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71.
装备环境适应性的定量化表征技术探讨 总被引:2,自引:2,他引:0
环境适应性的定量化表征技术对装备环境适应性的论证、考核、评价具有十分重要的意义,由于定量表征技术的复杂性,至今没有形成统一的方法。依据环境适应性的定义、内涵,将环境适应性定量表示为环境适应度,定义了环境适应度的概念,说明了环境适应度各计算参数的含义,并以算例的方式对环境适应度的计算进行了说明。 相似文献
72.
Satoru Isoda 《环境科学学报(英文版)》2013,(S1):S172-S179
Power conversion efficiency of p-i-n type microcrystalline silicon (c-Si:H) solar cells has been analyzed in terms of sequential processes of photo-induced electron transfer. The effect of the excitonic state on the charged carrier generation has been studied compared to a conventional scheme in which only charged carriers are taken into account for the operation of the solar cells. A numerical model has been developed to calculate current-voltage characteristics of solar cells on the basis of two types of charged carrier generation processes (exciton process and charged carrier process). The light trapping effect due to a textured back surface reflector (BSR) was embedded in the numerical model by using the effective medium theory in combination with the matrix method in the field of the electromagnetic theory of light. As an application of this modeling, it was found that the reported data of the power conversion efficiency were not explained by the conventional charged carrier process model and that the combined model of the charged carrier process with the exciton process well explains the performance of the p-i-n type c-Si:H solar cells. In this way, the typical power conversion efficiencies were estimated to be 10.5% for the device (i-layer thickness: 1.8 m) with the BSR (period: 600 nm; height: 250 nm) and 8.6% for the device with the flat reflector under the condition that the fractions of the exciton process and charged carrier process were 60% and 40%, respectively. 相似文献
73.
Power conversion efficiency of p-i-n type macrocrystalline silicon (µc-Si:H) solar cells has been analyzed in terms of sequential processes of photo-induced electron transfer. The effect of the excitonic state on the charged carrier generation has been studied compared to a conventional scheme in which only charged carriers are taken into account for the operation of the solar cells. A numerical model has been developed to calculate current-voltage characteristics of solar cells on the basis of two types of charged carrier generation processes (exciton process and charged carrier process). The light trapping effect due to a textured back surface reflector (BSR) was embedded in the numerical model by using the effective medium theory in combination with the matrix method in the field of the electromagnetic theory of light. As an application of this modeling, it was found that the reported data of the power conversion efficiency were not explained by the conventional charged carrier process model and that the combined model of the charged carrier process with the exciton process well explains the performance of the p-i-n type μc-Si:H solar cells. In this way, the typical power conversion efficiencies were estimated to be 10.5% for the device (i-layer thickness: 1.8 μm) with the BSR (period: 600 nm; height: 250 nm) and 8.6% for the device with the flat reflector under the condition that the fractions of the exciton process and charged carrier process were 60% and 40%, respectively. 相似文献
74.
75.
为了验证在钢铁企业中人的失效过程同服役年限有某种规律性的联系,采用马尔萨斯模型对人的服役年限--工龄与伤害事故频数之间的规律性进行机理推证.在对典型钢铁企业40年间工伤事故数据库中的1 465起伤害事故进行统计分析、建立回归模型后,结论显示伤害事故频数y与受害人员的本工种工龄x存在显著指数相关关系:y=167.13e0.012x、相关系数R=0.93,证实了马尔萨斯模型应用于"工龄-伤害事故频数"指数规律的准确性.改进后的指数规律模型对实际钢铁企业安全管理工作有着重要的研究价值和指导意义,且可以在其他领域中进行探索和推广. 相似文献
76.
77.
