共查询到19条相似文献,搜索用时 203 毫秒
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针对两种不同类型的工业铂电阻温度计(IPRTs),使其在-80℃和300℃下恒温一定时间后再测量其0℃下的电阻偏移,由此来确定其在该温度下的热迟滞性。试验结果表明:薄膜型铂电阻温度计在0℃的热迟滞性远大于铂丝型铂电阻温度计,并且随着测量次数的增多,热迟滞性会逐渐减小。 相似文献
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对研制成功的片状骨架结构高温铂电阻温度计进行了持续四年的试验研究。试验结果表明这种温度计的各种性能都很好,并突破了国外一些长期没有解决的技术难关。在1100℃退火,平均每百小时R_0的变化换算为温度约为1mK,快速热循环后(经中温补充退火)R_0的变化换算为温度也不超过1mK。温度计具有良好的抗震性能和热性能。在1064℃时的绝缘泄漏电阻大于27MΩ。石英套管的析晶问题已基本解决。 相似文献
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铂电阻温度计稳定性的研究 总被引:1,自引:0,他引:1
铂电阻温度计是ITS -1990国际温标中规定的内插仪器 ,也是复现保存温标及温标传递的必要仪器。同时在对各类水银温度计、工业铂电阻温度计等温度传感器及仪表的检定时都是最常用的标准 ,所以铂电阻温度计的稳定与否是非常重要的。铂电阻温度计的稳定性与多种因素有关 ,如制作温度计使用的铂丝均匀性、纯度及工艺 ,温度计的制作过程工艺及退火 ,充气处理 ,新制温度计的退火处理 ,温度计的使用等。这里主要对各类温度计的退火及使用中稳定性的变化做一些分析研究。一、铂电阻温度计的稳定性国际上评定铂电阻温度计的稳定性 ,主要是看其… 相似文献
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为了研究热迟滞性对工业铂电阻温度计测量不确定度的影响,选取了8支高精度铂电阻温度计进行实验。在-50~150℃内,选择3个温度区间,采用两种标准方法(IEC 60751,ASTM E644)测量水三相点(0.01℃)和所选温度范围内的中间点的迟滞性变化。实验结果表明:4支薄膜铂电阻温度计在两种标准方法测量下,随着温度区间跨度增大,热迟滞性影响增大,IEC 60751标准方法测量的热迟滞性最大值为14.2mK,ASTM E644标准方法测量的热迟滞性最大值为20.5mK;选取4支铂丝铂电阻温度计在温度范围为-50~150℃测量时,IEC 60751和ASTM E644标准方法测量的热迟滞性数据最大值分别为1.1mK和0.9mK;铂丝铂电阻温度计热迟滞性明显小于薄膜铂电阻温度计。 相似文献
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铂丝的位错是影响标准铂电阻温度计性能稳定性的重要因素之一。从微观角度出发,借助X射线衍射(XRD)分析方法,开展了退火时间对铂丝位错密度影响的研究,并利用标准铂电阻温度计退火实验数据进行了验证。结果表明:实际用于标准铂电阻温度计直径为0.07mm的新制铂丝(纯度99.999%)平均位错密度随着退火时间呈指数减小,经过100h退火后位错密度从1012cm-2下降到1011cm-2,300h后其位错密度基本保持稳定;新制标准铂电阻温度计在退火前300h其水三相点电阻值明显减小,退火300h后水三相点值变化量小于3mK并趋于平稳,此结果从热处理时间上与铂丝位错实验结果基本吻合。研究结果为标准铂电阻温度计制作工艺的提升及计量检定规程的修订提供技术支撑 相似文献
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利用俄歇电子能谱(AES)和X射线衍射(XRD)分析了室温条件下离子束外延生长Ga、Mn、As样品,在不同的温度条件下进行退火后组分和元素分布的变化。结果表明退火有助于样品内部元素的均匀分布,温度为400℃会导致MnO2和Ga5.2Mn的结晶。 相似文献
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R. Ding M. J. Zhao E. Nerdrum D. Meier 《International Journal of Thermophysics》2011,32(11-12):2252-2260
A triple-point-of-argon system was developed to realize the argon triple-point temperature defined in the International Temperature Scale of 1990 (ITS-90) and to calibrate long-stem standard platinum resistance thermometers (SPRTs). The system structure, the techniques for realization of the triple-point temperature, and the testing results are presented in this paper. In this system, there is a central argon cell that includes four re-entrant wells with an immersion depth of 160?mm which can be used to calibrate four long-stem SPRTs simultaneously. A high-accuracy temperature controller is used to control the realization process of the argon triple-point temperature plateau. The argon triple-point plateau can be easily realized with this system. The influence of different experimental parameters on the triple-point-of-argon plateau was investigated and is discussed. The testing results show that the duration of the plateau can be over 100?h with the temperature change less than 0.05?mK. The temperature homogeneity of the four re-entrant wells was tested. The immersion profile of the system was measured, and the measurement results were compared with the ITS-90 hydrostatic values. The uncertainty analysis shows that the uncertainty of the argon system is 0.25?mK (k = 2). 相似文献
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D. R. White M. Ballico D. del Campo S. Duris E. Filipe A. Ivanova A. Kartal Dogan E. Mendez-Lango C. Meyer F. Pavese A. Peruzzi E. Renaot S. Rudtsch T. Wang K. Yamazawa 《International Journal of Thermophysics》2010,31(8-9):1749-1761
