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Rheological study on 3D printability of alginate hydrogel and effect of graphene oxide

            materials were used without further purification.   on the fluid mechanics [27] , the viscosity is a function
               Aqueous solutions of alginate with various concen-  of shear rate. At a constant volume flow rate, the linear
            trations (2, 4, 6, 8 and 10 wt.%) were prepared using   flow rate in a pipe will change when the cross section
            deionized water from a Millipore water purifier. Then,   area of the pipe is changed. Therefore, the linear flow
            calcium  chloride  solutions with various molar  frac-  rate will change due to the change in the cross section
            tions were added to each solution of alginate to obtain   area from the syringe to the nozzle, which also results
            alginate hydrogels with various CaCl 2  contents. In   in a change in the shear rate. Shear rate is an important
            order to study the effect of GO on alginate hydrogels,   factor for an extrusion based printer. In this study, the
            alginate composite hydrogels filled with  various GO   range of shear rates in the syringe is estimated from a
            contents were prepared as follows. First, the suspen-  given piston moving speed of the 3D printer.
            sions with various GO contents were produced by ul-  Consider a laminar and steady flow of a time-ind-
            trasonic treatment using deionized water. After that, 5   ependent and incompressible fluid in a circular pipe of
            g of alginate powder (for a final concentration of 10   radius, R, as shown in Schematic 1A. Since there is no
            wt.% based on the total weight of DI water) was add-  angular velocity, the force balance in the z direction on
            ed into the suspension of GO under magnetic stirring.   a fluid element situated at a radius r (0 < r < R) can be
            Finally, alginate composite hydrogels were prepared   written as
                                                                                          2
            by adding a certain amount of calcium chloride solu-          ( p π r 2 )(p−  +∆  ) p π r =  2τπ rL    (1)
            tion into the solution of GO/alginate under magnetic                    −∆ P
            stirring.  The alginate concentration in the  composite              τ =     r                (2)
            hydrogels was fixed 10 wt.% and a CaCl 2 content of                      2L
            25 mM/L was also kept constant, while GO was loa-  where  p  is  the  pressure,  τ  is the shear  stress on  the
                                                               surface of the cylindrical element and L is the length
            ded to 0.05, 0.15 and 0.25 wt.% based on total deion-
            ized (DI) water. The  prepared samples were labeled   of the element.  Equation (2)  shows the  shear stress
            with GO a/Alg b, where a and b are the weight fraction   distribution across the cross-section of pipe, whereas
                                                               the shear stress being zero at the axis  of the pipe
            of GO and alginate, respectively.
                                                               (Schematic 1B). Note that Equation (2) is applicable
            2.2 Shear Rate in an Extrusion-based 3D Printing   to both turbulent and laminar flows of any fluid since
            Process                                            it is based on a simple force balance and also no as-
                                                               sumption has been made [27] .
            During an extrusion-based  3D  printing process,  mo-  For  a power-law fluid in a pipe,  shear stress is  a
            lecular crosslinks of hydrogels may have broken down   function of shear rate as follows [28] :
            by shear forces, reducing viscosity, and allowing highly                     n
                                                                                      ()γ =
            viscous hydrogels to be extruded out from the printing               τ  m                    (3)
            nozzle. A printable hydrogel needs to be optimized to   where  n  and m  are  the power-law index and power-
            have low viscosity during printing but sufficient me-  law consistency coefficient, respectively, whereas  γ 
            chanical strength after  printed. So,  it is ideal for a   is the shear rate. The viscosity for the power-law fluid
            printed hydrogel to  have a thixotropic  property and   can be described by
            then a recovery ability, which means that viscosity of              η = m ( ) γ   n− 1       (4)
            the hydrogel is low when a shear force is applied but
            the viscosity recovers quickly after the shear force is   So, the shear rate can be written as
            removed. A material is said to be thixotropic when its                du   −∆ P
                                                                               
            apparent viscosity decreases  with time  under a con-              γ =  dr  =  2 L  r         (5)
                                                                                        η
            stant shear rate. As for thixotropic materials, the best-
            known example is the thixotropic paints and the other   where  u is the flow velocity at r. Integrating the equ-
            examples include concentrated suspensions, drilling   ation, we can get the velocity in the pipe
            fluids, emulsions, protein solutions, laponite, and silk
            nanofibril-based hydrogel [23–26] .
               The 3D printing head consists of a piston, a syringe,
            and a nozzle. The syringe and nozzle possess different
            inner diameter. Before printing, the hydrogels are lo-

            aded into the syringe firstly, and then it is extruded to   Schematic 1. (A) Flow through a pipe, and (B) Stress and ve-
            the nozzle under the pushing action of a piston. Based   locity distribution of non-Newtonian flow in a pipe.

            56                          International Journal of Bioprinting (2016)–Volume 2, Issue 2
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