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LIFT hydrogel printing: A defined route for highly controlled process
           2.5 Visualization of jetting and measurement of     subsequent  transfer  to  an  acceptor  plate .  The
                                                                                                       [15]
           jetting velocity                                    processes  associated  with  the  formation  and
                                                               collapse of a gas bubble, as well as possible regimes
           The printing and transfer processes of the material   of jet formation are represented in Figure 4.
           were  visualized  and  investigated  using  a  high-  At the first stage of the LIFT process (t = 0.01
           speed  Fastcam  SA-3  camera  (Photron,  Japan)     a.u.), the metal energy absorbing layer, the nearest
           (shutter  1/60000,  FPS  10000-60000)  with  a
           long-focus microscopic lens providing a shooting    thin  layers  of  the  glass  slide,  and  the  hydrogel
           field of up to 5 × 3.5 mm. The illumination was     are heated to high temperatures due to the partial
           performed  using  a  K150  Laboratory  Illuminator   absorption of the laser pulse energy by the energy
           (Optics Co, China).                                 absorbing  layer.  In  the  applied  laser  printing
                                                               regimes,  the  achieved  temperature  significantly
           3 Results and discussion                            exceeds  the  melting  temperature  of  the  material
                                                               of the absorbing layer (for Au T≈1337 K) . On
                                                                                                        [13]
           3.1 General observations                            reaching a temperature of ~ 0.95 from the critical
           The  LIFT  process  is  based  on  local  heating   temperature  (for  water  T =  647  K),  the  water
                                                                                        c
                                                                                                     [34]
           occurring during the interaction of a laser pulse   contained  in  the  gel  boils  explosively ,  which
           with an absorbing layer, which leads to explosive   converts the water into steam compressed to a high
           boiling of water in a gel , while more intensive    (around critical) pressure (Pc ~ 22.5 MPa). As a
                                  [13]
           heating  can  lead  to  explosive  boiling  of  the   result, a rapidly expanding vapor bubble forms in
           absorbing  layer  material . As  a  result,  a  high-  the gel in the area of laser exposure.
                                   [45]
           pressure bubble is formed [46-48] , the expansion of   At t = 1, the size of this bubble already exceeds
           which leads, depending on the initial parameters ,   the  thickness  of  the  gel.  Due  to  the  hydrogel
                                                        [15]
           to  the  formation  of  various  types  of  jets ,  and   viscosity,  the  presence  of  a  solid  surface  of  the
                                                   [49]
           the separation of one or more droplets and their    donor plate and the limited thickness of the gel, this


                        A















                        B














           Figure 4. (A) The main stages of the jet and droplet formation during laser printing. Red arrows indicate
           the direction of fluid movement (B) changes in jetting regimes with the increase of laser energy.

           82                          International Journal of Bioprinting (2020)–Volume 6, Issue 3
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