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International Journal of Bioprinting                               Mechanically biomimicking 3D bone model











































            Figure 2. (A) Three-dimensional printing of infill-varied rectangular cuboid structure. (B) Compressive load–displacement curve of an infill-varied
            structure. (C) Cross-sectional images of compressed samples at different load states.


            several load states (Figure 2B and C). Initially, in the linear   the surficial hard part was initially compressed, followed by
            region of load–displacement curve, the soft part did not   the deformation of the central soft part. The transition of
            deform, but the hard part was compressed by the implant   deformation was observed at 50% load, where the gradient
            indentation. After reaching 50% of the maximum failure   of the load–displacement curve changed. This implies that
            load, the soft part apparently began to collapse, and the   the stiffness for initial deformation is associated with the
            outer  wall  of  the  sample  buckled  when  the  gradient  of   infill design of surficial region, whereas the failure load
            load–displacement  curve  approached  zero  (Figure  2B).   for final deformation is affected by the infill design of the
            To observe the internal deformation behavior, we selected   central region.
            load states of 25%, 50%, 75%, and 100% and observed the   To analyze these results, we used the finite element
            corresponding cross-sectional images (Figure 2C). At 25%   method  (ANSYS  2022.  R2)  to  simulate  the  strain
            load, there was no significant deformation, but the local   distribution and compared the infill-varied structure with
            surface compressed by the implant was slightly distorted,   the infill-uniform structure. In the simulation, the two
            causing mostly the hard part only to deform. At 50%   structures were locally compressed by the spinal implant
            load, the hard part surface in contact with the implant   (Figure 3A-i), which was then compared with the entire-
            was still dominantly deformed, initiating the distortion of   surface compression (Figure 3B-i). The compression in the
            the soft part. The 75% load condition produced apparent   finite element analysis (FEA) was simulated by applying
            deformation of the soft part, and the 100% load fully   a downward force of up to 1 mm from the top surface
            collapsed the overall structure. The overall compressive   of implant while fixing the bottom surface. We used a
            behavior showed sequential deformation from the surficial   tetrahedral mesh type with a size of 1 mm for efficient and
            to the central regions, which agreed with a previous study   accurate representation of the model geometry. The FEA
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            on indentation of porous structure.  Even though the infill-  employed a linear elastic and isotropic material model. The
            varied structure contained the hard part at the surficial   material parameters such as Young’s modulus and Poisson’s
            region, a similar deformation behavior was observed where


            Volume 10 Issue 1 (2024)                       421                          https://doi.org/10.36922/ijb.1067
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