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排序方式: 共有4067条查询结果,搜索用时 15 毫秒
31.
This research deals with the service evaluation of a retired CrMoV steel rotor that has been repaired using deep groove multi‐pass submerged arc welding (SAW) and gas tungsten arc welding (GTAW). Accelerated creep tests were conducted at several elevated temperatures and extrapolated to the service temperatures. The coalescence of carbides and cavity growth during creep were evaluated. For the CrMoV‐GTAW samples, it was found that the creep life depended on the location of the crossweld in the welded specimen. The service lives of the weldments were extrapolated. 相似文献
32.
33.
95W-Ni-Fe 合金工艺缺陷的 SAM 和 XPS 分析 总被引:3,自引:0,他引:3
齐芸馨 《兵器材料科学与工程》1997,20(5):36-40
藉助扫描俄歇探针、X射线光电子谱等分析了95W-Ni-Fe合金碳污染和氧化的本质。发现,碳污染试样中碳的化学状态主要为石墨,少量为铁或镍的有机化合物,这些物质的界面富集使材料脆化。钨合金氧化后,氧大量富集于钨/粘结相界面,使沿着该界面的断裂更容易发生。 相似文献
34.
Anna-Lena Larsson Jos Solis Gunnar A. Niklasson 《Solar Energy Materials & Solar Cells》2007,91(13):1248-1252
Thin films of amorphous and polycrystalline tungsten oxide were produced by reactive dc magnetron sputtering and nanocrystalline films were deposited by advanced gas evaporation. The films were submitted to electrochemical intercalation of Li ions before infrared reflectance measurements were carried out. For crystalline films, the reflectance in the wavelength region 10–30 μm increases upon intercalation, indicating an increasing free-electron contribution. On the other hand, all the films display an increased absorption at wavelengths less than 10 μm when intercalated. The thermal emittance could be varied from about 0.5 to 0.7–0.75 by intercalation in films with thicknesses in excess of 1 μm. Both absorption and interference contribute to the emittance contrast. 相似文献
35.
本文用热电偶误差计算的通用方法(极限误差表达法)分析了构成快速钨铼热电偶测温误差的因素,从量的角度探讨了各因素对总的误差的影响,对如何认识快速钨铼热电偶的测温精度,提出了可供参考的观点。 相似文献
36.
V. Didoukh A. Seifter G. Pottlacher H. Jäger 《International Journal of Thermophysics》1998,19(3):969-981
In earlier experiments we have studied pure elements with a fast pulse heating technique to obtain thermophysical properties of the liquid state. We report here results for thermophysical properties such as specific heat and dependences among enthalpy, electrical resistivity, and temperature, for four W–Re alloys (3.95, 21.03, 23.84, and 30.82 at % of Re) in a wide temperature range covering solid and liquid states. Thermal conductivity is calculated using the Wiedemann–Franz law for the liquid alloy, as.well as data for thermal diffusivity for the beginning of the liquid phase. Additionally, data for the entire temperature range studied have been analyzed in comparison with those of the constituent elements, tungsten and rhenium, since both metals have been studied previously with the same experimental technique. Such information is of interest in the field of metallurgy since W–Re alloys of low Re content in the region of mutual component solubility in the solid state are widely used as thermocouple materials for the purposes of high-temperature thermometry. 相似文献
37.
A new discharge system for resistive self-heating has been constructed for the measurement of accurate thermophysical properties. A constant-current pulse is used to heat metals over a time interval of 50 to 100 s, reaching temperatures up to the boiling point. New techniques have been developed to obtain sound speeds in the pulse-heated sample, emissivities, and vapor pressure. A new pyrometer allows the extension of the measured temperature range down to the melting point of copper. 相似文献
38.
39.
The knowledge of the thermal accommodation coefficient for gases on well-controlled surfaces as a function of temperature is imperative to understanding the mechanism of interphase heat transfer on the microscopic level. With this goal in view, a heat transfer column instrument is designed, fabricated, assembled, and tested for the specific case a argon—tungsten system. With 99.9999%, pure argon, six sets of data are taken in the rarefied gas region in the maximum temperature range of 500–1500 K. Four sets of these measurements are in the temperature-jump region and are analyzed by the constant-power method to compute the thermal accommodation coefficient of argon on a controlled tungsten surface. The other two sets are taken under free-molecular flow conditions and are interpreted in accordance with the man-free-path kinetic theory for the low-pressure regime. These data are compared and discussed in the context of reported data in the literature and interpreted in the light of the surface condition and finish of the tungsten wire.Nomenclature
A
area of the solid surface
-
C
j
constants in Eq. (3); j=0, 1, 2, 3, and 4
-
E
i
incident energy flux
-
E
r
reflected energy flux
-
E
s
reflected energy flux when the interaction between the gas and the solid atoms is complete
-
g
temperature-jump distance
-
L
half-length of the metal wire
-
M
molecular weight of the gas
-
P
gas pressure
-
Q
H
total thermal energy conducted by the gas per unit time from the hot surface
- QKT
total thermal energy conducted by the gas per unit time if the striking gas molecules were to attain thermal equilibrium with the hot surface
-
R
molar gas constant
-
r
radial coordinate
-
r
f
radius of the hot wire
-
S
sticking coefficient
- So
initial sticking coefficient
-
T
temperature
-
T
e
linearly extrapolated gas temperature on the hot-wire surface
-
T
g
temperature of the impinging gas molecules
-
T
H
temperature of the hot surface
-
T
i
temperature of the incident gas stream
-
T
r
temperature of the gas molecules receding after collision with the solid surface
-
T
s
temperature of the solid surface
Greek Symbols
thermal accommodation coefficient for the gas—solid surface
-
resistivity of the metal wire
-
gas coverage on the solid surface
For an explanation of symbols, see Nomenclature. 相似文献
40.
高纯钨中杂质元素的化学光谱法测定 总被引:2,自引:0,他引:2
采用以一定比例的HNO3和HCl为介质,使钨沉淀成钨酸与杂质分离,然后用碳粉吸附杂质再进行光谱测定的方法,对高纯钨(包括金属钨、三氧化钨、钨酸、钨酸铵)中15个杂质元素Fe、Ni、Cu、Mn、Al、V、Cr、Co、Ca、Ms、Pb、Sn、Bi、Cd、Be进行了测定,取得了理想的结果,测定下限可达(0.1~0.5)×10(-6)。 相似文献