毒物兴奋效应(hormesis)受到广泛关注。本文以秀丽线虫(Caenorhabditis elegans)的L1(自虫卵开始培养10 h)、L3阶段(36 h)和年轻成虫阶段(72 h)为起始暴露阶段,进行环境浓度(3.18E-3、3.18E-2、3.18E-1和3.18μmol·L-1)水平的72 h镍暴露试验,以体长与行为学指标为终点研究了不同生命阶段对毒物兴奋效应的影响。在所有暴露浓度下,镍对L1线虫的体长均表现出显著的刺激效应,3个较高浓度下(3.18E-2、3.18E-1和3.18μmol·L-1)的刺激效应相似,均表现为比空白多23.6%(P0.05)的水平;L3线虫的体长在低浓度受到刺激,在高浓度受到抑制,表现为毒物兴奋效应;年轻成虫在所设4个浓度下均没有显著响应。在所有暴露浓度下,镍对L1线虫的身体弯曲运动无显著效应;镍对L3线虫的身体弯曲频率表现为刺激效应,并且该刺激效应随暴露浓度增加,先增加后减小,在3.18E-2μmol·L-1表现出最大刺激效应,比空白多59.0%(P0.05);镍对年轻成虫的身体弯曲频率表现为比空白多17.7%~30.1%(P0.05)的刺激效应,该刺激效应在不同浓度下不具有显著性差异。镍对L1线虫的倒退运动表现出显著的、随暴露浓度增加而增加的刺激效应,在3.18μmol·L-1表现出最大刺激效应,比空白多187.0%(P0.05);镍对L3线虫的倒退运动在3.18μmol·L-1下表现为比空白多22.7%(P0.05)的刺激效应;镍对年轻成虫的倒退运动在较高的3个浓度下(3.18E-2、3.18E-1和3.18μmol·L-1)表现为比空白多46.7%~86.7%(P0.05)的刺激效应。研究揭示环境浓度水平的镍暴露对不同生命阶段秀丽线虫的体长与运动具有不同程度的刺激效应。 相似文献
78.
针对煤岩巷道锚杆支护锚固失效引起的冒顶问题,建立了煤岩巷道顶板锚杆树脂锚固模型,采用数值模拟的方法对不同锚固方式下树脂锚杆的波导特性进行研究,得到了不同锚固长度与树脂锚杆激振响应特性曲线。通过对比分析,研究得出无论何种锚固方式,检测结果与实际锚固长度的误差大约在1%-6%,同时可采用修正补偿的方法降低检测误差。研究结果得出:采用应力反射波法检测树脂锚杆的锚固长度是一种行之有效的无损检测方法,可实现树脂锚杆锚固长度的便携、准确检测提供技术支持。 相似文献
79.
黄河三角洲湿地土壤微生物群落结构分析 总被引:5,自引:0,他引:5
采用末端限制性片段长度多态性分析(T-RFLP)技术和16S rDNA克隆文库的方法,分析了黄河三角洲滨海湿地土壤不同深度细菌和古菌的群落结构.研究表明,随着深度的增加,细菌群落的多样性下降,而古菌群落多样性则有上升的趋势,且土壤的细菌和古菌群落结构都呈现出规律的层状分布.该土壤包括各种硫酸盐还原菌、产甲烷古菌、光合细菌等丰富的细菌和古菌资源.图5参27 相似文献
80.
Methodologies of API 579 have been widely accepted as the de-facto standard guideline for fitness for service assessment on crack-like flaws in pressure equipment. For different purposes and needs, the evaluation is divided into three levels, from critical length estimation in level 1, use of the failure analysis diagram (FAD) in level 2, to performing finite element stress analysis in level 3, that is from simplified to accurate. It is generally considered safe as long as the crack is smaller than the critical crack, but not all of them are actually the case. Therefore, it is very important to study the physical meaning behind the critical crack and understand the conservativeness of it.In this study, numerous examples of critical cracks determined according to API 579 Level 1 were put into Level 2 analysis for comparison. Each case is mapped onto the FAD of level 2 analysis to see its position and distance from the borderline between safe and danger zones. A huge amount of examples covering the majority of possible scenarios, including the geometry, thickness, inner diameter, pressure and half-length of the flaw, depth of the crack, crack tip and crack bottom, as a whole, there are 960 cases to be analyzed.Results show that cracks on the circumferential direction of the cylindrical and spherical vessels are distributed tightly in a small area far from the borderline on the FAD diagram. In these cases, the vessel is actually not as dangerous as the critical crack implies, since most of the points lie quite far from the danger zone. As for the longitudinal cracks of a cylindrical vessel, the results are scattered around, and three data points are located outside the allowable zone. The peculiar results are partly due to a discrepancy of interpolating procedure as the influence coefficient is being computed. Through this study, it is also found that the cumbersome process of estimating the critical crack length can be greatly simplified for longitudinal cracks in a cylindrical vessel. 相似文献