47 resultados para Blennerhassett, Harman, 1764-1831.
em Chinese Academy of Sciences Institutional Repositories Grid Portal
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Titanium carbide particle (TiCp) reinforced Ni alloy composite coatings were synthesized by laser cladding using a cw 3 kW CO2 laser. Two kinds of coatings were present in terms of TiCp origins, i.e. undissolved and in situ reacted TiCp, respectively. The former came from the TiCp pre-coated on the sample, whereas the latter from in situ reaction between titanium and graphite in the molten pool during laser irradiation. Conventional and high-resolution transmission electron microscope observations showed the epitaxial growth of TiC, the precipitation of CrB, and the chemical reaction between Ti and B elements around phase interfaces of undissolved TiCp. The hardness, H, and elastic modulus, E, were measured by nanoindentation of the matrix near the TiCp interface. For undissolved TiCp, the loading curve revealed pop-in phenomena caused by the plastic deformation of the crack formation or debounding of TiCp from the matrix. As for in situ generated TiCp, no pop-in mark appears. On the other hand, in situ reacted TiCp led to much higher hardness and modulus than that in the case of undissolved TiCp. The coating reinforced by in situ generated TiCp displayed the highest impact wear resistance at both low and high impact conditions, as compared with coatings with undissolved TiCp and without TiCp. The impact wear resistance of the coating reinforced by undissolved TiCp increases at a low impact work but decreases at a high impact work, as compared with the single Ni alloy coating. The degree of wear for the composite coating depends primarily on the debonding removal of TiCp.
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给出半圆柱前缘舵诱导的高超声速湍流分离激波运动特性。实验气流M数为7.8单位长度Re数为3.5×10~7/m。结果表明,随着M数的增加,分离激波两边压力比的平均值加大,但对其用前缘直径无量纲的激波运动区长度和用自由流速度无量纲的激波向上(下)游运动速度的平均值影响不大。
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采用单电子模型研究了圆偏振飞秒脉冲激光作用下电子振荡导致的谐波辐射频谱的特性。研究发现随着激光强度的增加,电子在激光场中运动的相对论效应可以导致谐波辐射,并且发现谐波辐射频谱随着激光强度的增加发生了展宽和红移。电子与强激光脉冲相互作用,电子除了在激光场的作用下做横向振荡运动之外,激光脉冲的纵向有质动力对电子还有推动作用,这是产生谐波频谱红移的原因,而谐波辐射频谱展宽是由电子纵向速度的变化引起的。分析激光场中电子在不同方向的辐射频谱表明:随着谐波阶数的升高,红移在有规律地变大;在θ=3π/4方向上电子频谱的
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Modulated UV light is used to increase the sensitivity of the two-centre holographic recording. Inherent mechanisms of nonvolatile holographic recording in oxidized and reduced crystals are numerically analysed based on solving the two-centre material equations modilied for UV-Iight recording. Experiments verification is performed with an oxidized crystal and a reduced crystal, and the role of UV intensity on the sensitivity is presented.
Resumo:
