2019
DOI: 10.1016/j.nanoen.2019.05.044
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Thermodynamic approach to tailor porosity in piezoelectric polymer fibers for application in nanogenerators

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Cited by 48 publications
(59 citation statements)
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“…5(C,D)). This observation is in agreement with recent literature 42,43 . At polymer concentrations ≤15 wt%, a larger volume fraction of solvent has to evaporate first before the fiber can solidify which in turn increases the drying time.…”
Section: Resultssupporting
confidence: 94%
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“…5(C,D)). This observation is in agreement with recent literature 42,43 . At polymer concentrations ≤15 wt%, a larger volume fraction of solvent has to evaporate first before the fiber can solidify which in turn increases the drying time.…”
Section: Resultssupporting
confidence: 94%
“…The production of porous or micro-/nanofibers is of high interest for reducing their weight and increasing their surface to volume ratio. For example, such porous or grooved fibers can be obtained by electrospinning and controlling the polymer/solvent/anti-solvent interaction 42,43 . The underlying mechanism of such processes relies on the formation of pores upon the evaporation from the polymer-poor phase and solidification of the polymer-rich phase, which is also reflected by the phase diagrams of such ternary phases 42,43 .…”
Section: Resultsmentioning
confidence: 99%
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“…It has been shown that energy harvesters based on porous P(VDF‐TrFE) films as well as nanofibers, with pores that are confined inside the polymer, show enhanced power output of the generator. [ 36 ] In the next step of FEM simulations we therefore introduced spherical air cavities inside the δʹ ‐phase nanofiber. The peak voltage is calculated for a fixed pressure of 250 kPa for stress‐charge mode.…”
Section: Resultsmentioning
confidence: 99%
“…The enhancement of the peak voltage is due to lowering of the relative permittivity and the enhancing deformability of the nanofibers upon increasing the amounts of pores. For a porous dielectric film consisting of spherical closed pores, the relative permittivity, ε′, decreases monotonically with the fractional porosity, P , as [ 36,37 ] ε= ε13Pfalse(ε 1false)Pε + 1 P + 2ε, where, ε = 4 [ 22 ] is the relative dielectric permittivity of nylon‐11. For the ideal case of uniformly distributed isolated spherical pores, the dielectric permittivity continuously drops as porosity increases to 2.67 for a fiber that is 37.5% porous.…”
Section: Resultsmentioning
confidence: 99%