Page 438 - IJB-10-3
P. 438

International Journal of Bioprinting                                  Different modeling of porous scaffolds




            Quantum GX II), which allowed for the documentation of   law, given in Equation II. 32-34  To facilitate the calculation,
            the external structure and the calculation of porosity. The   the ratio of height H  to H was set to be equal to e. The
                                                                                1
                                                                                     2
            CT scan parameters were set to 90 kV for voltage, 80 μA   time difference t (t = t - t ) was recorded for the fall of the
                                                                                1
                                                                                   0
            for current, and 14 min for scanning duration. The top   horizontal plane.
            of the porous scaffolds was imaged using a JEM-2100F                      lg H − lg H
            scanning electron microscope, and DM software was used          k =  µ hA  ×  1   2            (II)
            to analyze structural features, including pore size and             ρ gta    lg e
            strut dimensions.
                                                                  The parameters used in the formula are selected and
            2.3. Mechanical performance testing                shown in Table 2.
            According to the mechanical testing standard, ISO
            13314, for porous and cellular metallic materials, 29-31    Using the computational fluid dynamics software
            compression and tensile tests were conducted at room   ANSYS 16.0 Workbench with the Fluent module, a fluid
            temperature using an electronic universal testing   simulation analysis was conducted on individual scaffold
            machine (Suns, Shenzhen, China). At least three samples   units, as illustrated in Figure 3B. The entrance flow velocity
            were compressed for each structural sample. The    was set to 0.01 m/s to investigate the structural  factors
            compression strain rate was set at 0.5 mm/min until the   affecting permeability, with an outlet pressure of 0 Pa.
            samples became fully dense or fractured. The fracture   The wall was assumed to be non-slip, and the minimum
            morphology of the scaffolds was recorded using a   unit size was set to 0.01 mm to analyze the effect of the
            camera. Stress–strain curves were plotted; yield strength,   modeling strategy on the permeability from a microscopic
            ultimate strength, elastic modulus, and other mechanical   point of view.
            properties were calculated; and the data were expressed
            as mean ± standard deviation (SD).                 3. Results and discussion
            2.4. Permeability performance testing and          3.1. Macro- and microscopic characteristics
            simulation of scaffolds                            of scaffolds
            The permeability performance of the scaffolds was tested   Figure 4A and  B depicts the external morphology of
            using the falling head method, as illustrated in Figure 3A.   the scaffolds under optical microscopy and the CT-
            The scaffold permeability (k) was calculated using Darcy’s   reconstructed morphology for comparison. From the

































            Figure 3. (A) Schematic of permeability experiment. (B) Finite element boundary conditions for permeability. Abbreviations: d, diameter of the sample;
            D, diameter of the water pipe; H1, height of the liquid level before the test; H2, height at which the test stops, where H2/H1 = e; L, length of the sample in
            the direction of the water flow.


            Volume 10 Issue 3 (2024)                       430                                doi: 10.36922/ijb.2565
   433   434   435   436   437   438   439   440   441   442   443