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221.
为了深入研究反应堆结构中诸如燃料棒、蒸汽发生器传热管束等的流致振动问题,利用有限体积法离散大涡模拟的流体控制方程,利用有限元方法离散结构动力学方程,并结合动网格技术建立了模拟双向流固耦合作用的三维数值模型,实现了弹性管与弹性管之间以及弹性管与湍流流场之间的交互作用。利用该模型分别研究了节径比P/D为1.2、1.6、2.0、3.0、4.0的两交错排列弹性管在横向湍流作用下的振动响应及流场特性。通过分析发现:两交错排列弹性管的运动轨迹和尾涡结构与其间距、流速密切相关;两交错管的临界节径比为2.0;P/D=3.0时双管的临界流速Upr=2.2,P/D=1.6时双管的临界流速Upr=4.0。 相似文献
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Shifeng Du Dongxiang Zhang Baohua Feng Jing-Yuan Zhang Jing-Cun Zang 《Optics Communications》2009,282(14):2960-12186
We report the generation of high-peak power multi-wavelength picosecond laser pulses using optical parametric amplification (OPA) in BBO seeded with pulses generated in a 5-mm length BaWO4 crystal by stimulated Raman scattering of 18-ps laser pulses at 532 nm. The maximum output energy of the amplified first-Stokes component at 559.7 nm was about 1.76 mJ. The corresponding maximum peak power, pulse duration and spectral line width were measured to be 117.3 MW, 15 ps and 18.0 cm−1, respectively. The multi-wavelength picosecond laser pulses were in the visible and near infrared ranges. Using this Raman-seeded OPA technique, the beam quality of the stimulated Raman scattering pulses can be improved. 相似文献
225.
Xue‐An Chen Hai‐Ping Xue Xin‐An Chang He‐Gui Zang Wei‐Qiang Xiao 《Acta Crystallographica. Section C, Structural Chemistry》2005,61(11):i109-i110
Ga(IO3)3 crystallizes in the space group P63, with the Ga atom at a site with imposed threefold symmetry. The crystal structure consists of slightly distorted GaO6 octahedra that are bridged by I atoms of IO3− groups, giving rise to a three‐dimensional polar network. The framework contains unoccupied hexagonal channels running parallel to the hexagonal [001] direction. The iodate groups have their stereochemically active non‐bonded electron pairs pointing in the same direction along [001], which creates the polarity in the structure. The I—O bond distances and O—I—O angles are normal, being in the ranges 1.783 (3)–1.847 (2) Å and 94.68 (11)–99.61 (12)°, respectively. 相似文献
226.
Jun Zhou Yong-zhi Qiu Xiao-peng Zang Chang-wang Pan Qiang Chen Jian Shen Si-cong Lin 《高分子科学》2005,23(1)
N,N-dimethyl-N-methacryloyloxyethyl-N-carboxyethyl ammonium (DMMCA) was graft-copolymerized onto the surface of segmented poly(ether urethane) (SPEU) and PE film. The carboxybetaine structure on SPEU and PE film surfaces was confirmed by ATR-FTIR, XPS and water contact angle measurements. Through the experiments with platelet adhesion and protein adhesion assay in vitro, the two materials studied, including poly-DMMCA gel, all show excellent nonthrombogenicity. This confirms once again that the zwitterionic molecular structure on the surfaces of materials is essential for improving their nonthrombogenicity and biocompatibility. 相似文献
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Chengbin Jing Haiyang Shan Chuanjian Zhang Xiaodan Zang Wei Bai Junhao Chu 《Journal of Sol-Gel Science and Technology》2009,51(2):139-145
The solids content and gelation time of aqueous germanate solution were examined in this work. Samples of 5, 10 and 20 mol%
Mn doped Ge were prepared by using the aqueous germanate solution as a liquid Ge precursor. No second phase such as Mn5Ge3 was detected in the 5 and 10 mol% Mn doped samples, implying that Mn ions were uniformly diluted into the Ge host matrix.
The 5 and 10 mol% Mn-doped Ge samples exhibit room-temperature ferromagnetic behaviors that are likely originated from the
RKKY (Ruderman–Kittel–Kasuya–Yosida)-like interaction between the localized Mn ions in the Ge matrix. Therefore, the aqueous
germanate solution can be an alternative sol–gel precursor for preparation of the Mn
x
Ge1−x
diluted magnetic semiconductors (DMSs). 相似文献
230.
Liqing Yan 《Journal of Theoretical Probability》2009,22(4):827-836
Several sharp upper and lower bounds for the ratio of two normal probabilities $\mathbb{P}\Biggl(\,\bigcap_{i=1}^{n}\bigl\{\xi^{(1)}_i\leq \mu_i\bigr\}\Biggr)\Big/\mathbb{P}\Biggl(\,\bigcap_{i=1}^{n}\bigl\{\xi^{(0)}_i\leq \mu_i\bigr\}\Biggr)$ are given in this paper for various cases, where (ξ 1 (0) ,ξ 2 (0) ,…,ξ n (0) ) and (ξ 1 (1) ,ξ 2 (1) , …,ξ n (1) ) are standard normal random variables with covariance matrices R 0=(r ij 0 ) and R 1=(r ij 1 ), respectively. 相似文献