Introduction

Total hip prosthesis remains one of the most effective orthopedic solutions for restoring mobility1 and alleviating pain2 in patients with degenerative3, traumatic4, or congenital5 hip joint conditions. The total hip prosthesis helps millions of patients around the world regain functional independence and enhance their quality of life by substituting biomechanical parts such as the femoral stem, femoral head, acetabular cup, and acetabular shell for the natural hip joint6. The mechanical articulation between the femoral head and the acetabular cup functions as the central bearing interface, accommodating complex joint motion7 and withstanding substantial biomechanical loads8 during routine activities. Achieving long-term prosthesis durability and reducing the risk of revision surgery necessitates the use of optimal materials and structural designs capable of enduring physiological stress over extended periods.

The tribological and mechanical performance of total hip prosthesis components is critically dependent on the biomaterials used. Traditional bearing surfaces have employed polymers9, metals10, and more recently, advanced ceramics11. While polymers offer low friction12 and good biocompatibility13, they tend to produce wear debris that can trigger osteolysis14, chronic inflammation15, and eventual implant loosening16, leading to revision surgeries17. Metals, though mechanically robust18 and widely used19, but can corrode over time20 and release metallic ions into surrounding tissues21, potentially causing metallosis22 and systemic toxicity23. In contrast, ceramic materials particularly aluminum oxide (Al2O2), zirconium dioxide (ZrO₂), and silicon nitride (Si2N4) exhibit superior wear resistance24, excellent biocompatibility25, and high corrosion resistance26. Among these, Al2O2 stands out as a preferred material for ceramic-on-ceramic bearings due to its exceptional hardness27, high compressive strength28, chemical inertness29, and outstanding scratch resistance30 under high contact stress conditions. Its low coefficient of friction31 and minimal wear generation32 further enhance its clinical appeal by reducing the risk of osteolysis. Compared toZrO2, which may undergo phase transformation under stress33, and Si2N4, which presents challenges in fabrication34 and long-term in vivo and in vitro validation35, Al2O2 offers a well-documented history of clinical success36 and material stability37.

A critical design parameter influencing the functional performance of ceramic-on-ceramic bearings in total hip prosthesis is radial clearance, which defined as the intentional gap between the femoral head and the acetabular cup illustrated in Fig. 1. This clearance significantly affects contact mechanics by altering the distribution and peak values of contact pressure38, which in turn influence wear behavior39, lubrication regimes40, and localized stress patterns41 at the articulating surfaces. Alongside radial clearance, other geometric parameters such as femoral head diameter and acetabular cup thickness also play key roles in defining the load-bearing capacity and mechanical response of the joint. Larger femoral head diameters are generally associated with improved joint stability42 and a reduced risk of dislocation43, but may introduce greater frictional torque44 and altered stress paths45. Conversely, acetabular cup thickness contributes to structural integrity46 and resistance to fracture47, particularly under cyclic loading. However, among these parameters, radial clearance remains especially critical in ceramic-on-ceramic systems where wear is minimal and fracture becomes the dominant failure mode due to the brittle nature of ceramic materials like Al2O2. Both excessive and insufficient clearances can lead to unfavorable outcomes ranging from micromotion48, edge loading49, and instability50 to increased stress concentrations that may precipitate crack initiation51. Therefore, precise optimization of radial clearance is essential for achieving biomechanically favorable conditions that minimize the risk of catastrophic failure and enhance the long-term performance of ceramic hip implants.

Fig. 1
figure 1

Illustration of radial clearance parameter on the bearing of total hip prosthesis (with part of the figure has been adapted from Hansen137.  The figure was drawn by the authors using Microsoft Visio Professional 2019 (Microsoft Corporation, https://www.microsoft.com).

