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Sun J, et al.
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           Figure 3. Effect of the applied voltage on centroid and diameter under varied distance (65 wt/v% polycaprolactone, feed rate = 0.7 μl/min,
           stage speed = 150 mm/s). (A) Effect of voltage and distance on centroid. (B) Effect of voltage and distance on diameter

           cone is inversely proportional to the applied voltage. It is   we can manipulate the solidified electrospun fiber flying
           found that a voltage around 2.6 kV can generate a huge   in a stabilized helical manner. Thus, versatile serpentine
           size of Taylor cone, and this size reduces with the increase   structures  can  be  direct  written  on  a  moving  substrate
           of  the  voltage.  The  cone  shape  becomes  excessively   with diverse amplitude and cycles.
           tiny when the voltage is around 3.4 kV. In other words,
           increasing  the  applied  voltage  above  a  threshold  will   3.3.2 Effect of the SS
           reduce the stability of the jet . Similar phenomena are   We conduct several tests to examine the effect of the SS
                                   [10]
           also observed for the nozzle-substrate distance at 3.5 mm   (100–300 mm/s) on Taylor cone and jet. The mechanical
           and  4 mm.  Similarly,  we  also  investigate  the  size  and   drawing  force  acting  on  the  jetting  increases  with  the
           shape of Taylor cones using 70 wt/v% PCL and draw the   SS. This leads to an increasing degree of slant jet and
           same conclusion.                                    its elongation  rate and eventually  generates diverse
           About the effect of the applied voltage on the cone-jet   trajectory.  When  the  SS  is  greater  than  the  downward
           diameter  in  Figure 3B, increasing  the applied  voltage   speed of the jet, the fiber length deposited on the substrate
           leads  to  slightly  decrease of  the  jet  diameter when  the   is larger than the jet length fallen on substrate per unit
           nozzle-substrate  distance  is  3 mm.  The  jet  diameter   time .
                                                                  [13]
           decreases  more  significantly  when  the  nozzle-substrate   As shown in Figure 5, the EHDP jet falls down almost
           distance increases to 3.5 and 4 mm. As the electrostatic   vertically and buckles in some degree near the substrate
           force  becomes  weaker  under  a  larger  distance,  EHDP   at the SS range of 50–150 mm/s. The jet evolves into a
           process  generates  a  thicker  jet  which  can  be  further   compressed “heel” shape (Figure 5A and B) and becomes
           stretched with the increase of the applied voltage .  unstable with periodically meandering. Thus, a lower SS
                                                    [10]
           The captured cone images at 3 kV under different nozzle-  may lead to a series of bifurcations, such as alternating
           substrate distances and their  corresponding deposited   loops, and translated coiling on the substrates as shown in
           fiber patterns are shown in Figure 3B. Compared with the   Figure 2. This jet buckling effect is less obvious when the
           Taylor cone shape at 3 mm, the cone deforms significantly   SS is above 200 mm/s, and straight fibers can be observed
           at  4 mm.  To  achieve  stable printing,  the ratio of the   on the substrate.
           applied voltage to the nozzle-substrate distance should be
           kept in a reasonable range. At 3 mm, EHDP could avoid   4. CNN in EHDP Cone Modes’ Classification
           the  whipping  instability  and  realize  the  direct  writing
           of straight micro-/nano-fibers. With the increase of this   Conventional  machine  learning algorithms  such as
           distance to 3.5 mm and above, the serpentine structures   support vector (v) machines have limited  capability
           are observed on the substrate.                      to  process  natural  data  (such  as  the  pixel  values  of
           At  3 mm,  the  deposited  fiber  patterns  on  the  substrate   an  image).  Constructing  a  pattern  recognition  system
           may vary with the applied voltage as shown in Figure 4.   requires  considerable  domain  expertise  to  design  a
           When the applied voltage is about 2.6–3 kV, the straight   feature  extractor  which  transforms  these  data  into
           fiber can be collected on the substrate. When the applied   suitable features for these learning algorithms. Applying
           voltage  reaches  to  3.2 kV,  the  fiber  patterns  change  to   these algorithms in EHDP cone mode classification need
           serpentine  structure.  The  amplitude  of  the  serpentine   to go through both feature extraction and classification
           structure  increases  significantly  at  3.4 kV  applied   processes  in  a  separated  way,  which  inevitably  lead  to
           voltage. Through adjusting the key process parameters,   information loss. Furthermore, a feature selection process

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