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A Concerted International Project to Establish High-Temperature Fixed Points for Primary Thermometry
G. Machin P. Bloembergen J. Hartmann M. Sadli Y. Yamada 《International Journal of Thermophysics》2007,28(6):1976-1982
Research into high-temperature fixed points above 1,100°C has made significant progress since they were first reported in
1999. In particular, it has been established that single cells are repeatable at the sub-50 mK level, and intra-cell reproducibility
at the 100 mK level has been demonstrated even at temperatures as high as 2,500°C. The fixed points have been used to compare
temperature and radiometry scales over a wide temperature range, and are being developed and established as secondary references
for thermocouple calibrations. However, before they can be fully accepted as primary temperature references, much work remains
to be done, namely: (1) Establishment of long-term stability of the fixed-point temperature; (2) Development of robust procedures
for the reliable construction of the fixed-point cells (to ensure routine intra-cell reproducibility of 100 mK); (3) Demonstration
of long-term robustness of the fixed-point cells; (4) Assignment of thermodynamic temperatures to a selected set of fixed
points; (5) Agreement and acceptance of these temperature values by the CCT; (6) Agreed methods on how to take full utility
of these new fixed points into any future International Temperature Scale (ITS)—or the current ITS-90 via an addendum to the
mise en pratique for the definition of the kelvin. To ensure that this work progresses to completion in a reasonable time frame, a research
project, under the auspices of the CCT-WG5, has been formulated and is currently in progress with the aim of achieving the
above mentioned targets by 2012. This article will describe this project and detail partner contributions. 相似文献
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A. Burdakin B. Khlevnoy M. Samoylov V. Sapritsky S. Ogarev A. Panfilov S. Prokhorenko 《International Journal of Thermophysics》2009,30(1):20-35
Melting/freezing temperature curves are studied for the single-component Ga and bimetallic eutectic alloys Ga–In, Ga–Sn, Ga–Zn,
and Ga–Al in small-size cells. These phase-transition studies were conducted at VNIIOFI in order to design small-size fixed-point
devices for metrological monitoring of temperature sensors on autonomous (e.g., space borne) platforms. The results show that
Ga and some Ga-based eutectic alloys in small cells can be used as melting fixed points. The repeatability of melting temperatures
of Ga, Ga–In, Ga–Sn, and Ga–Zn fixed points is studied. The effects of the concentration of the second element of Ga-based
eutectic alloys and the thermal history on the melting plateau’s shape and the melting temperature are studied. 相似文献
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Saber G. R. Salim Nigel P. Fox Emma R. Woolliams Rainer Winkler Heather M. Pegrum Tong Sun Ken T. V. Grattan 《International Journal of Thermophysics》2007,28(6):2041-2048
A small palm-sized, reference spectrometer, mounted on a remote-controlled model helicopter is being developed and tested
by the National Physical Laboratory (NPL) in conjunction with City University, London. The developed system will be used as
a key element for field vicarious calibration of optical earth observation systems in the visible-near infrared (VNIR) region.
The spectrometer is hand held, low weight, and uses a photodiode array. It has good stray light rejection and wide spectral
coverage, allowing simultaneous measurements from 400 to 900 nm. The spectrometer is traceable to NPL’s primary standard cryogenic
radiometer via a high-temperature metal-carbon eutectic fixed-point blackbody. Once the fixed-point temperature has been determined
(using filter radiometry), the eutectic provides a high emissivity and high stability source of known spectral radiance over
the emitted spectral range. All wavelength channels of the spectrometer can be calibrated simultaneously using the eutectic
transition without the need for additional instrumentation. The spectrometer itself has been characterized for stray light
performance and wavelength accuracy. Its long-term and transportation stability has been proven in an experiment that determined
the “World’s Bluest Sky”—a process that involved 56 flights, covering 100,000 km in 72 days. This vicarious calibration methodology
using a eutectic standard is presented alongside the preliminary results of an evaluation study of the spectrometer characteristics. 相似文献
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Under the cold-chamber high pressure die casting (HPDC) process, samples were produced with AM60B magnesium alloy to investigate the microstructure characteristics of the eutectics, especially focusing on the constitution, morphology and distribution of the eutectics over cross section of the castings. Attentions were also paid to study the effect of heat treatment on the eutectics in the die castings. Based on experimental analysis using optical microscopy (OM), X-ray diffraction (XRD), scanning electron microscopy (SEM) and energy-dispersive spectroscopy (EDS), it was determined that fully divorced eutectics consisting of α-Mg and β-Mg17Al12 appeared at the grain boundary of the primary α-Mg in the as-cast microstructure. Islands and networks of β-Mg17Al12 phase were observed in the central region of the castings, while the β-Mg17Al12 phase revealed a more dispersed and granular morphology on the surface layer. The two phases ratio β/α in the central region of the castings was approximately 10%, which was higher than that on the surface layer. Besides, the defect bands contained a higher percentage of the eutectics than the adjacent regions. After aging treatment (T6), only α-Mg phase was detected by XRD in the AM60B magnesium alloy, though a small amount of precipitated β-Mg17Al12 phase was observed at the grain boundary. In contrast to the microstructure of die cast AZ91D magnesium alloy under the same T6 heat treatment, no discontinuous precipitation of the β-Mg17Al12 phase was observed in AM60B magnesium alloy die castings. 相似文献
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Glass surface temperature can be measured using a radiation thermometer operating at a mid-IR wavelength, typically the 3–5 μm band, where the glass is opaque. For optical fiber preforms, the temperature measurement requirement may exceed 2,200°C.