In the context of total hip prosthesis biomechanics, stress analysis is essential for evaluating implant safety, understanding failure mechanisms, and guiding design optimization. Classical failure theories based on yield criteria are commonly employed to assess the mechanical integrity of prosthetic components under physiological loading. Among these, von Mises stress is widely utilized due to its applicability to isotropic materials under complex stress states, and has been adopted in numerous hip prosthesis studies, including those by Ismail et al.52, Göktaş et al.53, and Chethan et al.54. In contrast, the Tresca criterion, which is based on maximum shear stress offers a more conservative assessment by defining a smaller allowable stress zone55, making it particularly valuable in safety–critical applications. Although its use in total hip prosthesis research has been relatively limited, Tresca stress has been effectively applied in other medical implant-related investigations, as reported by Moser et al.56, Mabrouk et al.57, and Farroukh et al.58. While Tresca stress is traditionally associated with ductile materials59,60,61, its application in the analysis of ceramic components is justified when used for comparative stress evaluation. This is especially relevant for Al2O2 as commonly used ceramic in hip bearings, which possesses high compressive strength62, but comparatively low shear resistance63. Mapping regions of elevated shear stress through Tresca analysis can provide valuable insight into areas prone to crack initiation, thereby contributing to the early identification of mechanical risk in brittle ceramic components and informing safer prosthesis design.

Advancements in computational modeling have significantly transformed the way complex engineering and biomedical problems are investigated. Among the various numerical techniques, finite element analysis has emerged as a powerful and widely utilized method for assessing the mechanical behavior of structures under various loading64, material65, and geometry66 conditions. Its ability to replicate conditions that are difficult or impractical to reproduce experimentally makes it particularly valuable for evaluating design alternatives67, identifying critical stress concentrations68, and predicting mechanical failure modes69. In the field of orthopedic implant research, especially total hip prosthesis, finite element analysis has been extensively used to analyze the mechanical performance of bearing components under physiological loads. While 3D models offer detailed representations of joint anatomy, triaxial motion, and complex contact behavior as done by Hidayat et al.70, Wibowo et al.71, and Alpkaya and Mihcin72, they require significant computational resources and time. To address this challenge, many studies have employed 2D axisymmetric models that simplify the ball-in-socket geometry of total hip prostheses performed by Saputra et al.73, Jamari et al.74, and Lestari et al.75. This approach enables efficient simulation of symmetric loading conditions, such as those encountered during normal gait, while maintaining accuracy in stress evaluation.

This study aims to investigate the influence of radial clearance on Tresca stress distribution in Al2O2-on-Al2O3 bearings used in total hip prosthesis, where is a continuation of our previous work investigating various ceramic materials for ceramic-on-ceramic bearing that can be found on Ammarullah et al.76. Using a 2D axisymmetric finite element model, the authors simulate the mechanical behavior of the bearing system under a physiologically representative walking cycle comprising 32 load phases. Six radial clearance values (0.03 mm, 0.05 mm, 0.075 mm, 0.1 mm, 0.15 mm, and 0.3 mm) are examined to identify the configuration that minimizes maximum Tresca stress and thereby reduces the risk of fracture. The outcomes of this work provide critical insights into stress-based performance optimization for Al2O2-on-Al2O3 hip bearings and contribute toward the development of safer, more reliable implant designs.

Materials and methods

Geometry parameters

The geometric configuration used in this study was based on widely adopted design standards bearings in total hip prosthesis, as reported in Ramadhoni et al.77. These parameters were selected to ensure relevance to clinically used implant designs and to facilitate comparison with existing literature78. The baseline model consists of a femoral head with a radius of 14 mm articulating against an acetabular cup with a wall thickness of 5 mm. To investigate the effect of radial clearance on mechanical safety from the perspective of Tresca stress distribution, six clearance values were adopted from Shankar and Nithyaprakash79 were examined: 0.03 mm, 0.05 mm, 0.075 mm, 0.1 mm, 0.15 mm, and 0.3 mm, as summarized in Table 1.

Table 1 Geometry parameters of Al2O3-on-Al2O3 bearings.

