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The phase relationship between 3C- and 6H-SiC is investigated in the pressure range 2.5–6.5 GPa and the temperature range 400°–2500°C, by analyzing recovered samples, using X-ray diffractometry and Raman-scattering techniques. The phase transition from 3C- to 6H-SiC occurs at 2200°C and 2.5 GPa. In the pressure range >4.5 GPa, 6H-SiC transforms to 3C-SiC at 2500°C, via an intermediate state, as indicated by broadening peaks in the X-ray diffraction profile. Thermodynamically, 3C-SiC appears to be the low-temperature stable form, and the temperature of transition to 6H-SiC, which is stable at high temperature, appears to increase with pressure. 相似文献
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Sea-Fue Wang Chiang-Chuang Chung Chai-Hui Wang Jinn P. Chu 《Journal of the American Ceramic Society》2002,85(6):1619-1621
Preparation of dense and phase-pure Ba2 Ti9 O20 is generally difficult using solid-state reaction, since there are several thermodynamically stable compounds in the vicinity of the desired composition and a curvature of Ba2 Ti9 O20 equilibrium phase boundary in the BaO–TiO2 system at high temperatures. In this study, the effects of B2 O3 on the densification, microstructural evolution, and phase stability of Ba2 Ti9 O20 were investigated. It was found that the densification of Ba2 Ti9 O20 sintered with B2 O3 was promoted by the transient liquid phase formed at 840°C. At sintering temperatures higher than 1100°C, the solid-state sintering became dominant because of the evaporation of B2 O3 . With the addition of 5 wt% B2 O3 , the ceramic yielded a pure Ba2 Ti9 O20 phase at sintering temperatures as low as 900°C, without any solid solution additive such as SnO2 or ZrO2 . The facilities of B2 O3 addition to the stability of Ba2 Ti9 O20 are apparently due to the eutectic liquid phase which accelerates the migration of reactant species. 相似文献
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压力容器设计中对高温结构的考虑 总被引:1,自引:0,他引:1
一些设计人员在设计高温压力容器时,通常采用常规的设计方法,并未对高温结构问题予以特殊的关注。在实际设计中,应对其材料、局部结构、压力容器整体的膨胀量等加以注意。文中对一些高温设备结构设计中的几个问题进行探讨,可供压力容器设计人员参考。 相似文献
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Joong-Gon Kho Kyo-Tae Moon Jong-Hee Kim Dong-Pyo Kim 《Journal of the American Ceramic Society》2000,83(11):2681-2683
Boron-rich boron nitride (BN) films have been prepared on Si and SiO2 /Si substrates by the vacuum pyrolysis of spin-coated polyborazine films. Physical properties of the prepared films such as film strength, thermal conductivity, and dielectrics were determined. The BN films vacuum-pyrolyzed at 900°C showed residual N–H bonds with a 0.75 N/B ratio, interdiffusion phenomena, and preferred orientation at the interfacial zone. Hardness and the elastic modulus of the film increased to 1.6 GPa and 50 GPa by nanoindentation loading. It had a thermal conductivity of 134 W/(m·K) at 296.5 K, and a dielectric constant in the range of 5–7, with tan ∂ between 0.01 and 0.47, depending on the film thickness. 相似文献
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中东地区伊拉克新投产的H油田地表水资源有限,急需研究注海水工程配套技术,因此海水对注水管柱的腐蚀速率显得至关重要。以H油田注水系统环节涉及的6种挂片(碳合金、35Cr Mo、N80、L80、80ss、90s)为研究对象,以高温高压动态腐蚀仪为技术手段,研究了高温高压及离子浓度变化条件下的动态腐蚀速率情况,研究表明,碳合金、35Cr MO和N80属于尚耐蚀型材料,L80、80ss和90s属于完全耐蚀型材料,从技术经济较大考虑推荐L80和80ss管材。Cl~-、SO_4~(2-)和HCO_3~-浓度对腐蚀速率影响主次顺序为:Cl-HCO_3~-SO_4~(2-)。 相似文献
