Finite element analysis of the tibial bone graft in cementless total knee arthroplasty
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Achieving stability of the tibial implant is essential following cementless total knee arthroplasty with bone grafting. We investigated the effects of bone grafting on the relative micromotion of the tibial implant and stress between the tibial implant and adjacent bone in the immediate postoperative period.
Tibial implant models were developed using a nonlinear, three-dimensional, finite element method. On the basis of a preprepared template, several bone graft models of varying sizes and material properties were prepared.
Micromotion was larger in the bone graft models than in the intact model. Maximum micromotion and excessive stress in the area adjacent to the bone graft were observed for the soft and large graft models. With hard bone grafting, increased load transfer and decreased micromotion were observed.
Avoidance of large soft bone grafts and use of hard bone grafting effectively reduced micromotion and undue stress in the adjacent area.
KeywordsTotal knee arthroplasty Bone graft Finite element analysis
Large bone graft with hard bone
Large bone graft with soft bone
Medium bone graft with hard bone
Medium bone graft with soft bone
Small bone graft with hard bone
Small bone graft with soft bone
Total knee arthroplasty
Ultra-high molecular weight polyethylene
Tibial bone defects in total knee arthroplasty (TKA) often are managed with various types of bone grafts, such as solid bone, morselized bone, and combined grafts [1, 2, 3, 4]. For optimal results, patients with bone grafts require long-term postoperative therapy. In particular, during weight-bearing gait training, the mechanical condition of the grafted bone and micromotion-preventing fixation of the tibial component influence the degree of micromotion . Whether the patient is able to walk safely immediately postoperatively is an important concern after cementless TKA. The finite element method is being used increasingly for biomechanical analysis of tibial component micromotion. Several studies have analyzed the relative micromotion of implanted prostheses using this method [5, 6, 7, 8]. We have previously reported that tibial bone graft combined with cortical bone can be expected to reduce micromotion and stress . However, the simulation was not enough to include the characteristics of implant and bone graft materials in the models or to examine the detailed status of contact and stress distribution while considering micromotion. To our knowledge, no analysis has been conducted considering the actual bone graft size and material properties. We used the finite element method to develop a new precise model of the proximal tibia and tibial implant and meticulously analyzed the biomechanical effects of various types of bone grafts on relative micromotion and stress distribution at the tibial tray–bone interface in the immediate postoperative period.
Intact (I) model
An appropriate modular tibial baseplate made of cobalt–chrome alloy (#3 size, Osteonics 7000 tibial component; Howmedia Osteonics Corp., Mahwah, NJ, USA), applied in accordance with the manufacturer’s guidelines, was considered in this study (Fig. 1c). The geometry of the modular tibial component was obtained by direct measurement. The tibial insert was composed of 8-mm-thick ultra-high molecular weight polyethylene (UHMWPE). The rounded top surface of the UHMWPE was ignored, and a flat surface was defined (Fig. 1b). The inferior surface of the UHMWPE was attached to the tibial baseplate, which was positioned at the geometric center of the tibia, tilted 3° posteriorly (Fig. 1d).
Bone graft models
For the tibia, Young’s modulus of cortical and cancellous bone was set at 17,000 and 400 MPa, with Poisson’s ratio of 0.30 [10, 11]. Young’s modulus of morselized bone graft for bone graft models has been reported as 42–150 MPa [12, 13, 14]. In the present bone graft models, simulating the treatment of bone defects with morselized bone graft, Young’s modulus for the bone graft site was set at 42 or 150 MPa with Poisson’s ratio of 0.2, the respective low- and high-strength bone graft values according to the literature.
The cobalt–chrome alloy used for the tibial baseplate component and the UHMWPE used for the tibial insert were given Young’s modulus (Poisson’s ratio) of 248,000 MPa (0.30) and 667 MPa (0.46), respectively . The interface between the bone and tibial component was treated as a frictional contact problem, with friction set at 0.2 according to the literature .
Boundary and loading conditions
The inferior surface of the distal tibia was fixed in all directions. The maximum loads used in the analyses were the maximum physiological loads used in previously described experiments [16, 17]. A compressive force of approximately three times the body weight, or 1800 N, was used in this study. Regarding the site of loading, the posteromedial portion was used, as in the previously described experiments [5, 18], to simulate a varus alignment. For nonlinear analyses, incremental force control was used in the numerical procedure. Each model was loaded, and the resultant displacement, maximum liftoff, subsidence, and von Mises stress distribution were analyzed and compared.
For the medial load application shown in Fig. 1d, the stability of the implant and stress distribution are important from the biomechanical viewpoint. Relative micromotion between the tibial tray (Fig. 1c) and tibial bone (Fig. 1a) model at the location of maximum liftoff and at the distal tip of the stem and stress distribution in the tibial bone for the intact and various types of bone graft models shown in Fig. 2 were calculated.
Displacement and micromotion
The maximum liftoff was smaller in the hard than in the soft bone graft models. Comparing the L–S and L–H, M–S and M–H, and S–S and S–H models revealed that the maximum liftoff of the tibial tray was lower in the hard bone graft models by approximately 39, 26, and 12%, respectively, indicating a decrease in the micromotion of hard bone. In the M–H and S–H models, the magnitudes of liftoff were almost identical and smaller than those in the I model.
Relative micromotion beneath the stem
Compared with the soft bone graft models, the magnitudes of micromotion beneath the stem in the hard bone graft models were significantly lower. The L–H and M–H models showed a larger and the S–H model a slightly larger magnitude of micromotion than the I model, demonstrating that hard bone grafts have increased stability.