The implementation of these clearances in the finite element model was carried out by systematically modifying the internal radius of the acetabular cup, while keeping the femoral head radius constant at 14 mm for all cases. This approach allowed for precise control over the radial clearance without altering the overall geometry or dimensions of the femoral component. Furthermore, the outer diameter of the acetabular cup was adjusted accordingly to maintain a constant cup thickness of 5 mm across all simulations. This ensured structural consistency and comparability among the models, allowing the observed stress variations to be attributed solely to differences in radial clearance.

Material properties

In this study, the mechanical behavior of Al2O2 used in the ceramic-on-ceramic bearing components was modeled under the assumptions of homogeneous, isotropic, and linear elastic referred from Gutmann et al.80. A Young’s modulus and a Poisson’s ratio were applied for Al2O2 acetabular cup and femoral head taken from Shankar et al.81. These parameters reflect the material’s ability to resist elastic deformation under compressive loads, which is critical in load-bearing applications such as total hip prostheses. The constant coefficient of friction between the articulating surfaces Al2O2 femoral head and Al2O2 acetabular cup adopted from Uddin and Zhang82. Detailed computational simulation input for modelling materials behaviour presented in Table 2.

Table 2 Computational simulation input for modelling materials behaviour of Al2O3-on-Al2O3 bearings.

Finite element simulation of Al2O3-on-Al2O3bearing

The finite element analysis conducted in this study focused exclusively on the articulation between the Al2O2 femoral head and Al2O2 acetabular cup, which together form the core load-bearing interface in total hip prostheses. To achieve computational tractability while preserving geometrical relevance, a 2D axisymmetric model was developed based on a ball-in-socket configuration, simplifying the inherently 3D joint into a rotationally symmetric quarter-circle geometry presented in Fig. 2. This modeling approach has been validated in prior studies and is particularly suitable for symmetric loading conditions such as those reported from the previous study76.

Fig. 2
figure 2

Finite element model of Al2O2-on-Al2O3 bearing with varying radial clearance(with part of the figure has been adapted from Hansen137). The figure was drawn by the authors using Microsoft Visio Professional 2019 (Microsoft Corporation, https://www.microsoft.com).

Simulations were performed using ABAQUS CAE 6.14-1 (Dassault Systèmes, Vélizy-Villacoublay, France) employing a static loading scheme with implicit solver routines83. The contact between the femoral head and acetabular cup was modeled under dry conditions, reflecting the low-lubrication behavior of ceramic-on-ceramic interfaces84. Contact modeling was defined through surface-to-surface interactions using a master–slave algorithm, with the acetabular cup designated as the master surface85. An adiabatic contact process was assumed to capture time-independent interaction behavior, adopting Alpkaya and Mihçin86. Regarding boundary conditions, the outer surface of the acetabular cup was fully constrained in all directions to replicate its fixation within the pelvic bone as referred from Alpkaya et al.87. The femoral head was subjected to an axial compressive load applied at the lower edge of the axisymmetric boundary to represent gait-induced forces during normal walking. Lateral displacements were restricted, allowing only vertical translation to simulate physiological load transfer through the femoral stem88.

A detailed mesh convergence study (see Section "Mesh convergence study") was conducted to ensure numerical stability and solution accuracy. The final mesh configuration consisted of approximately 5500 four-node axisymmetric elements (CAX4) that have been used in several previous study from Močilnik et al.89, Esmaeili and Rizvi90, and Han et al.91, with 2000 elements assigned to the femoral head and 3500 elements to the acetabular cup. Mesh density was refined at the articulating surfaces to improve the resolution of contact stresses and ensure convergence of peak stress values across all simulated conditions.

Mesh convergence procedure

To ensure the reliability and accuracy of the finite element simulations, a mesh convergence study was conducted using the h-refinement technique, as described by Ramlee et al.92. This method involves systematically increasing the number of elements in the model to evaluate how solution outputs, specifically Tresca stress that stabilize with finer discretization. The convergence study was performed on the Al2O2-on-Al2O3 bearing model configured with a radial clearance of 0.3 mm, selected to represent a worst-case scenario in terms of potential stress amplification. Across all models, boundary conditions, loading (derived from the peak stance phase of the gait cycle), material definitions, and contact properties were kept constant to isolate the influence of mesh density on the computed stress field.

