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Traceable Measurements of the Static Permittivity of Dielectric Reference Liquids at Temperatures from 5 to 50 deg C using a Micrometer Driven Admittance Cell

机译:使用千分尺驱动导纳电池可追溯到介电参考液体的静电介电常数,从5至50℃的温度下

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Traceability of RF and Microwave dielectric measurements is much facilitated by the use of reference dielectrics and NPL has been pursuing a programme of measurements to make more of these materials available [1]. Both solid and liquid reference materials have their value, but the former suffer from variability of electrical properties from one manufactured batch to another. Reference liquids have the advantage that samples of a high-purity grade taken straight from a newly-opened bottle are very consistent and so their properties can be published for use in the calibration and checking of instruments for complex permittivity measurements. To suit this purpose liquids having a range of complex permittivities are required. Both non-polar and polar reference liquids are useful, as they have quite different properties. Non-polar liquids (e.g. cyclohexane and silicone oil) generally have low permittivity, low loss, low temperature coefficient and low frequency dependence of permittivity, whereas polar liquids (e.g. alcohols and water) have none of these characteristics. Polar liquids with short-chain molecules (e.g. water, methanol and ethanol) are of value for calibrating and checking high loss, aqueous and particularly biological tissue measurements. Their dielectric behaviour throughout much of the RF and microwave range is conveniently described by dielectric relaxation models, such as the single and multiple Debye models [2, 3]. They allow the complex permittivity to be calculated easily from the relaxation parameters at a specified frequency and temperature. One of the most important of these parameters is the 'static' (i.e. low frequency) permittivity [2, 3]. A limited programme of RF and Microwave measurements on reference liquids was carried out at NPL during the years 1990-1992 [2]. This covered measurements of static permittivity in a micrometer-driven admittance cell and measurements of high-frequency permittivity (up to 3 GHz) in coaxial transmission line cells. The earlier project was limited, however, to a temperature range of 20 - 30 deg C, which does not encompass the full industrial range of interest, and the number of measurements undertaken was limited by the slowness of the temperature control in the admittance cell. Full experimental details of this earlier work have not previously been published and some of the details are given here for the first time. The current programme extends the earlier work in three ways: (i) the temperature control of the liquid admittance cell has been improved, allowing for faster, more reliable control, (ii) a wider range of temperatures is possible: 5 - 50 deg C, (iii) a wider range of liquids is being measured. The static permittivity measurements reported here will be followed by RF & Microwave measurements next year. When the work has been completed, results will be published in NPL reports.
机译:射频和微波介电测量的可追溯性多通过使用参考电介质容易,NPL一直追求的测量程序,使更多的可用的[1]这些材料。固体和液体的参考材料具有其值,但是从电性能从一个制造批次的不同的变性前者受到影响。参考液体具有的优点是从新开瓶直取高纯度等级的样本非常一致,因此它们的属性可以发布在校准使用和手段复介电常数测量的检查。为了满足这一目的的液体有需要复杂的介电常数的范围内。这两种非极性和极性参考液体是有用的,因为它们具有完全不同的性质。非极性液体(例如环己烷和硅油)通常具有低的介电常数,低损耗,低温度系数和介电常数的低频率的依赖性,而极性液体(例如醇和水)没有这些特性。与短链分子(例如水,甲醇和乙醇)极性液体是有价值的,用于校准和检查高损耗,水性和尤其生物组织的测量。他们的整个多射频和微波范围的介电性能可方便地由介电弛豫模型,例如单和多德拜模型[2,3]中描述。它们允许容易地从松弛参数在指定的频率和温度计算得到的复介电常数。其中最重要的这些参数中的是“静态”(即低频率)介电常数[2,3]。对参考液体射频和微波测量的有限程序在NPL在1990 - 1992年年[2]进行。在千分尺驱动的导纳细胞静态电容的这种覆盖测量和高频介电常数(高达3 GHz)在同轴传输线的小区的测量。然而,早期的项目是有限的,以一个温度范围20 - 30摄氏度,这不包括全工业范围的利益,且进行测量的次数是通过在导纳小区中的温度控制的缓慢限制。这个早期工作的全部实验细节以前没有被公布,一些细节在这里给出的第一次。当前程序扩展了早期的工作方式有三种:(i)所述液体导纳电池的温度控制进行了改进,从而允许更快,更可靠的控制,(ⅱ)一个较宽的温度范围内是可能的:5 - 50℃下,(ⅲ)的液体的更宽范围的被测量。静态电容测量人员在这里之后,将射频和微波测量明年。当工作已经完成,结果将刊登在NPL报告。

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