Scale realization at national measurement institutes at these temperatures is usually carried out at short wavelengths, typically
less than 1 μm. The mismatch in wavelength can lead to significant uncertainties when calibrating a radiation thermometer working at 3–5 μm. To overcome this, a narrow band 3.95 μm radiation thermometer has been built that is designed to be used from 1,000 to 2,500°C. It is calibrated by measurement
of high-temperature metal–carbon eutectic fixed-points. The instrument is based on silicon lenses, with a liquid nitrogen
(LN2)-cooled InSb detector, and narrow-band interference filter. An anti-reflection coated objective lens/aperture stop focuses
onto a field stop giving a 1 mm target, then a collimating lens, and glare stop. All parts visible to the detector, other
than the target area, are either at LN2 temperature or are part of a temperature-stabilized housing. A relay-operated shutter that blocks the field stop is used
to subtract the background. The size-of-source effect of the instrument has been measured. Gold-point measurements have been
made to assess the stability. The device has been calibrated using high-temperature fixed points. A three-parameter fit has
been applied and the resultant scale compared to an ITS-90 realization. 相似文献
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Laboratoire national de métrologie et d’essais has recently constructed a new device to realize the indium fixed point adiabatically.
In parallel, a numerical heat transfer model has been developed as an aid to understanding its thermal behavior. This transient
axially symmetric two-dimensional (2D) model simulates the melting process using the apparent specific heat method; the effects
of mixing and convection within the liquid phase of indium are not taken into account. The thermal parameters, the nonuniformity
of the furnace, and the thermal control of the surroundings were assessed with the aim of reducing parasitic heat exchanges.
The results of the modeling are in good agreement with the measurements and clarify the parasitic heat flux observed during
the phase transition. This article describes the model and the first results obtained. The model is a helpful tool in evaluating
future technical improvements of the enclosure used to realize the indium fixed point. 相似文献
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B. Khlevnoy M. Sakharov S. Ogarev V. Sapritsky Y. Yamada K. Anhalt 《International Journal of Thermophysics》2008,29(1):271-284
A large-area furnace BB3500YY was designed and built at the VNIIOFI as a furnace for high-temperature metal (carbide)–carbon
(M(C)–C) eutectic fixed points and was then investigated at the NMIJ. The dependence of the temperature uniformity of the
furnace on various heater and cell holder arrangements was investigated. After making some improvements, the temperature of
the central part of the furnace was uniform to within 2K over a length of 40 mm—the length of the fixed-point cell—at a temperature
of 2,500°C. With this furnace, the melting plateaux of Re–C and TiC–C were shown to be better than those observed in other
furnaces. For instance, a Re–C cell showed melting plateaux with a 0.1K melting range and a duration of about 40 min. Furthermore,
to verify the capability of the furnace to fill cells, one Re–C and one TiC–C cell were made using the BB3500YY. The cells
were then compared to a Re–C cell made in a Nagano furnace and a TiC–C cell filled in a BB3200pg furnace. The agreement in
plateau shapes demonstrates the capability of the BB3500YY furnace to also function as a filling furnace.