Six levels of mesh density were applied, ranging from an initial coarse mesh of 13 total elements to an ultra-refined mesh of 550,000 elements. Element refinement was performed independently in the femoral head and acetabular cup, with additional emphasis on the contact interface, where high stress gradients are expected. The purpose of this procedure was to determine the minimum mesh density required to achieve convergence without incurring excessive computational cost.

Human gait cycle

To simulate physiologically relevant loading conditions representative of daily activities, this study incorporated a quasi-static loading profile based on the human gait cycle referred from Saputra et al.93. Normal walking is the most frequent and clinically relevant activity performed by patients following total hip replacement surgery94, and thus serves as a valuable framework for evaluating stress behavior in implant components95. The loading data were adapted from Shankar et al.96, who modelled the hip joint forces during a complete gait cycle. The cycle was discretized into 32 load phases, capturing the full range of biomechanical loading experienced throughout a single step, which is a common values that can be found in an established study by Yu and Zhang97, Nithyaprakash et al.98, and Liu et al.99. The cycle is conventionally divided into two primary phases: the stance phase, comprising 60% of the cycle, during which the limb bears weight; and the swing phase, accounting for the remaining 40%, when the limb is in motion without ground contact100. The peak loading phase occurs at the 7th phase, where the hip joint is subjected to a maximum force of 2326.09 N, corresponding to approximately 3.5 times the body weight of an average adult.

Due to the geometric constraints of the 2D axisymmetric ball-in-socket model, dynamic joint kinematics such as rotation, flexion–extension, and femoral offset were not incorporated in this study. Instead, the analysis focused exclusively on axial loading conditions, which dominate during mid-stance and allow for meaningful stress evaluations under symmetric and repeatable load application. This modeling decision enables clear isolation of radial clearance effects on internal stress behavior without the added variability of joint orientation. The applied gait cycle used in the simulation is presented in Fig. 3, illustrating the temporal distribution and magnitude of joint reaction forces throughout the cycle.

Fig. 3
figure 3

Gait cycle loading profile adapted from Shankar et al.96 (with part of the figure has been adapted from Hansen137). The figure was drawn by the authors using Microsoft Visio Professional 2019 (Microsoft Corporation, https://www.microsoft.com).

Results and discussion

Mesh convergence study

The results of the mesh convergence analysis demonstrated that mesh density had a significant influence on the calculated Tresca stress values up to a certain threshold. Beyond this point, further refinement resulted in only marginal changes. Among the six mesh configurations tested, a model with 5,500 CAX4 elements (comprising 3500 elements in the acetabular cup and 2000 elements in the femoral head) was identified as optimal. This configuration exhibited less than 2% variation in maximum Tresca stress compared to the densest model (550,000 elements), indicating satisfactory numerical convergence (see Fig. 4). This mesh resolution provided a balance between computational efficiency and accuracy, ensuring that subsequent stress evaluations were not significantly influenced by discretization artifacts. Therefore, all further simulations involving radial clearance variations were conducted using this validated mesh configuration.

Fig. 4
figure 4

Mesh convergence of the Tresca stress from Al2O2-on-Al2O3 bearing.

Tresca stress investigation

This study examined Tresca stress distributions in Al2O2-on-Al2O3 hip bearings under physiological loading, with a specific focus on the influence of radial clearance throughout a complete gait cycle consisting of 32 phases. Tresca stress, based on maximum shear stress theory, offers a conservative measure of mechanical safety and is especially relevant for brittle ceramics such as Al2O2, which are more susceptible to failure under shear and tensile stresses than under compression.

