Page 497 - IJB-10-5
P. 497

International Journal of Bioprinting                  3D bioprinting of full-thickness skin with a rete ridge structure




            may not always match that of the precursor cartridge due to   a controlled temperature of 4°C, consistent with the
            the complex flow path created by the precursor cartridge,   bioprinting temperature. Subsequently, the obtained shear
            syringe, and nozzle, as well  as the non-Newtonian   viscosity data of SdECM were fitted to the power-law fluid
            properties of the hydrogel. Therefore, achieving the desired   model (Equation I):
            cross-sectional shape required a trial-and-error process,
            which was time-consuming and unaffordable.                                  m −1
                                                                                 µ    ⋅ γ = K  ·           (I)
               In this study, we fabricated FTSEs with a rete ridge
            structure using a preset extrusion bioprinting technique. To
            achieve this without an ineffective trial-and-error process,   where K is the flow consistency index, γ˙ is the shear rate
            we used a computational fluid dynamics (CFD) method   and m is the flow behavior index. The shear viscosity data
            to design a precursor cartridge to print deep and narrow   of the alginate solution were fitted to the Carreau model
            fissure structures. The dermal layer was bioprinted within   (Equation II):
            the 3D-printed polycaprolactone (PCL) frame, which
            provides structural support until the bioink used in the                        n −1
                                                                                         ·
            dermal layer is fully gelled. This was followed by furrowing      µ  µ =  0 ⋅ +1[  ( λγ )]  2  (II)
                                                                                          2
            steps to establish a substrate for the stable anchoring of
            strands produced by the preset extrusion bioprinting
            process for creating a fissured structure. The epidermis   where μ  is the viscosity value at zero shear rate, λ is the
                                                                        0
            was formed by differentiating keratinocytes on the surface   characteristic time, and n is the power index.
            of the dermis with fissure structures. We conducted   2.2. Computational simulation for the design of a
            histological and immunostaining analyses, followed by UV   precursor cartridge
            treatment, which confirmed differences between the rete   To design a precursor cartridge for generating narrow
            ridge and conventional FTSEs using dermal-epidermal   fissures within extruded strands, CFD simulation was
            junction (DEJ), epidermal, and proliferation markers.   conducted. 3D computer-aided design (CAD) models
            These differences yield test results akin to those in vivo,   of bioinks in the bioprinting process were created with
            suggesting that preset extrusion 3D bioprinting techniques   dimensions matching those of the precursor cartridge,
            can serve as a useful tool for fabricating structures that   syringe, and nozzle using SolidWorks 2022 (Dassault
            mimic in vivo environments.                        System, France). The 3D CAD model was then imported
                                                               to COMSOL Multiphysics 5.6 (COMSOL Inc., Sweden).
            2. Materials and methods
                                                                  Initially, the physics module for the laminar flow of
            2.1. Preparation and characterization of hydrogels  single-phase fluids was used to simulate the flow of bioinks
            Porcine skin-derived decellularized ECM (SdECM) was   during the bioprinting process. The viscosity of bioinks was
            prepared as described in a previous study.  Briefly, dermal   based on rheological data. The inlet pressure was applied
                                             24
            tissue was cut and immersed in phosphate-buffered   at the top of the precursor cartridge, corresponding to the
            saline (PBS;  Welgene, Korea),  containing  0.5%  trypsin   actual bioprinting pressure, while the pressure at the end
            (Welgene, Korea) and 0.2% ethylene diamine tetra acetic   of the nozzle was set to zero relative pressure as an outlet.
            acid (EDTA; Welgene, Korea), for 24 h. Subsequently,   The other boundaries were considered as walls with a no-
            the treated dermal tissues were washed, followed by the   slip condition. Subsequently, the model was discretized to
            addition of  PBS containing 1%  Triton X-100 (Samchun   the tetrahedral solid mesh by an automatic mesh generator
            Pure Chemical Co., Ltd., Korea) for 24 h. Decellularized   and then solved with the Navier-Stokes equation using a
            tissues were washed several times with distilled water and   stationary solver.
            lyophilized. SdECM was solubilized through digestion with
            0.5 M acetic acid (Sigma-Aldrich, United States of America   To visualize the cross-sectional pattern at the outlet
            [USA]) containing pepsin (1 mg/10 mg lyophilized   of the printing nozzle, particle tracing for the fluid flow
            SdECM). The SdECM was dissolved in 0.5 M acetic acid   interface was used in the solved result for the velocity field
            and neutralized to a concentration of 3.25% (w/v) for use   of laminar flow simulation.  The massless solid particles
                                                                                     25
            in 3D bioprinting. Alginate (A2033; Sigma-Aldrich, USA)   were released on the domain of alginate hydrogel, and
            was dissolved in PBS at a concentration of 2.75% (w/v).   all boundaries were set to the wall and conditioned as
            As the hydrogels used in this study were non-Newtonian   “Freeze.” Subsequently, the simulation was performed
            fluids, their shear viscosity profiles were obtained using a   with a time-dependent solver. Finally, the cross-section of
            rheometer (Kinexus pro+; NETZSCH GmbH, Germany)    the end of the nozzle was visualized by implementing the
            with cone-plate geometry and a 1 mm gap, maintaining   Poincaré map.


            Volume 10 Issue 5 (2024)                       489                                doi: 10.36922/ijb.3961
   492   493   494   495   496   497   498   499   500   501   502