B. Khlevnoy and K. Anhalt are guest scientists at NMIJ at the time of investigation. 相似文献
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根据国际温度咨询委员会辐射测温工作组(CCT-WG5)对世界各国计量机构开展Co-C共晶点研制工作的相关要求,设计并搭建了Co-C共晶点灌注系统,采用直接共晶法成功灌注了满足复现实验要求的Co-C共晶点坩埚。针对直接共晶灌注法效率低、坩埚破裂风险大的缺陷,提出了对灌注方法的改进方案,并依据该方案成功灌注了2个Co-C共晶点坩埚。对灌注的Co-C-2#共晶点进行了复现试验,结果显示:拐点温度的不确定度为5.3 mK,满足小于10 mK的CCT要求;短期重复性为9.6 mK,满足小于20 mK的CCT要求。 相似文献
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随着环境保护的需要,具有较低Pb含量或不含Pb元素的多元低熔点合金越来越受到工业界的重视和青睐,但是该类合金的组织结构形态、相组成和基本的物理化学数据比较缺乏,不利于其工业化应用。鉴于此,文章对两种具有较低Pb含量的Sn_(16)Bi_(52)Pb_(32)(质量分数)合金和In_(21)Sn_(12)Bi_(49)Pb_(18)(质量分数)合金进行了凝固组织、相组成以及物化性能方面的研究。扫描电镜(SEM)、差示扫描量热法(DSC)、X射线衍射(XRD)等分析测试结果表明:Sn_(16)-Bi_(52)Pb_(32)合金由Bi-(Pb)固溶体相、Sn-(Bi,Pb)固溶体相以及Pb_7Bi_3化合物相组成,具有准规则共晶凝固组织结构。而In21Sn12Bi49Pb18合金由InBi化合物相、PbBi化合物相以及Sn-(Bi,In)固溶体相组成,具有复杂规则的共晶组织形貌。 相似文献
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在900-1150℃氧化的NiAl-28Cr-5.94Mo-0.05Hf-0.01Ho定向共晶合金,在其表面生成了连续的Al_2O_3氧化膜,具有良好的抗氧化性能。定向凝固工艺使合金的组织细化并提高了Cr(Mo)相中Al元素的含量,以及加入微量稀土元素Ho,都有利于生成Al_2O_3氧化膜。在NiAl-28Cr 5.94Mo-0.05Hf-0.01Ho定向共晶合金的氧化过程中表面氧化膜发生相变θ-Al_2O_3→α-Al_2O_3,导致其1000℃氧化质量增加出现反常。 相似文献
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热处理对铸造AlSiCuMg合金硅相形貌及力学性能的影响 总被引:4,自引:0,他引:4
通过对共晶硅相立体形貌的观察和定量金相学参数的测定,发现固溶处理过程中共晶硅相形貌的变化及其对合金力学性能的影响可划分为三个阶段:固溶初期硅相的熔断和钝化,使合金的塑性得到显著的提高;固溶中期以粒化为主,同时由于合金元素的充分固溶引起时效强化,合金的力学性能达到了峰值;固溶后期,硅相的粗化符合LSW粗化模型,硅相形貌呈现棱角小面特性,合金性能降低。同时,人工时效显微组织的TEM观察发现,合金峰时效时有过剩的硅质点析出,而且随着时效时间的延长,硅质点的长大很快,加速了合金的过时效。 相似文献
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The Cr3C2–C (1,826°C) peritectic point was investigated for its performance as a high-temperature fixed point. Dependence on the impurity
content was observed, although it was less severe for the higher of the two equilibrium temperatures obtained with the same
cell, the Cr3C2–C peritectic point, than for the lower, the Cr7C3–Cr3C2 eutectic point. Thermal history had an effect on the melting plateau duration, but not on the point-of-inflection temperature
nor on the melting range. The melting rate had no apparent effect. The repeatability evaluated as the standard deviation of
the repeated melting plateaux within a day was 20 mK for the Cr3C2–C peritectic point, while for the Cr7C3–Cr3C2 eutectic point, this was 210 mK. For both the Cr3C2–C peritectic and the Cr7C3–Cr3C2 eutectic, the freezing plateaux often showed deep supercools, which made them unsuitable for use. The observed good repeatability
shows the peritectic-point performance to be comparable to the best MC-eutectic high-temperature fixed points investigated
so far. The insensitivity to thermal history constitutes an important and practical advantage. The low price of chromium is
a clear benefit as compared to Pt–C (1,738°C) or Ru–C (1,953°C) eutectic points, the M–C eutectic points in this temperature
range. 相似文献