As illustrated in Fig. 5a, Tresca stress varies across the gait cycle, with the 7th phase consistently corresponding to the peak stress for all configurations. This phase represents maximum joint loading during the mid-stance phase of normal walking, and the observed trend reinforces prior literature identifying this as the most mechanically demanding condition for hip implants. The stress values were further summarized in Fig. 5b, which reports the minimum, average, and maximum Tresca stress values for each radial clearance. A progressive increase in all three metrics was observed as clearance increased from 0.03 to 0.3 mm. The average Tresca stress rose from 45.42 MPa at 0.03 mm to 185.76 MPa at 0.3 mm, while the maximum stress spiked from 58.12 to 234.1 MPa, representing a fourfold increase. This trend can be attributed to reduced conformity between articulating surfaces at higher clearances, which concentrates contact loads into smaller areas, increasing localized shear stress101.

Fig. 5
figure 5

Tresca stress of Al2O3-on-Al2O3 bearings for different radial clearance: (a) maximum value under gait cycle and (b) lowest, average, and highest value.

Figure 6 displays Tresca stress contours at phases 1, 7, and 32, showing that peak loading significantly increases both the magnitude and extent of the stress field. With increasing radial clearance, these contours expand inward into the acetabular cup, indicating a deeper penetration of stress into the bulk material. Importantly, the model’s axisymmetric and centrally loaded configuration prevented edge loading, a known driver of catastrophic stress localization in ceramic components102.

Fig. 6
figure 6

Tresca stress distribution contour on Al2O3-on-Al2O3 bearings for different radial clearance.

To explore deeper into the internal stress behavior, Tresca stress was evaluated along a radial line across the acetabular cup thickness at phase 7 as shown in Fig. 7. This analysis reveals a striking pattern: the maximum Tresca stress does not occur at the articulating surface, but instead within the subsurface layers of the cup, typically at 20–40% of the wall thickness from the surface. This pattern becomes more pronounced with increasing radial clearance. At 0.03 mm clearance, the stress profile shows a relatively gentle gradient, peaking modestly below the surface and decaying toward the outer radius. However, as the clearance increases, the profiles become more nonlinear and peaked, with larger stress gradients and deeper stress concentrations. For example, at 0.3 mm clearance, the Tresca stress remains elevated well into the bulk material, with localized maxima that could serve as critical zones for crack nucleation, especially under cyclic loading. This behavior reflects the mechanical interplay between contact pressure distribution and structural constraint within the cup. While the articulating surface absorbs initial loading, internal constraint forces redistribute the load inward, leading to hoop stresses103 and shear interactions104 within the mid-thickness zone. These zones are particularly vulnerable in ceramics, which lack plastic deformation mechanisms to blunt internal stress peaks105.

Fig. 7
figure 7

Tresca stress profile as a function of Al2O3 acetabular cup thickness for different radial clearance: (a) Data retrieval line set and (b) Profile at peak loading.

Comparison with previous studies

To contextualize and validate the findings of this study, a comparative analysis was conducted against key previous investigations involving ceramic-on-ceramic hip bearing systems. The results from Ammarullah et al.76 are particularly relevant, as their finite element analysis investigated the influence of ceramic material types, starting from Al2O2, Si2N4, and ZrO2 on Tresca stress values under similar loading and geometrical conditions, using a fixed radial clearance of 0.05 mm. Their study reported a maximum Tresca stress of 78.29 MPa for Al2O2-on-Al2O3, 68.92 MPa for Si2N4-on-Si2N4, and 56.97 MPa for ZrO2-on-ZrO2. Ammarullah et al.76 findings indicate that while all ceramic materials remained structurally safe, which is under respective yield strengths (580 MPa for Al2O2106, 950–1200 MPa for Si2N4107, and 1000–1200 MPa for ZrO2108) under simulated gait loading, Al2O2 exhibited relatively higher internal stress, attributable to its lower toughness and higher elastic modulus compared to the others.

