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International Journal of Bioprinting                Simulation-based comparative analysis of nozzles for bioprinting
























































             Figure 2. Cross-section blueprint (A) and computational model geometry (B) of the 22G conical tip (left) and E3D V6.4 3D printing nozzle (right).

               Each simulation considered two domains: the first one   Regarding the simulations, four different simulations
            referred to the hydrogel inside of the Cone or Nozzle, and   were performed. A 10 s simulation with a 1 ms step was done
            the second one referred to air. In Figure 2, the geometrical   for each geometrical model and inlet configuration. The
            models of the simulations (B) with the boundaries   simulation study was composed by a phase initialization
            considered and the domains (blue for hydrogel and gray   and time-dependent steps.
            for air) are represented. Model inlets were configured to   A laminar flow based on a low Reynolds number
            two approaches: a pneumatic process with 15 kPa inlet   (Re ≅ 0.4) was assumed in the simulations, according to
            pressure, as recommended by Cellink , and a piston-  a  previous  study ,  where  simulations  formed  a  falling
                                            [54]
                                                                             [50]
            driven process with 10 mm /s volumetric inlet flow.
                                 3
                                                               drop with a later accumulation of material until it reached
               In this work, Cellink bioink (Cellink USA) was   the tip.
            simulated at 37°C with the following fitted potential law:
                                                               2.2. Experimental test
               μ = 87.906(γ˙)  -0.792                   (I)
                                                               Pneumatic  simulations  were  validated  through
            where μ is the dynamic viscosity (Pa·s) and γ˙ is the shear   experimental tests to assure that they were accurate within
            rate (s ).                                         acceptable error ranges, despite the assumed simplifications.
                 −1
            Volume 9 Issue 4 (2023)                        212                         https://doi.org/10.18063/ijb.730
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