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International Journal of Bioprinting                                 Swelling–shrinking behavior of hydrogel




                                uL                               where c is the concentration of water vapor; D' denotes
                           R                         (III)   the diffusion coefficient; and J is the diffusive flux vector,
                            e
                                                               which measures the amount of substance that flows
                                                               through a unit area during a unit time interval.
               where ρ is the density of moist air;u is the flow speed;
            μ is the dynamic viscosity of the fluid; and  L is the   According to the mass conservation equation
            characteristic length, which can be estimated according to   (Equation V), directly using RH as an input parameter
            the proposed FEM model:                            in the calculation is impractical. Hence, to analyze
                                                               geometric variations under a variety of RH conditions,
                                                               the relationship between the vapor concentration and RH
                          L   D  D 2                 (IV)    must be clarified :
                                                                            38
                               1
                                2
                                                                                   c
               where  D  and  D  are the diameters of the printed             RH =  v                    (VII)
                      1
                             2
            filament and the ambient air domain, respectively. Given               c sat
            the  low speed  of the  moist  airflow,  the  value  of  R e  was
            estimated to be lower than 2300. It implies that the flow   where the c v and c sat are the concentration and saturation
            condition of the ambient air should be defined as laminar   concentration of water vapor, respectively. When defining
            flow in the FEM model. Furthermore, as the density of   RH in the FEM model, a conversion from RH to c v must
            fluid exhibits little fluctuation with pressure in the model,   be implemented in advance. By inputting the calculated c v
            the laminar flow in the ambient air domain was regarded   and corresponding c sat into the simulation, the geometric
            as incompressible.                                 variation of printed filaments under various ambient RH
                                                               conditions can be calculated. In the model, the  c v was
            2.2.3. Cold source of the plate                    set to the same value for both the ambient air and the
            According to the configuration presented in  Figure 1,   outlet boundary.
            hydrogel filaments are deposited onto a temperature-  2.3. Preparation of hydrogel filaments
            controlled plate during the 3D printing of hydrogel   for experimental validation
            architectures. Hence, the top surface of the plate,   To validate the reliability of the calculation results,
            represented as a cold source in Figure 2, was defined as a   printing trials were conducted using hydrogel filaments.
            temperature boundary. Specifically, the initial temperatures   F-127, selected for these trials, is a well-acclaimed
            of the plate, the ambient air, and the printed filament were   medical hydrogel material in regenerative medicine due
            all set to room temperature in the FEM model.      to its excellent biodegradation properties and outstanding
            2.2.4. Water vapor transport at the                biocompatibility.
            fluid–fluid interface                                 In this study, a 30% (w/v) F-127 solution was prepared
            When hydrogel filaments are exposed to ambient air with   for the 3D printing experiments. Specifically, the mixture
            inappropriate RH levels, moisture exchange between the   of 1.5 g F-127 powder (P2443-1KG, Sigma-Aldrich, USA)
            hydrogel filaments and the surrounding environment often   and 5 mL phosphate-buffered saline (Thermo Fisher
            results in swelling or shrinking of the filaments. To account   Scientific Inc., USA) was prepared and stored at 4°C for 24
            for water vapor transport across the fluid–fluid interface,   h. Before each 3D printing, the prepared 30% (w/v) F-127
            the transport of diluted species model was utilized in the   solution was transferred into syringes and centrifuged for
            FEM simulation. To achieve the calculation of the diffusion   10 min at 4°C to remove air bubbles within the hydrogel
            and the convection process of water vapor, a widely   material. Hydrogel filaments with diameters of 0.2, 0.3,
            adopted mass conservation equation, which is associated   and 0.4 mm were then extruded using a self-designed
            with Fick’s laws of diffusion,  was employed:      high-precision 3D printing device. A humidity-controlled
                                  37
                                                               enclosure was used to maintain a constant ambient RH for
                                                               hydrogel filaments during and after the deposition process.
                          c                                   To evaluate the geometric variation of the printed filaments
                                Ju
                                      c
                               0                (V)
                          t                                   under the RH of 50, 60, 70, 80, and 90%, an electronic
                                                               digital  microscope  (Inskam-316,  Aomekie,  China)  was
                                                               employed to capture micrographs of the filament cross-
                           J  D  c                 (VI)    sections. Representative geometric variations of hydrogel

            Volume 11 Issue 4 (2025)                       414                            doi: 10.36922/IJB025220222
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