The present study extends this understanding by systematically varying radial clearance while keeping the material (Al2O2) constant. Notably, the maximum Tresca stress of 78.29 MPa was replicated at a 0.05 mm clearance, closely matching the value reported by Ammarullah et al.76. This consistency validates the numerical modeling approach and affirms the reliability of Tresca stress as a conservative safety metric. However, by further expanding the analysis across radial clearances ranging from 0.03 to 0.3 mm, the current study reveals a significant increase in Tresca stress with increasing clearance, culminating in a maximum value of 234.1 MPa at 0.3 mm, which is nearly three times higher than at 0.05 mm. Conversely, reducing the clearance to 0.03 mm yielded a substantial decrease in stress to 58.12 MPa, suggesting an optimal clearance threshold for minimizing internal shear and tensile stress in ceramic bearings.

Complementary insights are drawn from the work of Shankar109, who investigated the effect of radial clearance on contact pressure presented in Table 3. Their results similarly demonstrated that increasing radial clearance leads to a proportional rise in peak contact pressure from 72.53 MPa at 0.03 mm to 292.41 MPa at 0.3 mm. Although contact pressure and Tresca stress represent different mechanical metrics, the parallel trends reinforce the hypothesis that larger clearances exacerbate mechanical stresses at the articulating interface, reducing the conformity and distributing forces over smaller areas. Importantly, the correlation between Shankar’s peak contact pressure and the Tresca stress values obtained in this study explains a mechanistic linkage: higher contact pressures at the surface likely translate into more severe internal shear stresses.

Table 3 Comparison with contact pressure study on various radial clearance from Shankar109.

Engineering and clinical discussion

The finite element analysis revealed that across all examined radial clearances, the computed Tresca stress values remained well below the static yield strength of Al2O2, reported at 580 MPa106. This finding confirms that, under modeled physiological gait loading, the Al2O2-on-Al2O3 bearing configurations are mechanically safe in terms of static structural integrity. The lowest maximum Tresca stress of 58.12 MPa occurred at a radial clearance of 0.03 mm, while the highest, 234.1 MPa, was observed at a clearance of 0.3 mm, which is still within the allowable material limits. These margins are reassuring from a short-term safety perspective, yet they highlight an important design consideration there are minimizing radial clearance not only reduces the magnitude of shear stress but also widens the safety margin against potential failure.

From an engineering standpoint, these results emphasize the critical role of manufacturing precision and dimensional control. Even minor deviations in radial clearance, whether due to fabrication tolerances110, thermal expansion during sterilization111, or wear-in effects112 can significantly alter the internal stress distribution. Higher clearances lead to increased contact pressures113, reduced conformity114, and elevated Tresca stress76, especially within the subsurface bulk of the acetabular cup. These stresses, though below the material’s yield limit, could initiate fatigue-driven damage over prolonged use115. Therefore, maintaining sub-millimeter tolerances, particularly within the range of 0.03–0.05 mm, is vital for ensuring long-term mechanical stability and mitigating fracture risk. Engineering teams involved in the production of ceramic bearings must therefore prioritize tight tolerance control, surface finish accuracy, and post-processing verification, potentially utilizing advanced inspection methods such as 3D metrology116 and laser scanning117.

From a clinical perspective, the findings provide valuable insights into the role of radial clearance as a modifiable factor in implant longevity. Although no stress exceeded Al2O2’s yield limit, the progressive increase in Tresca stress with clearance and its localization within the bulk material suggest a higher susceptibility to sub-surface damage in patients implanted with bearings manufactured at or beyond the upper range of allowable clearances. Such stress concentrations may not lead to immediate failure118, but under cyclic loading and in vivo microseparation events, they could contribute to long-term degradation119 or spontaneous fracture120. These concerns are particularly relevant for younger, more active patients, who exert higher mechanical demands on their implants121. Thus, the results advocate for stringent quality assurance in component production, pre-implantation verification of dimensional accuracy, and where feasible, personalized prosthesis selection based on patient-specific biomechanics. Additionally, they underline the need for continued post-market surveillance and longitudinal clinical studies that correlate radial clearance specifications with real-world implant performance and revision rates.

