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The results showed that chemisorption of Hg atoms could facilitate dislocation emission and motion.

结果表明:加载裂纹吸附Hg原子后能促进位错的发射、增殖和运动;当吸附促进位错发射和运动达到临界状态时,脆性微裂纹就在原裂纹顶端或在无位错区中形核并解理扩展。

The results showed that chemisorption of liquid metal atoms could facilitate dislocation emission ,multiplication and motioll.

结果表明:液体金属吸附后能促进位错的发射、增殖和运动;当吸附促进位错发射和运动达到临界状态时,脆性微裂纹就在原裂纹顶端或在无位错区中形核并解理扩展。

In this study, for the complicated distribution of dose rate in time and space, considering the repair of the sub-death cells, the radionuclide decay law and exponential proliferation of clonogenic cells, the dose-response relationship is built based on the known linear-quadratic model, and the concept of tumor control probability is introduced into the therapy method. Furthermore, the concepts about "curable stage" and "critical time point" and the methods calculating the amount of radionuclide injected into tumor in clinical are proposed.

本课题针对这一方法中靶区复杂的剂量率时-空分布特点,以公认的"线性-二次模型"理论为基础,同时考虑亚致死性细胞修复、核素衰变规律和克隆原性细胞指数增殖,建立了适合这一治疗方法的具有时-空分布特点的剂量效应关系,并进一步将肿瘤控制概率的概念引入这一方法中,提出了"治愈期"及"临界时间点"的概念以及由此指导临床确定药物注射剂量的方法。

The results are as follows: 1 mean length and weight tend to increase while dominant length and weight groups are noted to be increasing from Oct. 2004 to Sep. 2007; 2 by using length-weight formula, calculated weight value at the same length is higher for track-data than that for background-data; 3 growth parameters of L∞, W∞ and K respectively increase from 140.5 mm, 36.5 g and 0.28 a-1 to 186.0 mm, 118.5 g and 0.36 a-1 after artificial reef deployment; 4 appreciable increases are noted in body length and weight growth rate after artificial reef deployment, and inflexion age of weight growth increases from 2.55 to 2.58 years after artificial reef deployment; 5 there is an increase in critical biomass age from 3.21 to 3.77 years after artificial reef deployment; 6 there is a decrease in total instantaneous population mortality from 1.065 to 0.75 per year after artificial reef deployment; and 7 the overall population biomass of small yellow croaker stands at 131.5 tons.

结果表明:投礁后小黄鱼的平均体长和体重均呈上升趋势,优势体长组和体重组均向高值移动;同等体长情况下由投礁后体长体重关系式估算的体重比用投礁前的体长体重关系式估算的值大;投礁后小黄鱼个体生长方程的参数 L∞、W∞、K 值分别从投礁前的140.5 mm、36.5 g和0.28 a-1增加到186.0 mm、118.5 g和0.36 a-1;投礁后体长与体重生长速度与投礁前相比有所增大,且体重生长的拐点年龄从投礁前2.55 a提高到2007年的2.58 a;小黄鱼种群生物量增长的临界年龄从投礁前的3.21 a提高到3.77 a;小黄鱼种群的总瞬时死亡率从投礁前的1.065 a-1减小到0.75 a-1;鱼礁区小黄鱼资源量约

The CHF for upflow are regualarlygreater than those for downflow, but it becomes to reverse in the range of low critical quality.

上升流CHF试验值大于下降流,但在小临界含汽量区,下降流试验值开始等于和大于上升流试验值。

The grating spectrometer has several advantages over existing commercial products for being able to measure semi-continuous spectrum in critical hydrocarbon peak region and better signal baseline stability critical for accurate spectroscopy.

与目前的商业产品相比,该光栅光谱仪具有几个优点:能够测定临界油气峰区的半连续光谱,信号基线稳定性更好,后者对光谱的准确性非常重要。

Due to the physical properties exhibit extremely rapid variations with the change of temperature near the pseudocritical point, the heat transfer performance of supercritical fluids are very different from that of conventional refrigerants.

二氧化碳跨临界循环放热过程处于超临界区,由于在准临界点附近CO2 的热物理参数变化非常剧烈,超临界区流体的换热有别于传统制冷剂,气体冷却器的换热优劣对系统性能影响较大。

Observation of transmission electron microscope reveals that the f'me structure of CGHAZ and IRCGHAZ of both in- service welding and routine is ferrite laths and the second phase particles that distribute on or between ferrite laths.

透射电镜下,在役焊接和常规焊接的粗晶区与临界粗晶区的主要形貌都是铁素体板条和分布在板条之间或板条基体上的岛状物,铁素体板条的亚结构都是高密度位错。

Based on exploding dynamics theory, the scope of smash area, crush area and crack area, which is shaped under the action of a blast wave and stress wave resulting from the explosion of cartridge bag, is studied respectively.

基于爆炸动力学理论,得出了药包爆炸裂隙区半径的计算值与药卷临界埋藏深度基本吻合的结论,从而证明了&三区&理论计算式的正确性,为特定条件下爆破工程控制参数的设计提供了理论依据。

Lacking of impersonal observation information of triggering area of debris flow, this essay brings forward to cell automaton model to study on it based on sand pile model.

由于泥石流产流区的观测数据的缺乏,本文首次提出基于沙雄模型来建立改进的二维沙堆自动机模型,来研究泥石流产流区系统的自组织临界性。

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