TY - JOUR
T1 - Correlation between processing parameters and microstructure of electrospun poly(D,l-lactic acid) nanofibers
AU - Wang, Chi
AU - Chien, Huan Sheng
AU - Yan, Kuo Wei
AU - Hung, Chien Lin
AU - Hung, Kan Lin
AU - Tsai, Shih Jung
AU - Jhang, Hao Jhe
N1 - Funding Information:
The financial support for this work has been received from the National Science Council of Taiwan (NSC 92-2216-E-006-016), Taiwan Textile Research Institute (TTRI), Industrial Technology Research Institute (ITRI) as well as the NCKU through the “Landmark Program of the NCKU top University Project”.
PY - 2009/11/27
Y1 - 2009/11/27
N2 - Using dimethyl formamide as the solvent, electrospinning of poly(D,l-lactic acid) (PDLLA, d-lactide content:10%) solutions with various concentrations was performed by means of a heating jacket for controlling the solution temperature range from 25 to 104 °C. In addition, an IR emitter was used to control the surrounding temperature at ∼110 °C. The effects of solution properties and processing variables on the morphologies of the cone/jet/fiber were investigated, and the internal structure of the electrospun fibers was characterized using polarized FTIR, WAXD and DSC. A sufficient entanglement density existing in a given solution was an important requirement for successfully obtaining uniform fibers without beads. The log-log plot of specific viscosity (ηsp) versus PDLLA volume fraction (φ{symbol}v) provided us with a useful guideline to determine the entanglement concentration (ce) for preparing fiber-shaped electrospun products. The φ{symbol}v-dependence of ηsp varied from ηsp ∼ φ{symbol}v 1.1 for a dilute solution to ηsp ∼ φ{symbol}v 4.7 for a solution possessing entangled chains. From the incipient concentration of entanglements, the determined ce was ∼10 wt%, which was in fair agreement with what was predicted theoretically by a simple relation of 2Me/Mw, where Me and Mw were the molecular weight between melt entanglements and the average molecular weight of PDLLA, respectively. To obtain uniform PDLLA fibers without beads, however, a minimum concentration of ∼1.9ce was required for the entangled solutions possessing sufficient network strength to prohibit the capillary instability during jet whipping. The log-log plots of the jet diameter (dj) and fiber diameter (df) versus zero shear viscosity (ηo) showed two scaling laws existing for the present solution, that is, dj ∼ ηo 0.07 and df ∼ ηo 0.45. For a given solution, an intimate relation between dj and df was derived to be df ∼ dj 0.61, regardless of the variations of processing variables applied. High-temperature electrospinning produced small diameter fibers because of the reduction of ηo, but the effect was gradually diminished for solution temperatures higher than 56 °C owing to the enhanced solvent evaporation. The as-spun nanofibers of this thermally slow-crystallizing PDLLA species were amorphous, and the Hermans orientation function calculated from the polarized FTIR results was ca. -0.063 regardless of the electrospinning conditions applied. This suggests that there was no preferential chain orientation developed in the nanofibers. In the heating in a DSC cell at a rate of 10 °C/min, however, rapid crystallization took place at 97 °C, followed by two well-separated melting endotherms centered at 121 and 148 °C, respectively. WAXD and FTIR results exhibited the exclusive presence of α-form crystals. These unique features were attributed to the occurrence of phase separation during electrospinning, which interrupted the chain orientation along the fiber during jet stretching, and yielded more trans-trans conformers with more extended chain structure to readily facilitate the cold crystallization during post-heating.
AB - Using dimethyl formamide as the solvent, electrospinning of poly(D,l-lactic acid) (PDLLA, d-lactide content:10%) solutions with various concentrations was performed by means of a heating jacket for controlling the solution temperature range from 25 to 104 °C. In addition, an IR emitter was used to control the surrounding temperature at ∼110 °C. The effects of solution properties and processing variables on the morphologies of the cone/jet/fiber were investigated, and the internal structure of the electrospun fibers was characterized using polarized FTIR, WAXD and DSC. A sufficient entanglement density existing in a given solution was an important requirement for successfully obtaining uniform fibers without beads. The log-log plot of specific viscosity (ηsp) versus PDLLA volume fraction (φ{symbol}v) provided us with a useful guideline to determine the entanglement concentration (ce) for preparing fiber-shaped electrospun products. The φ{symbol}v-dependence of ηsp varied from ηsp ∼ φ{symbol}v 1.1 for a dilute solution to ηsp ∼ φ{symbol}v 4.7 for a solution possessing entangled chains. From the incipient concentration of entanglements, the determined ce was ∼10 wt%, which was in fair agreement with what was predicted theoretically by a simple relation of 2Me/Mw, where Me and Mw were the molecular weight between melt entanglements and the average molecular weight of PDLLA, respectively. To obtain uniform PDLLA fibers without beads, however, a minimum concentration of ∼1.9ce was required for the entangled solutions possessing sufficient network strength to prohibit the capillary instability during jet whipping. The log-log plots of the jet diameter (dj) and fiber diameter (df) versus zero shear viscosity (ηo) showed two scaling laws existing for the present solution, that is, dj ∼ ηo 0.07 and df ∼ ηo 0.45. For a given solution, an intimate relation between dj and df was derived to be df ∼ dj 0.61, regardless of the variations of processing variables applied. High-temperature electrospinning produced small diameter fibers because of the reduction of ηo, but the effect was gradually diminished for solution temperatures higher than 56 °C owing to the enhanced solvent evaporation. The as-spun nanofibers of this thermally slow-crystallizing PDLLA species were amorphous, and the Hermans orientation function calculated from the polarized FTIR results was ca. -0.063 regardless of the electrospinning conditions applied. This suggests that there was no preferential chain orientation developed in the nanofibers. In the heating in a DSC cell at a rate of 10 °C/min, however, rapid crystallization took place at 97 °C, followed by two well-separated melting endotherms centered at 121 and 148 °C, respectively. WAXD and FTIR results exhibited the exclusive presence of α-form crystals. These unique features were attributed to the occurrence of phase separation during electrospinning, which interrupted the chain orientation along the fiber during jet stretching, and yielded more trans-trans conformers with more extended chain structure to readily facilitate the cold crystallization during post-heating.
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U2 - 10.1016/j.polymer.2009.10.025
DO - 10.1016/j.polymer.2009.10.025
M3 - Article
AN - SCOPUS:70449721096
SN - 0032-3861
VL - 50
SP - 6100
EP - 6110
JO - polymer
JF - polymer
IS - 25
ER -