The CCT has completed the guide summarizing the uncertainties in the realization of the SPRT subranges of ITS-90 between the triple point of neon (24.5561 K) and the freezing point of silver (961.78 °C). This article identifies aspects of standard platinum resistance thermometry where either data or models are lacking and further research is required. In the calibration of SPRTs, the two main concerns are the need for data on liquidus slopes for the different impurities in the fixed points and improved understanding of the impact of the thermal environment of the fixed point on the realized temperature. In the use of SPRTs, the two largest sources of uncertainty are Types 1 and 3 non-uniqueness and oxidation. The causes of Type 3 non-uniqueness are not yet understood, especially at low temperatures, and there is a paucity of data for the high-temperature subranges. In respect of oxidation, there is a need for validation of the models developed in the 1980s, especially in light of the reduced partial pressure of oxygen used in modern SPRTs. A range of other effects including vacancy effects in SPRTs, isotopic effects in fixed points, and improved statistical methods are discussed. 相似文献
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氩三相点作为国际温标ITS-90的重要低温固定点,在国家基准量值传递中有着重要的意义。中国计量科学研究院研制了基于准绝热原理的密封型氩三相点装置,能够对长杆铂电阻温度计进行氩三相点高精度复现,并且通过开发自动控制与测量软件实现了实验过程自动化测量与控制。实验结果表明,使用新研制的密封氩三相点装置使氩三相点的温坪时间提高到23 h以上,其中在16 h的温坪变化在0.2 mK以内,同时温坪复现性达到0.1 mK以内,成功解决了恒定热流法氩三相点复现过程中温坪时间短、复现难度大等问题,保证国家基准量值传递的准确性。 相似文献
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E. Filipe S. Gentil I. Lóio R. Bosma A. Peruzzi 《International Journal of Thermophysics》2018,39(2):26
Interpolation error is a major source of uncertainty in the calibration of standard platinum resistance thermometer (SPRT) in the subranges of the International Temperature Scale of 1990 (ITS-90). This interpolation error arises because the interpolation equations prescribed by the ITS-90 cannot perfectly accommodate all the SPRTs natural variations in the resistance–temperature behavior, and generates different forms of non-uniqueness. This paper investigates the type 3 non-uniqueness for fourteen SPRTs of five different manufacturers calibrated over the water–zinc subrange and demonstrates the use of the method of divided differences for calculating the interpolation error. The calculated maximum standard deviation of 0.25 mK (near \(100\,^{\circ }\hbox {C}\)) is similar to that observed in previous studies. 相似文献
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R. L. Rusby 《International Journal of Thermophysics》2010,31(8-9):1567-1572
This paper investigates the discontinuity in the derivative [dW/dT 90]TPW of the ITS-90 at the triple point of water, using data for over 40 calibrated standard platinum resistance thermometers (SPRTs). It finds that the discontinuity is in most cases somewhere between 0 and ?6 parts in 105, in relative terms, but that the higher numerical values are obtained for ‘less ideal’ SPRTs (those with lower temperature coefficients of resistance), and also for sub-ranges not extending beyond the indium point. These results are investigated vis-à-vis the long-standing observation that the ITS-90 reference values W r(Ga) and W r(Hg) are not completely consistent with data for W(Ga) and W(Hg) for real SPRTs. It discusses what may be done in a future scale to ensure continuity in the first derivative, and it concludes with a comment about the acceptance criteria for SPRTs in the scale. 相似文献