排序方式: 共有273条查询结果,搜索用时 15 毫秒
21.
22.
23.
为研制出耐辐照的新型单相陶瓷燃料,采用溶胶-凝胶法,通过复合溶胶配制、分散胶凝、洗涤、干燥煅烧与烧结过程,开展了UO2-(Zr0.8Ca0.2)O1.8燃料微球制备工艺研究,制备出铀摩尔分数含量分别为30mol%、50mol%、70mol%的UO2-(Zr0.8Ca0.2)O1.8燃料微球样品。在对工艺过程进行分析的基础上,通过实验确定了工艺参数。采用X射线衍射(XRD)对3种燃料微球样品进行分析,分析结果表明:铀摩尔分数含量分别为30mol%、50mol%、70mol%的UO2-(Zr0.8Ca0.2)O1.8燃料微球样品均为面心立方(FCC)固溶体结构。 相似文献
24.
25.
为保障核级海绵Zr的质量,应用电感耦合等离子体质谱法(ICP-MS)测定海绵Zr中痕量U。样品经HNO3-HF快速溶解后,从同位素质量数的选择、内标同位素选择、基体的影响等方面进行分析。结果表明,以232Th作为内标,可有效校正基体效应及仪器漂移引起的干扰;在样品中加入浓度分别为0.20、1.00、1.50 μg/g的U标准储备溶液,其加标回收率均在94%~99%之间,相对标准偏差最大为5.1%,合成相对标准不确定度为5.9%,方法的检出限为0.001 μg/g。采用该方法对实际样品U含量进行测定,测定结果满足核级海绵Zr对U含量的控制要求。 相似文献
26.
??The tensile creep of HT9 steel was measured at 700 and 800?? with different stress levels. Stress exponent was fitted by power law relation. Rupture time vs. minimum creep rate of HT9 steel was fitted by M- G relationship and modified M- G relationship. The fracture morphology after creeping and the creep mechanism and damage mechanism were analyzed by scanning electron microscopy, transmission electron microscopy and X- ray diffraction. The results showed that the minimum creep rate and creep rupture time of HT9 steel obeyed a linear relationship with the stress in double logarithmic coordinates, which could be described by M- G and modified M- G relationship. The stress exponent increased with the temperature. The dislocations bypassed the second phase particles during the creep process according to the Orowan mechanism. The fracture had a distinct dimple structure, and some of the second phase particles coarsened. The oxidation of HT9 steel was obvious during the creep at 800??. The main precipitates were M23C6 during the creep, which showed different forms, with significant differences in the size of the precipitated phases. The damage mechanism of HT9 steel included external cross- sectional area loss, material microstructure degradation, environmental damage, etc. There may also be internal sectional area loss. 相似文献
28.
《核动力工程》2015,(3):167-171
采用现有RDL-50型拉伸蠕变试验机,改装部分试验装置后研究Ag In Cd合金加Sn前后在300~400℃温度及12~30 MPa应力范围内的压缩蠕变行为。根据试验结果详细分析稳态速率与温度、应力的关系,计算应力指数n和蠕变激活能Qa;并根据透射电子显微镜结果探讨合金的压缩蠕变机制。结果表明:随温度和应力水平的升高,合金的稳态蠕变速率增加。加Sn后,Ag In Cd对应力敏感性更大,且在任一应力下激活能更高,其抗蠕变性能较好。根据计算,300、350、400℃条件下,加Sn与不加Sn合金的蠕变应力指数n分别为9.41、8.07、9.48和3.31、4.10、5.77;12、18、24 MPa条件下,加Sn与不加Sn合金的蠕变激活能Qa分别为147.9、126.9、149.9 k J/mol和68.1、103.7、131.6 k J/mol。微观形貌以层错为主,300℃的主要蠕变机制为孪生,400℃的主要蠕变机制为位错攀移生成位错墙。 相似文献
29.
目前有关FeCrAl-ODS钢在高温水蒸汽下的氧化过程中氧化膜结构的演变少有分析研究.以FeCrAl-ODS合金为研究对象,采用XRD、SEM、EPMA、EDS等分析手段,在700~1100℃条件下开展了高温水蒸气氧化试验,从氧化动力学和氧化层结构形貌、物相、成分等方面研究了其高温水蒸气氧化行为.研究结果表明:在700~1100℃,FeCrAl-ODS合金高温水蒸气氧化动力学满足抛物线增重规律,抛物线速率常数Kp随温度增加而增大.高温水蒸气氧化96 h后,700℃时FeCrAl-ODS合金表面氧化层以Fe2O3为主;900℃时FeCrAl-ODS合金表面氧化层的外层以Fe2O3为主,内层以A12O3为主,氧化层比较疏松,不能很好地对基体起到保护作用;1100℃氧化过程中,在不同氧化时间段氧化层均为单层致密的Al2O3氧化层结构. 相似文献
30.