本研究在野外调查的基础上,采用随机扩增多态DNA (RAPD)分析和形态学方法,研究了我国三种珍稀濒危兰科植物硬叶兜兰(Paphiopedilummicranthum)、麻栗坡兜兰(P. malipoense)和独花兰(Changnienia amoena)的遗传多样性与群体遗传结构,主要结果如下: 1.采用1 2个引物对分布于我国云贵地区的4个硬叶兜兰群体共161个体进行RAPD扩增和分析,得出物种水平的多态条带百分率(PPB)为71.6%,Nci的基因多样度(h)为0.217,Shannon多样性指数(1)为0.3301;4个群体的平均多样性水平为PPB=45.2%,h=0.1457,1= 0.2204:低于远交兰花的平均水平。分子方差分析(AMOVA)表明,在总遗传变异中,群体间遗传变异占20.31%.群体内占79.69%;POPGENE给出的基因分化系数 (Gst)为0.2958;遗传分化略高于远交物种的平均水平。空间自相关分析表明,所检测的两个群体中存在明显的空间结构,基因型在群体中以不同的小斑块存在。遗传距离和空间距离不存在相关关系。 2.用于麻栗坡兜兰的RAPD引物同上,但取样范围只有贵州的2个群体共10个个体。就所研究的个体柬看,麻栗坡兜兰的遗传多样性明显低于远交兰花物种的平均水平。物种水平上,多态条带百分率(PPB)为49.5%。Nei的基因多样度(h)为0. 1174, Shannon多样性指数(I)为0.1764:在群体水平上,上述三个指标的平均值则分别为12. 75%、0.0486和0.0712,均大大低于硬叶兜兰。然而,尽管作了种种努力,麻栗坡兜兰的取样个体数量仍很少,因此所得结果可能会有误差。 3.用16个引物对分布于河南、湖北、湖南、江西4个省11个独花兰群体共216个体进行了RA PD扩增和分析,独花兰在物种水平PPB=80. 7%,h=0.197.1=0. 3116;在群体水平,上述三个指标的平均值则分别为40. 9%、0.1247和0. 1902,均低于远交兰花的平均水平。AMOVA分析表明,11个独花兰群体间的遗传变异占43.48%,群体内的占56.52%:在神农架和新宁地区内部,群体间的遗传变异分别占13.68%和49.3g%(AMOVA)。POPGENE给出的11个群体的基因分化系数(Gst)为0.3580.神农架和新宁地区内的Gst,值分别为0.1194和0.2597。可见,群体间的遗传分化明显高于远交物种的平均水平。空间自相关分析表明,独花兰的遗传变异在群体内不存在明显的空间结构。群体之间的遗传距离和空间距离不存在相关关系。 4.对独花兰7个群体形态性状的分析发现,12个形态性状在群体内均有较高的变异性,cv值变动于0.022-0.30O。庐山群体(LS)在所有性状上的平均值均为最高。营养性状和花部性状的变异性基本一致。除花葶长和花距直径与某些花部性状之间没有显著的相关关系外,各性状之间均有显著的相关性。对XN4群体的统计没有发现假磷茎数目与其他性状之间存在显著相关性。 根据以上对硬叶兜兰、麻粟坡兜兰和独花兰遗传多样性和群体遗传结构韵研究,结合其他方面的资料;对三种兰花的濒危机制进行了初步的分析。首先,人为采挖和破坏是导致这些兰花物种濒危的直接原因,尤其是麻栗坡兜兰。其次, 适宜兰花生存的生境正在只益萎缩、退化和片段化。这两方面因素的共同作用导致上述兰花群体的数目和规模日益下降,由此引发的遗传多样性降低和遗传结构的改变进一步加剧其濒危状况。对于独花兰而言,较低的繁殖能力又使其生存状态雪上加霜。针对三个物种不同的繁殖特性和遗传学状况,提出如下保护措施。(1)硬叶兜兰由于繁殖能力较强、现存个体尚多,遗传多样性损失不甚严重,因此以保护其所在的生境为基础、实施原位保护,是比较合适的保护策略。(2)麻粟坡兜兰目前受破坏程度非常严重;所剩个体很少,遗传多样性较低,已经很难进行有效的原位保护。因此;应利用迁地保护手段抢救目前尚存的个体。(3)独花兰的繁殖能力较弱,因此在保护生境和严禁采摘的基础上,可采用人工授粉等方式,提高结实率、增加繁殖效率,促使其复壮:在进行迁地保护时,则应注意不同群体间存在较大遗传变异而群体内多样性较低这一现实。
Resumo:
缘毛鸟足兰是在具有近20,000种的兰科中迄今为止报导过的雄性不育类型与两性类型共存的唯一例子。深入研究缘毛鸟足兰中雄性不育类型和两性类型共存的现象有助于丰富对兰科生殖系统演化的理解。本文通过生殖生态学研究,得出如下结论。 1. 证实了缘毛鸟足兰中只存在两性类型和雄性不育类型。雄性不育类型始终与两性类型出现在同一居群中,没有单独的雄性不育类型居群。雄性不育类型在调查的16个居群中,在6个居群中出现,约占38%。两种类型共存的居群中雄性不育类型的比率变化很大,从1%到78%,但只在一个居群中超过50%。 2. 通过交配系统实验发现,共存于同一居群中的短距雌性类型和两性类型都存在无融合生殖方式,种子的形成无需授粉。本文第一次报导了在兰科中存在同一无融合生殖种中两性类型和雄性不育类型共存于同一居群的现象。 3. 缘毛鸟足兰花部结构变异很大,结合性别和花的形态特征,将缘毛鸟足兰划分为6类生物型,分别是小花两性、大花两性、短距两性、短距雌性、长距雌性和三瓣雌性。 4. 在同一居群中短距雌性型和小花两性型在生殖和生态上存在差异:1)短距雌性型更能耐受不利的环境条件;2) 短距雌性型的花期早于两性型;3) 短距雌性型平均单株结实较多,但从平均单株产生的胚总数上看,两种类型之间却没有显著差异;4)在资源分配策略上,两种类型各有利弊。
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本发明涉及新颖的化学结构式(I)的炭球菌素。本发明还涉及该化合物的制备方法,以该化合物为活性成分的药物组合物,以及本发明化合物和药用组合物在制备治疗和预防艾滋病的药物中的应用。
Resumo:
以滇池2个典型的严重富营养化湖湾———马村湾和海东湾为研究区域,研究分析了2个湖湾沉积物及水体悬浮物中4种磷的赋存形态:松散吸附态磷(NH4Cl-P)、氧化还原敏感态磷(BD-P)、金属结合态磷(NaOH-P)和钙结合态磷(HCl-P)以及有机质含量及总磷(TP)含量.结果表明:沉积物随着风浪搅动悬浮进入水体后,4种形态的磷含量及其所占总磷的比例均发生了较大变化,NH4Cl-P的含量升高,是由于快速的吸附作用所致;NaOH-P在4种磷形态中的比例下降,含量上升,表明沉积物再悬浮进入水体后磷的活化特性加大,
Resumo:
In this study, the levels of 25 semi-volatile organic compounds (SVOCs) were measured in samples of water, suspended particulate matter (SPM) and sediment from two urban lakes in Wuhan, China. The total concentrations of 25 SVOCs varied from 529.4 to 2168.9 ng/L, 120.7 to 22543.7 ng/g dry weight and 1577.3 to 61579.6 ng/g dry wt. in water, SPM and sediment, respectively. The concentration of SVOCs in SPM was 9-10 times higher than that in water, and the concentration of SVOCs in sediment 