoe and ground plate based on surface conditions, with values ranging from 1.0 to 1.5 (Chen and Lee, 2015). An alternative approach was proposed by Hannah et al. (2016), who developed a dynamic FE model of a shod footstrike. Instead of defining frictional contact between the foot and the shoe, they constrained adjacent foot and footwear surfaces solely using foot segment kinematics data. However, their results failed to meet validation criteria, limiting the practical applicability of this method. This underscores the critical role of interface contact, particularly in dynamic simulation scenarios, where accurate force transmission is essential. To conduct FE simulations after defining boundary and loading conditions, researchers have extensively used commercial software such as ANSYS (ANSYS, Canonsburg, PA, USA) and ABAQUS (Simulia, Johnston, RI, USA) (Table 2). Earlier studies also employed other research software, such as COSMOSWorks (Dassault Systèmes, Paris, France) (Even-Tzur et al., 2006). The computational cost (simulation run time) is normally influenced by the processor configurations of the computing planforms used. However, as shown in Table 2, despite improvements in the number and power of processors, the overall simulation run time has not significantly decreased. This may be directly related to the increased complexity of the models. In general, researchers always strive to achieve an optimal balance between computational expense and accuracy, without assuming the necessity of acquiring high-performance computing hardware or costly commercial FE analysis software licenses. Finally, the results of the FE simulation must be validated to ensure consistency with experimental findings. Most foot-running shoe FE models in this review were validated by comparing the distribution and peak values of plantar and outsole pressures with experimental data or published literature (Verdejo and Mills, 2004; Chen and Lee, 2015; Li et al., 2019; Nonogawa et al., 2021; Yang et al., 2022; Song et al., 2023; 2024; Zhu et al., 2023). Based on the findings of Zhang et al., (2007), an error of less than 10% is considerable between the computational and experimental data. For studies using dynamic modeling approaches, validation was achieved by comparing ground reaction forces, the center of pressure, and soft tissue deformation over time (Chen and Lee, 2015; Hannah et al., 2016). This is particularly effective as dynamic models simulate a portion of the stance phase during running, rather than just a single moment. Additionally, statistical methods are increasingly being used for validation (Song et al., 2023; 2024). Pearson correlation coefficients and intraclass correlation coefficients (ICC) are calculated to evaluate the agreement between simulation and experiment. The Bland-Altman plot is also employed to assess bias and establish limits of agreement between the two methods. |