In this paper, the amorphous PVDF (Polyvinylidene Fluoride) and PE (Polyethylene) models are established. The relationship between configuration density and temperature is calculated by molecular dynamics simulation. The rationality of model is determined by comparing with the experimentally determined glass transition temperature T. Secondly, the strain gradient is applied to the main chain carbon atoms of the amorphous PVDF and PE equilibrium configuration. Electric polarization occurs when the microstructure of the configuration changes. The transverse flexoelectric coefficients μ of amorphous PVDF and PE configurations are 1.24×10 C/m and -2.63×10 C/m, respectively, obtained by fitting the relationship between polarization and strain gradient. Finally, through the micromechanical analysis, the CF and CH dipoles rotate around the main chain along the inner side of the curved surface under the strain gradient, accompanied by some small structural adjustments. This leads to the electric polarization of the amorphous PVDF and PE configuration. Due to the difference in charge number and electronegativity between the amorphous PVDF and PE groups, the calculated transverse flexoelectric coefficients of the amorphous PVDF and PE are opposite, and the absolute value of the transverse flexoelectric coefficient of PE is greater than that of PVDF.
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http://dx.doi.org/10.1016/j.jmgm.2019.07.005 | DOI Listing |
Polymers (Basel)
January 2025
School of Computer Engineering, Weifang University, Weifang 261061, China.
Polymeric dielectrics have garnered significant interest worldwide due to their excellent comprehensive performance. However, developing polymeric dielectric films with high permittivity () and breakdown strength () and low dielectric loss (tan) presents a huge challenge. In this study, amorphous aluminum oxide (AlO, AO) transition interfaces with nanoscale thickness were constructed between titanium oxide (TiO, TO) nanosheets and polyvinylidene fluoride (PVDF) to manufacture composites (PVDF/TO@AO).
View Article and Find Full Text PDFJ Colloid Interface Sci
April 2025
Department of Physics, Nanchang University, Nanchang 330031, China. Electronic address:
Polyvinylidene fluoride (PVDF) materials have been widely investigated as polymer matrix for solid polymer electrolytes (SPEs) due to their high dielectric constant, electroactive effect (piezo-, pyro-, and ferroelectricity), and excellent thermal stability. However, the poor interface compatibility caused by highly reactive residual solvents and unsatisfactory ionic conductivity owing to sluggish Li transport kinetics are principal bottlenecks impeding the further development of PVDF-based electrolytes. Herein, we design a PVDF-based electrolytes with the assistance of hydrophilic-amorphous silica (HA-SiO).
View Article and Find Full Text PDFSoft Matter
November 2024
Department of Physics & Astronomy, Tufts University, Medford, MA 02155, USA.
This study reports the fabrication of non-woven fibrous membranes from electrospinning blended solutions of PVDF with polyampholytes in -dimethylformamide and methanol. Polyampholytes are macromolecules that have both positive and negative charged units in different side groups attached to the backbone. In this study, we used a random polyampholyte amphiphilic copolymer (r-PAC) synthesized by co-polymerizing a hydrophobic monomer in addition to the positive and negative charged monomer units, to reduce the fouling propensity of PVDF electrospun membranes while preserving its inherent hydrophobicity.
View Article and Find Full Text PDFPhys Chem Chem Phys
September 2024
Department of Energy Science and Engineering, DGIST, Daegu 42988, Korea.
Ferroelectric β-phase crystals of a polyvinylidene fluoride (PVDF) polymer grown or deposited on a graphene channel of a field effect transistor would induce various degrees of electrostatic doping (, various amounts of charge carriers) into graphene and in turn ON/OFF switching of the device, only if the electric field applied at the gate can reorient its polarization (, the well-aligned F-to-H dipole moments perpendicular to the all-trans polymer backbone) around the polymer backbone. To assess the feasibility of achieving a β-PVDF/graphene ferroelectric field effect transistor or memory device, we mimic (1) the electric-field-controlled PVDF polarization reversal (with density functional theory calculations and molecular dynamics simulations) and (2) the conductance switching of β-PVDF/graphene by PVDF reorientations (F-, H- and FH-down) representing a cycle of gate-voltage sweep (with density functional theory combined with non-equilibrium Green's function formalism). The low energy barrier of the collective synchronous PVDF chain rotation around the backbone (0.
View Article and Find Full Text PDFACS Appl Mater Interfaces
July 2024
Department of Materials Engineering, Indian Institute of Science (IISc), C V Raman Avenue, Bangalore 560012, Karnataka, India.
The switching of conventional field-effect transistors (FETs) is limited by the Boltzmann barrier of thermionic emission, which prevents the realization of low-power electronics. In order to overcome this limitation, among others, unconventional device geometry with a ferroelectric/dielectric insulator stack has been proposed to demonstrate stable negative-capacitance behavior. Here, the switching of the ferroelectric layer behaves like a step-up amplifier and results in a body factor less than 1.
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