1.5-2 times higher than that in SPM. The level of total SVOC25 in the samples from Moshuihu Lake was higher than that in Yuehu Lake. Among the 25 SVOCs, phthalate compounds were on the highest level in all observed samples ranging between 441.9-1831.2 ng/L, 116.3-17566.8 ng/g, dry wt. and 6432.8-48177.6 ng/g dry wt. in water, SPM and sediment, respectively. Bis(2-ethylhexyl)phthalate, the predominant component of the analyzed pollutants, was in the range from 246.7 to 537.5 ng/l, 51.2 to 15540.0 ng/g dry wt. and 468.2 to 45010.3 ng/g dry wt. in water, SPM and sediment, respectively. The content of PAHs, dinitrotoluene and isophoton in sediment was higher than that in water and SPM at most of the locations. The possible sources of the pollutants and their inter-relation with human activities were discussed.
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The transgenic carp were produced by micro-injection of CAgcGHc into the fertilized eggs. Observation of the thymus development between the transgenics and non-transgenic controls was carried out. The thymus of one-year-old transgenics F1 showed a great increase in both size and weight. The unilateral thymus of the transgenics weighed from 190 to 295 mg with average 218.6 mg, whereas the unilateral thymus of the controls weighed 20-81 mg with average 42.5 mg; i.e. the thymus weight in the transgenics was 5.14 fold over that in the controls. The index of thymus/body weight in the transgenics was 2.97 fold over the controls. Light microscopy observation indicated that the thymus of the transgenics; well developed with the thickened outer region and compactly arranged thymocytes, while the thymus in the controls were degenerating with the thinned outer region, scattered thymocytes and groups of fatty cells. Further analysis with the electron microscopy revealed that pro-liferous cells in the transgenics; were mainly small lymphocytes and no pathological changes were found. The results confirmed that the "All-fish" GH-transgene promotes thymus development and thymocyte proliferation, and retards thymus degeneration. The study has laid a foundation for further analysis of the immunobiological function in GH-transgenic carp.
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Mode characteristics of three-dimensional (3-D) microsquare resonators are investigated by finite-difference time-domain (FDTD) simulation for the transverse electric (TE)-like and the transverse magnetic (TM)-like modes. For a pillar microsquare with a side length of 2 pin in air, we have Q-factors about 5 X. 103 for TM-like modes at the wavelength of 1550 run, which are one order larger than those of TE-like modes, as vertical refractive index distribution is 3.17/3.4/3.17 and the cororresponding center layer thickness is 0.2 mu m. The mode field patterns show that TM-like modes have much weaker vertical radiation coupling loss than TE-like modes. TM-like modes can have high Q-factors in a microsquare with weak vertical field confinement.