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The cation solubility limits of the n = 2 and n = 3 superconducting phases in the Bi2 (Sr x Ca1 − x ) n +1 Cu n O y system were established along tie lines with compatible phases via electron probe microanalysis on bi- (or poly-) phasic samples prepared at 860°C. Pb additions (15 mol% of the Bi content) were used to facilitate formation of the n = 3 phase. In each case football-shaped volumes in composition space were established as the solubility limits which bordered on the nominal compositions 2212 or 2223 (Bi:Sr:Ca:Cu) with the long axis parallel to the Sr-Ca side of the quaternary (i.e., Sr-to-Ca intersolubility) but also extending toward Bi and Cu. This means that, for the most part, the superconducting phases are alkaline-earth deficient relative to the ideal 2212 and 2223 compositions. The Pb content in the 2223 phase is typically 10% of the Bi content. T c variations could be correlated with variations in Sr or (Sr + Bi) content and the length of the c -axis parameter. 相似文献
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选用Rheo-Stress 6000型高温高压流变仪,测定不同密度、不同温度(60℃、120℃、150℃、180℃和200℃)和压力梯度下白油全油基钻井液的流变特性。实验结果表明,无论哪种密度的油基钻井液,温度升高都使其表观粘度、剪切应力降低,压力增加都使其增大:150℃的高温下,随着压强的增加,钻井液粘度增幅越来越小,后期趋于平缓,温度和压力同时作用于钻井液流体时,温度占主导作用;在较高的压力和温度下,白油全油基钻井液体系仍有很好的塑性粘度和动切力;此配方白油全油基钻井液在高温高压条件下体系稳定,剪切稀释性好。 相似文献
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针对航空燃料高温高压条件下的等压热容测试,建立了一种新的在线测量装置和测试方法。通过冷、热油对冲混合方式,基于能量守恒原理建立了等压热容的计算公式;基于自制的燃料高温高压流动装置,增加混油和测温部件建立了等压热容测试的实验装置。通过对相关物理量测试不确定度分析,计算得到等压热容的相对扩展不确定度为±3.78%;采用纯水进行标定,验证了该方法测试等压热容的可靠性和精确性。采用航空燃料中的常用组分正十烷,实验测定了在2.1和3.0MPa压力下的等压热容数据,与采用Supertrapp软件的拟合值吻合很好,误差基本在±5%以内。 相似文献
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分析了高温高压临氢换热器硫化氢腐蚀原因,介绍了腐蚀表面现场修复方法,包括腐蚀表面加工、预热、施焊操作与安全防护、焊后热处理及检验等关键工艺。采用ER309LSi不锈钢作为堆焊层,通过合理的焊接工艺,可以减缓温高氢-硫化氢环境下的腐蚀。 相似文献
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高温高压下气体在水/地层水中的溶解度:实验装置的建立和校核 总被引:5,自引:0,他引:5
高温高压下气体在水/地层水中的溶解度实验装置的建立和校核郑大庆高军孙大平郭天民(石油大学油气藏流体高压相态及物性研究室,北京102200)关键词高温高压气体溶解度实验装置1引言近年来在我国陆上和海上地层更深处相继发现了一些储量可观的天然气藏。其中有... 相似文献
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将环氧有机硅固化剂9301以及异氰酸固化剂2102加入到增黏丙烯酸酯乳液中,成功制备出耐高温丙烯酸酯压敏胶。研究压敏胶的固化行为,探讨固化剂的种类和用量对压敏胶粘接性能及耐温性的影响。结果表明:固化剂与复合物发生了交联反应,9301和2102固化体系的适宜固化条件分别为150℃/5min和110℃/3min。随着固化剂用量增加,压敏胶的凝胶率和玻璃化转变温度提高,剥离时由内聚破坏转变为界面破坏,初黏力与剥离强度降低,耐高温性能得到改善。当9301与2102用量为2wt%时,压敏胶的剥离强度分别为11.6N/25mm与10.2N/25mm,可耐180℃高温。 相似文献
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在-40℃下,通过落锤撞击制备了不同破碎程度的DAGR125和NR11发射药,利用染料吸附量表征了发射药的破碎程度,结合密闭高压爆发器实验,分析了破碎发射药结构特征与高压燃烧特征的关系。结果表明,随着小颗粒破碎发射药的增加,动态活度变化率在燃烧初始阶段发生转折。当破碎程度较小时,初始动态活度、染料吸附量均可衡量发射药初始燃面和破碎程度;当破碎程度较大时,利用传统方法获取的初始动态活度明显小于实际值,不适合用来表征初始燃面,而染料吸附量法更为准确。初始动态活度变化规律显示,当落锤高度大于60cm时,发射药药粒的破碎程度快速增加;动态活度变化规律显示,落锤高度分别大于23.0cm和23.1cm时,DAGR125和NR11破碎发射药整体燃烧过程由增面性转变为减面性。 相似文献
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Phase Relations and Volume Changes of Hafnia under High Pressure and High Temperature 总被引:1,自引:0,他引:1
Osamu Ohtaka Hiroshi Fukui Taichi Kunisada Tomoyuki Fujisawa Kenichi Funakoshi Wataru Utsumi Tetsuo Irifune Koji Kuroda Takumi Kikegawa 《Journal of the American Ceramic Society》2001,84(6):1369-1373
Using multi-anvil high-pressure devices and synchrotron radiation, X-ray in situ observations of HfO2 under high pressure and high temperature have been performed to investigate its phase relations and compression behavior. An orthorhombic phase (orthoI) is stable from 4 to 14.5 GPa below 1250°–1400°C and transforms to a tetragonal phase, which is one of the high-temperature forms of HfO2 , above these temperatures. Another orthorhombic phase (orthoII) with a cotunnite-type structure appears above 14.5 GPa. OrthoII is stable up to 1800°C at 21 GPa. OrthoII is quenchable to ambient conditions. The orthoI-to-orthoII transition is accompanied by ∼8 vol% decrease. The bulk moduli of orthoI and orthoII at room temperature are 220 and 312 GPa, respectively. This low compressibility of orthoII indicates that it is a potential candidate for very hard materials. 相似文献