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Materials Science in Additive Manufacturing                                  Thixotropic metal 3D printing
























            Figure 4. Plunger extrusion-based printing system design.
                                                               Figure 6. Flow front displacement for varied Oh number. The We number
            A                                 B                is fixed at 0.018.

                                                               A              B                C










            Figure 5. (A) Funnel-shaped printing nozzle. (B) Axisymmetric model
            for flow and extrusion.

            set method is used, where the interface is tracked by a level
            set function ϕ governed by

                   dφ  +   γ    ∇  φ  − )φ  ∇φ     (1  − ε∇   2 φ   
                    dt           ∇φ                (2)    Figure 7. Thixotropic fluid interface at (A) Oh = 0.0167, (B) Oh = 167,
                                                            and (C) Oh=833.
              where t is time, and γ and ε are parameters controlling   This can lead to a stable filament extrusion process at high
            numerical convergence. A similar method has previously   Oh number. In fact, the preliminary experimental work also
            been used by others to simulate inkjet printing and channel   showed that a thixotropic fluid with a high viscosity is highly
            flow of thixotropic fluids [16,17] .               controllable during printing and the extruded filaments can
              As an example, some simulation results about the effect of   be readily deposited on the printing platform.
            the Oh number on the flow front displacement are provided   The simulation results presented above are rather
            here. The Weber number (defined as We = ρu L /σ where u is   preliminary, and  yet  demonstrate  the  importance  of
                                               2
            velocity) is set constant at We = 0.018. As shown in Figure 6,   viscosity in affecting the extrusion and printing process.
            for a low Oh number (e.g., Oh = 0.167), the flow front is
            leveled off as time increases. This indicates that continuous   3.2. Simulation for material liquid fraction and
            extrusion is not possible at low Oh number or low viscosity.   temperature distribution
            On the contrary, at higher Oh number (corresponding   The purpose of simulation within the reservoir is to
            to high viscosity), the flow front continuously penetrate   determine the liquid fraction of material contained within
            forward. The simulation also shows that the flow front   the reservoir when the desired heating source is used. In this
            moves slower at a high Oh number, and the diameter of the   simulation, a simplified reservoir with an integrated 1 mm
            extruded filament becomes larger (Figure 7 for a snapshot).   diameter nozzle was adopted, and a Bi-Pb alloy was used as


            Volume 1 Issue 1 (2022)                         5                       http://doi.org/10.18063/msam.v1i1.5
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