共查询到16条相似文献,搜索用时 296 毫秒
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《计量技术》2016,(9)
汞三相点(-38. 8344℃)是ITS-90国际温标重要的定义固定点之一。为提高汞三相点复现水平,实现-38. 8344~29. 7646℃海水温度的高精度测量,满足海水温度校准需求,开展了汞三相点研究。本文介绍了金属外壳的汞三相点容器及热管自动复现装置、汞三相点的复现过程及测量结果。实验结果表明:热管汞点复现装置可高精度复现汞三相点。采用测量精度为0. 2×10~(-6)的1594A测温电桥时熔化温坪稳定后19小时温度变化小于0. 2mK。采用测量精度为0. 02×10~(-6)的6622A-XPS测温电桥时,18小时内的汞点熔化温坪变化小于0. 1mK。因此,汞点复现水平与测量电桥的精度有关。 相似文献
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介绍了微型镓基共晶固定点的灌注工艺和准绝热相变特性测量系统;结合空腔黑体和非近位安装的温度传感器,研究了Ga-Sn和Ga-Zn共晶固定点的相变温坪重复性和Ga固定点的相变温坪长期稳定性;通过特定的热环境下镓及2个镓基共晶固定点三者熔化过程中温度传感器测量到的相变温坪值,对嵌入空腔黑体底部的温度传感器进行校准,其校准结果与实验室常规校准方法得到的结果差异均小于2mK。实验结果表明:在热环境保持不变的条件下,随着相变时间的增加,相变温坪值就越靠近理论上相变物质的熔化温度,即固定点与温度传感器测孔之间的异位温差越小;对于Ga-Sn和Ga-Zn共晶固定点,温度传感器测量到的相变温坪值与加热功率呈线性关系,零功率下的单点校准温度分别为20.352℃和25.187℃。 相似文献
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ITS-90温标固定点温坪受到诸多方面的影响,温场是其中重要影响因素之一。为提升温场性能弥补漏热造成的影响,借鉴低温固定点中广泛采用的绝热原理,设计基于准绝热的锌固定点装置,温场梯度性能由传统固定点的100 mK提升至20 mK,固定点高纯金属使用量由2.0kg降至200 g。实验结果表明该装置的温坪可持续时间较长,复现性0.1 mK,既能大幅度提升温场性能,同时达到了装置小型化、可重复使用经济实用的目的,又为高纯金属中微量杂质对相变温度的影响评估降低温场因素的干扰提供研究基础。 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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A multi-national project (the EMRP InK project) was completed recently, which successfully determined the thermodynamic temperatures of several of the high-temperature fixed points above the copper point. The National Metrology Institute of Japan contributed to this project with its newly established absolute spectral radiance calibration capability. In the current study, we have extended the range of thermodynamic temperature measurement to below the copper point and measured the thermodynamic temperatures of the indium point (\(T_{90} =\) 429.748 5 \(\hbox {K}\)), tin point (505.078 K), zinc point (692.677 K), aluminum point (933.473 K) and the silver point (1 234.93 K) by radiance comparison against the copper point, with a set of radiation thermometers having center wavelengths ranging from \(0.65\,\upmu \hbox {m}\) to \(1.6\,\upmu \hbox {m}\). The copper-point temperature was measured by the absolute radiation thermometer which was calibrated by radiance method traceable to the electrical substitution cryogenic radiometer. The radiance of the fixed-point blackbodies was measured by standard radiation thermometers whose spectral responsivity and nonlinearity are precisely evaluated, and then the thermodynamic temperatures were determined from radiance ratios to the copper point. The values of \(T-T_{90}\) for the silver-, aluminum-, zinc-, tin- and indium-point cells were determined as ?4 mK (\(U = 104\,\hbox {mK}, k=2\)), ?99 mK (88 mK), ?76 mK (76 mK), ?68 mK (163 mK) and ?42 mK (279 mK), respectively. 相似文献
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Hisashi Nakagawa 《International Journal of Thermophysics》2016,37(11):112
In this study, the Provisional Low Temperature Scale of 2000 (PLTS-2000) was realized below 650 mK for the purpose of launching low-temperature resistance thermometer calibration services in Japan. A Straty–Adams-type \(^{3}\)He melting pressure thermometer (MPT) and a dilution refrigerator were used to realize the PLTS-2000. Offsets due to hydrostatic pressure head in a filling capillary line of the MPT were adjusted using the minimum pressure fixed point on the \(^{3}\)He melting curve. A rather large MPT hysteresis between the decreasing and increasing pressures was observed during pressure calibration of the MPT and was the main source of uncertainty. The combined standard uncertainty (\(k = 1\)) between 50 mK and 650 mK was estimated to be in the range of 0.40 mK to 2.62 mK. The MPT and a number of resistance thermometers with negative temperature coefficients were mounted on the experimental platform with a thermal connection to a mixing chamber and compared in a multiple-temperature-point calibration. The temperature range around the melting pressure minimum, 250 mK to 400 mK, was not used for the calibration. The expanded uncertainty (\(k = 2\)) in the calibration based on realization of the PLTS-2000 between 50 mK and 650 mK was estimated to be in the range of 0.86 mK to 5.25 mK. 相似文献