In the soft bone graft models, a stress increase was evident in anteromedial and posteromedial cortical bone and in the medial host cancellous bone region, including in the keel of the tibial baseplate adjacent to the bone graft, relative to the I model (Fig. 6b–d). In particular, the L–S model exhibited high stress in host cancellous bone. In the hard bone graft models, a stress increase was found in the bone graft area, whereas stresses adjacent to the bone graft area were reduced (Fig. 6e–g).
Medial loading resulted in subsidence of the loaded medial tibial plate and liftoff at the periphery on the opposite, unloaded side. The tilting motion of the tibial components observed in this study implies instability of the initial fixation, which could possibly compromise bony ingrowth. The success of cementless implants depends on the ingrowth of bone into the porous coating, which is inhibited by relative micromotion at the implant–bone interface during patient activity [19, 20]. Excess implant micromotion prevents bone formation within porous-surfaced implants. According to Jasty et al. , 150 μm of motion results in unstable ingrowth of bone into porous-surfaced implants. Although the 150-μm limit often is quoted in the literature, a range of ± 50 μm was used to assess the sensitivity of the micromotion limit . Our findings showed that soft bone grafting leads to considerable implant micromotion. The relative micromotion observed in the L–S model exceeded 100 μm. This degree of micromotion, if occurring in a clinical situation, may inhibit bony ingrowth and lead to implant loosening. Conversely, use of hard bone decreases micromotion. In all hard bone graft models, the relative micromotion was less than 100 μm. These results suggested that hard bone grafting is necessary in patients requiring a large bone graft.
Loads were transferred via contact between the tibial baseplate and tibial bone. This contact resulted in an increase in the loading of the medial plateau of the tibia. Analysis of the soft bone graft models revealed considerable unloading of the bone graft area concentrated around the bone graft compared with the I model. Tibial host cancellous bone stresses were reduced by hard bone grafting. The L–S model caused high stress in host cancellous bone. High stress levels, particularly acting on weak cancellous bone, have been implicated as the predominant cause of tibial component loosening [23, 24], and the abnormal stress pattern may cause stress shielding in long-term follow-up [25, 26]. The stress pattern produced by load sharing between the implant and bone suggests that large soft bone grafting should be avoided in favor of grafting with hard bone to eliminate excessive stress in host cancellous bone.
In the previous report, the maximum liftoff and relative micromotion were approximately 2–10 times higher than those in this study and suggested that bone grafting causes excessive instability . However, from a modeling viewpoint, the shape of the keel of the tibial baseplate was simple, and the roughness of the keel surface to improve fixation was ignored, treating the interface between the bone and implant as a frictionless contact in the previous report. Furthermore, the graft size and material properties were impractical. However, in this study, the shape of the keel designs was precise, treating the interface between the implant and bone as a frictional contact to provide additional stability, in addition to considering realistic graft size and material properties. We believe that these distinct differences are the main reasons that affected the results.
With regard to the elastic modulus of bone graft materials, several studies have demonstrated that material stiffness and strength vary substantially according to age, diagnosis, and composition of cancellous and corticocancellous bone and that improved fixation can be achieved by impaction during bone grafting [13, 14, 27, 28, 29]. In this study, hard bone models showed lower relative micromotion than soft bone grafting models, suggesting that increased stiffness of the bone graft material by impaction led to decreased micromotion and improved the initial fixation of the tibial baseplate. In clinical cases where the quality of host bone varies substantially between patients, the appropriate bone, including impacted bone, should be grafted into bone defects to achieve optimal stability and a good clinical outcome [4, 30, 31].
With respect to eccentric loading, the finite element analysis of bone grafts undertaken in this study represented the worst-case scenario. Our results suggested that grafting defects with hard bone is more likely to yield better fixation especially for larger, posteromedial defects. During surgery, mechanically effective fixation can be achieved by impaction according to the bone graft material used and type of tibial defects. However, this study did not consider changes in mechanical conditions because of bone remodeling, ingrowth, or stress relaxation. Thus, the qualitative trends outlined here offer an approximation of what occurs during the immediate postoperative phase. This study was designed to provide a foundation for a biomechanical rationale that will support selection of treatment. Because the severity of tibial bone defects and range of bone grafts vary in the clinical setting, care should be taken when interpreting these results. Considering these limitations, combining our results with those of previous cadaveric studies may enhance the clinical use of this technique.
The purpose of this study was to investigate the effects of bone grafting on the relative micromotion of the tibial implant and stress between the tibial implant and adjacent bone. Maximum micromotion and excessive stress in the host bone area adjacent to the bone graft were observed for the soft and large graft models. On the basis of these biomechanical findings, avoidance of large soft bone grafts and use of hard bone grafting will produce better clinical outcomes.
We would like to thank Enago (www.enago.jp) for the English language review.
This work was supported in part by a grant from the Ministry of Education, Culture, Sports, Science and Technology of Japan.
Availability of data and materials
Please contact the author for data requests.
KT, EC, and HH contributed to the conception and design and data analysis and interpretation. GY, KO, SY, and GD designed the computer model and performed the finite element analysis. All authors helped to draft the manuscript. All authors read and approved the final manuscript.
Ethics approval and consent to participate
This study was approved by the Ethics Committee of the University of Miyazaki.
Informed consent to participate in the study was obtained from the participant.
The authors declare that they have no competing interests.
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
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