TY - JOUR
T1 - Extension rate of the straight jet in electrospinning of poly(N-isopropyl acrylamide) solutions in dimethylformamide
T2 - Influences of flow rate and applied voltage
AU - Wang, Yu
AU - Hashimoto, Takeji
AU - Li, Chang Chou
AU - Li, Yang Cheng
AU - Wang, Chi
N1 - Funding Information:
This work was supported by the Ministry of Science and Technology, Taiwan, Republic of China (research grants MOST103-2221-E-006-262-MY3 and MOST106-2221-E-006-211-MY3).
Publisher Copyright:
© 2017 Wiley Periodicals, Inc.
PY - 2018/2/15
Y1 - 2018/2/15
N2 - In the electrospinning process, the measurement of extension rate of the straight jet is not an easy task. In this study, the diameter profile of the tapering straight jet is determined with a laser light-scattering technique. Afterwards, the jet extension rate ɛ is derived and used to compare with the solution-intrinsic rates, for example, the terminal relaxation rate and the Rouse relaxation rate. The extension rate of the straight jet depends on position: it is highest near the cone apex (region I) and decays to a constant value in the major jet (region II) until approaching the jet end (region III), at which the extension rate abruptly drops to nearly zero, that is, ɛI > ɛII ≫ ɛIII ∼ 0. The jet diameter in region III is independent of solution concentration and applied voltage, but is scaled to the flow rate with an exponent of ∼0.37. The derived exponent is consistent with a simple prediction based on the counterbalance between the stretching electric force and the compressive force induced by the air drag force. Provided that air friction becomes overwhelming at the straight jet end, the long electrified jet is likely to buckle, thereby triggering the instability of jet whipping.
AB - In the electrospinning process, the measurement of extension rate of the straight jet is not an easy task. In this study, the diameter profile of the tapering straight jet is determined with a laser light-scattering technique. Afterwards, the jet extension rate ɛ is derived and used to compare with the solution-intrinsic rates, for example, the terminal relaxation rate and the Rouse relaxation rate. The extension rate of the straight jet depends on position: it is highest near the cone apex (region I) and decays to a constant value in the major jet (region II) until approaching the jet end (region III), at which the extension rate abruptly drops to nearly zero, that is, ɛI > ɛII ≫ ɛIII ∼ 0. The jet diameter in region III is independent of solution concentration and applied voltage, but is scaled to the flow rate with an exponent of ∼0.37. The derived exponent is consistent with a simple prediction based on the counterbalance between the stretching electric force and the compressive force induced by the air drag force. Provided that air friction becomes overwhelming at the straight jet end, the long electrified jet is likely to buckle, thereby triggering the instability of jet whipping.
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U2 - 10.1002/polb.24544
DO - 10.1002/polb.24544
M3 - Article
AN - SCOPUS:85034243686
SN - 0887-6266
VL - 56
SP - 319
EP - 329
JO - Journal of Polymer Science, Part B: Polymer Physics
JF - Journal of Polymer Science, Part B: Polymer Physics
IS - 4
ER -