2019
DOI: 10.1002/polb.24814
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Enhanced dielectric performance and energy storage of PVDF‐HFP‐based composites induced by surface charged Al2O3

Abstract: In order to enhance dielectric properties and energy storage density of poly(vinylidene fluoride‐hexafluoro propylene) (PVDF‐HFP), surface charged gas‐phase Al2O3 nanoparticles (GP‐Al2O3, with positive surface charges, ε’ ≈ 10) are selected as fillers to fabricate PVDF‐HFP‐based composites via simple physical blending and hot‐molding techniques. The results show that GP‐Al2O3 are dispersed homogeneously in the PVDF‐HFP matrix and the existence of nanoscale interface layer (matrix‐filler) is investigated by SAX… Show more

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Cited by 39 publications
(42 citation statements)
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References 74 publications
(71 reference statements)
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“…Comparison of previous published data and our work (1#, 42 2#, 43 3#, 43 4#, 18 5#, 44 6#, 45 7#, 22 8#, 46 and 9# 40 ). PVDF, polyvinylidene fluoride; TNSs, titania nanosheets [Color figure can be viewed at wileyonlinelibrary.com]…”
Section: Resultssupporting
confidence: 77%
See 1 more Smart Citation
“…Comparison of previous published data and our work (1#, 42 2#, 43 3#, 43 4#, 18 5#, 44 6#, 45 7#, 22 8#, 46 and 9# 40 ). PVDF, polyvinylidene fluoride; TNSs, titania nanosheets [Color figure can be viewed at wileyonlinelibrary.com]…”
Section: Resultssupporting
confidence: 77%
“…Meanwhile, the unique 2D structure of TNSs plays an important role in enhancement of breakdown strength. According to the F I G U R E 9 Comparison of previous published data and our work (1#, 42 2#, 43 3#, 43 4#, 18 5#, 44 6#, 45 7#, 22 8#, 46 and 9# 40 ). PVDF, polyvinylidene fluoride; TNSs, titania nanosheets [Color figure can be viewed at wileyonlinelibrary.com] previously reported literatures, the TNSs can act as charge barriers under electric field, 39,40 which prevents the formation of electric conductive paths in the nanocomposites.…”
Section: Breakdown Strength and Energy Storagementioning
confidence: 77%
“…Compared with the LTNSs, the STNSs possess largely increased ultimately exposed active sites and hydroxyl groups, which could induce more β phase transition. 31…”
Section: Resultsmentioning
confidence: 99%
“…It can be obtained as Us=EnormaldD${U_{\rm{s}}} = \smallint E{\rm{d}}D$, which can be determined by the electric displacement (D) and the applied electric field (E). [ 13–18 ] For ideal linear dielectrics, the energy loss due to leakage conduction is assumed to be zero in the charge and discharge processes because ε r does not vary with E. The U e of linear dielectrics is related to E and ε r , as follows: Us=12εrε0E2${U_{\rm{s}}} = \frac{1}{2}{\varepsilon _{\rm{r}}}{\varepsilon _0}{E^2}$, where ε 0 = 8.85 × 10 −12 Fm −1 is the vacuum permittivity. For nonlinear dielectrics, there is always an energy loss issue during the charging and discharging processes.…”
Section: Introductionmentioning
confidence: 99%