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Conductivity and space charge in LDPE/BaSrTiO3 nanocomposites

机译:LDPE / BaSrTiO 3 纳米复合材料的电导率和空间电荷

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Nano-sized BaSrTiO3 particles and a dispersant were incorporated in samples of low density polyethylene (LDPE). The nanoparticle loading was 2% or 10% by weight (w/w), and the dispersant loading was 4 parts per hundred relative to BaSrTiO3. dc conductivity measurements were made in the temperature range 30-70°C in vacuum, and in air at 30°C. The vacuum dc conductivity in samples containing only the dispersant (0.4%) was approximately five times larger than that in LDPE samples without additive, but approximately an order of magnitude larger than that in samples containing 10% nanoparticles and 0.4% dispersant. Addition of 10% nanoparticles and 0.4% dispersant increased ε'', the real part of the relative permittivity, from approximately 2.34 to around 2.58 at 30°C, in air and in vacuum. Space charge measurements were made in air using the Laser Intensity Modulation Method (LIMM), and the profiles calculated using the LIMM Monte Carlo method. The maximum space charge density adjacent to the negative poling electrode was 600 C/m3, for the pure LDPE and the LDPE with dispersant, and 200 C/m3 near the positive electrode. The corresponding maxima for LDPE with nanoparticles were approximately an order of magnitude smaller. The Monte Carlo method is more accurate than other methods of analyzing LIMM data, and this may account for the very large densities close to the electrodes.
机译:纳米BaSrTiO 3 颗粒和分散剂被掺入低密度聚乙烯(LDPE)样品中。相对于BaSrTiO 3 ,纳米颗粒的载量为2重量%或10重量%(w / w),分散剂的载量为每100份4份。直流电导率测量是在30-70°C的温度范围内,真空和30°C的空气中进行的。仅含有分散剂(0.4%)的样品的真空直流电导率约为不含添加剂的LDPE样品的五倍,但比含有10%纳米颗粒和0.4%分散剂的样品的真空直流电导率大一个数量级。在空气和真空中,在30°C下,相对介电常数的实部ε''(相对介电常数的实部)的添加将使ε''(相对介电常数的实部)从约2.34增至约2.58。使用激光强度调制方法(LIMM)在空气中进行空间电荷测量,并使用LIMM蒙特卡洛方法计算轮廓。对于纯LDPE和带有分散剂的LDPE,与负极极化电极相邻的最大空间电荷密度为600 C / m 3 ,而在靠近极化电极的附近,最大空间电荷密度为200 C / m 3 。正极。具有纳米颗粒的LDPE的相应最大值大约小一个数量级。蒙特卡洛方法比其他分析LIMM数据的方法更准确,这可能解释了靠近电极的非常大的密度。

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