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首页> 外文期刊>Carbon: An International Journal Sponsored by the American Carbon Society >Electret, piezoelectret, dielectricity and piezoresistivity discovered in exfoliated-graphite-based flexible graphite, with applications in mechanical sensing and electric powering
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Electret, piezoelectret, dielectricity and piezoresistivity discovered in exfoliated-graphite-based flexible graphite, with applications in mechanical sensing and electric powering

机译:基于剥离 - 石墨的柔性石墨中发现的驻极体,压电,电介质和压阻性,具有机械传感和电力的应用

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This paper reports the in-plane dielectric, electret, piezoelectret and piezoresistive behavior of exfoliated-graphite-based flexible graphite, with demonstrated feasibility of electret-based electric powering and piezoelectret-based/piezoresistivity-based mechanical stress sensing under elastic tension. The powering is enabled by the inherent DC electric field E and DC electrical conductivity (resistivity rho = 7.5 x 10(-6 )Omega m). E is supported by relative permittivity kappa = 1170 and directionally asymmetric polarization-induced electrical resistance increase. It increases linearly with increasing inter-electrode distance l, with E = 2.6 x 10(-5) V/m at l= 40 mm. With increasing stress, E, rho, kappa and capacitance increase monotonically; E and rho increase smoothly - totally reversibly for stress <= 1.85 MPa and slightly irreversibly for stress between 1.85 and 3.18 MPa. The fractional increases in E and kappa at <= 3 MPa are <= 110% and <= 73%, respectively. The kappa-stress curve abruptly increases in slope at 2.1 MPa, which is accompanied by the onset of some kappa increase irreversibility. This 2.1-MPa slope increase is attributed to a microstructural change that does not affect the strain reversibility or rho, but increases kappa. The change possibly involves interfacial loosening, which promotes polarization without affecting conduction. The piezoelectret coupling coefficient d(33) is 3.7 x 10(-8) pC/N. The piezoresistivity gage factor is 50. (C) 2019 Elsevier Ltd. All rights reserved.
机译:本文报道了基于剥离 - 石墨型柔性石墨的面内电介质,驻极体,压电电和压阻性能,并在弹性张力下证明了基于驻极体的电力和基于压电电流/压电电阻的基于压电的机械应力传感的可行性。通过固有的直流电场E和直流电导率(电阻率RHO = 7.5×10(-6)OMEGA M)实现电力。 E由相对介电常数Kappa = 1170和定向的不对称偏振引起的电阻增加支持E.它随着电极间距离L的增加而线性增加,E = 2.6×10( - 5)v / m在L = 40mm。随着压力的增加,e,rho,κ和κ和电容单调增加; e和rho平稳地增加 - 完全可逆地用于应力<= 1.85 MPa,略微不可逆地,应对1.85和3.18 MPa之间的应力。 E和Kappa的分数增加分别为<= 3MPa的<= 110%和<= 73%。 Kappa-ressuly曲线在2.1MPa的斜率下突然增加,伴随着一些Kappa的发作增加了不可逆转性。该2.1-MPA斜率增加归因于不影响应变可逆性或rho的微观结构变化,而是增加了κBAPA。可能涉及界面松动的变化,这促进了极化而不影响传导。压电耦合系数D(33)是3.7×10(-8)PC / n。压阻性测量因子是50.(c)2019 Elsevier Ltd.保留所有权利。

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