Study limitations and future directions

Despite offering valuable insights into the mechanical behavior of Al2O2-on-Al2O3 bearings, several limitations inherent to this study must be acknowledged to ensure appropriate interpretation and to guide future improvements. First and foremost, the absence of experimental validation limits the direct clinical applicability of the finite element simulation results. While numerical analyses provide powerful approximations of physical phenomena, validation through in vitro testing as conducted by Kotta et al.122 or comparison with in vivo data preformed by Hung and Wu123 is essential to confirm the accuracy and reliability of the model predictions.

Secondly, the coefficient of friction between the Al2O2 femoral head and acetabular cup was modeled as a constant value. In reality, this coefficient can vary significantly over time due to evolving surface roughness124, wear117, fluid-film lubrication effects125, and third-body particle interactions126. A time-dependent work, like Rebenda et al.127 would improve the predictive fidelity of future simulations.

Third, the study employed a 2D axisymmetric ball-in-socket model, which, while computationally efficient, does not fully capture the complex 3D motion and multi-axial loading experienced in real human hip joints. Important biomechanical phenomena such as edge loading128, femoral anteversion129, pelvic tilt130, and non-symmetric gait forces131 are not addressed in the current framework. Incorporating 3D geometries and physiological loading conditions in future work would yield more anatomically and biomechanically representative insights.

Fourth, although Tresca stress was selected in this study to provide a conservative estimate of mechanical safety due to its sensitivity to maximum shear stress and smaller yield surface, it may not be the most suitable criterion for predicting brittle failure in ceramic materials. Al2O2 ceramics primarily fail under tensile loading rather than shear, making maximum principal stress a more appropriate predictor. As shown by Moga et al.132 and Fischer-Cripps133, tensile-based criteria better reflect crack initiation behavior in brittle materials, where tensile strength is considerably lower than compressive or shear strength. Additionally, the current model omits the femoral stem taper, which in practice induces significant tensile and hoop stresses in the femoral head, particularly under microseparation and dynamic loading. Nevelos et al.134 demonstrated that these stresses are critical in the initiation and propagation of ceramic fractures. Excluding this anatomical feature may lead to an underestimation of localized tensile stress and fracture risk. Future models should incorporate the stem taper and adopt maximum principal stress analysis to improve failure prediction accuracy and clinical relevance.

In addition, the simulation assumes idealized boundary conditions by excluding the mechanical constraints and interactions associated with the pelvic bone and implant fixation. This simplification may underestimate stress transfer dynamics at the bone–implant interface, which are crucial for assessing implant longevity and bone remodeling behavior. As noted by Ali135, such assumptions limit the accuracy of load transmission and can mask potential risks like stress shielding or micromotion. Furthermore, the material properties of Al2O2 were modeled as homogeneous, isotropic, and linearly elastic. However, ceramics exhibit microstructural variability and are susceptible to damage accumulation, particularly under cyclic loading or subcritical stress. According to Wan136, using linear-elastic models can underpredict crack initiation and progression, while nonlinear or damage-based models better capture real-world fracture behavior. Future studies should incorporate both realistic anatomical constraints and advanced constitutive models to enhance the biomechanical relevance and clinical applicability of finite element simulations.

Conclusions

This study investigated the influence of radial clearance on Tresca stress distribution in Al2O2-on-Al2O3 hip prosthesis bearings using finite element analysis under physiologically relevant gait cycle loading. The results demonstrate that radial clearance plays a critical role in determining the internal stress distribution of ceramic bearings, with smaller clearances (0.03–0.05 mm) yielding significantly lower Tresca stress values. All simulated configurations produced maximum Tresca stress well below the yield strength of Al2O2 (580 MPa), affirming their mechanical safety under static loading conditions. However, higher radial clearances substantially increased the peak Tresca stress, potentially amplifying the risk of subsurface crack initiation due to the ceramic’s susceptibility to tensile and shear stresses. These findings highlight the importance of tight manufacturing tolerances and precise quality control in the production of ceramic hip implants. From an engineering perspective, optimizing radial clearance is essential for mechanical efficiency and ensuring long-term durability and reducing the likelihood of fatigue-induced failure. Clinically, this research highlights the relevance of component design and fit in minimizing internal stresses that could compromise implant longevity.