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排序方式: 共有262条查询结果,搜索用时 373 毫秒
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This study is to numerically test the interfacial instability of ferrofluid flow under the presence of a vacuum magnetic field. The ferrofluid parabolized stability equations(PSEs) are derived from the ferrofluid stability equations and the Rosensweig equations, and the characteristic values of the ferrofluid PSEs are given to describe the ellipticity of ferrofluid flow. Three numerical models representing specific cases considering with/without a vacuum magnetic field or viscosity are created to mathematically examine the interfacial instability by the computation of characteristic values. Numerical investigation shows strong dependence of the basic characteristic of ferrofluid Rayleigh-Taylor instability(RTI) on viscosity of ferrofluid and independence of the vacuum magnetic field.For the shock wave striking helium bubble, the magnetic field is not able to trigger the symmetry breaking of bubble but change the speed of the bubble movement. In the process of droplet formation from a submerged orifice, the collision between the droplet and the liquid surface causes symmetry breaking. Both the viscosity and the magnetic field exacerbate symmetry breaking. The computational results agree with the published experimental results. 相似文献
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Wei Mingjun Zhu Wanzhen 《Annals of Differential Equations》2007,23(4):511-518
In this paper we consider the system of classical particles coupled with a Klein-Gordon field in two dimensions.We establish a-priori-bounds on the solutions of this system with initial data satisfying a size restriction derived from conservation of energy.This result,together with the smoothing of"velocity averaging",yields the existence of global weak solutions to the corresponding restricted initial value problem.The size restriction is necessary since energy of the system is indefinite.Finally,we show that the weak solutions preserve the total mass. 相似文献
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A hybrid heterogeneous catalyst system, which has been synthesized by covalently anchoring oxodiperoxo molybdenum chelate complexes onto the surface of mesoporous MCM-41, is highly active and truly heterogeneous for the liquid-phase epoxidation of cyclooctene with tBuOOH as the oxygen source. 相似文献
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全无机金属卤化物灵活多变的结构及优异的发光性能使其在固态光电子领域显示出重要的应用前景。本研究采用异价阳离子取代策略,用三价锑离子部分取代CsCdCl3中的二价镉离子,促进自陷激子的产生,使CsCdCl3∶Sb3+产生了明亮的宽带绿色发光,中心波长为530 nm。机理研究结果表明,CsCdCl3∶Sb3+中相邻SbCl6八面体被孤立,形成了低维电子构型,促进了Sb3+局域化,实现了量子效率最高为95.5%的高效发光。此外,尽管CsCdCl3和RbCdCl3均属于ACdCl3(A为碱金属家族),但它们的晶体结构明显不同。RbCdCl3属于正交晶系,空间群为Pnma;CsCdCl3属于六方晶系,空间群为P63/mmc。CsCdCl3的结构对称性大于RbCdCl3,其... 相似文献
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Self‐Propelled Janus Mesoporous Silica Nanomotors with Sub‐100 nm Diameters for Drug Encapsulation and Delivery 下载免费PDF全文
Mingjun Xuan Jingxin Shao Dr. Xiankun Lin Dr. Luru Dai Prof. Qiang He 《Chemphyschem》2014,15(11):2255-2260
The synthesis of an innovative self‐propelled Janus nanomotor with a diameter of about 75 nm that can be used as a drug carrier is described. The Janus nanomotor is based on mesoporous silica nanoparticles (MSNs) with chromium/platinum metallic caps and propelled by decomposing hydrogen peroxide to generate oxygen as a driving force with speeds up to 20.2 μm s?1 (about 267 body lengths per second). The diffusion coefficient (D) of nanomotors with different H2O2 concentrations is calculated by tracking the movement of individual particles recorded by means of a self‐assembled fluorescence microscope and is significantly larger than free Brownian motion. The traction of a single Janus MSN nanomotor is estimated to be about 13.47×10?15 N. Finally, intracellular localization and drug release in vitro shows that the amount of Janus MSN nanomotors entering the cells is more than MSNs with same culture time and particle concentrations, meanwhile anticancer drug doxorubicin hydrochloride loaded in Janus MSNs can be slowly released by biodegradation of lipid bilayers in cells. 相似文献
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保健食品样品用50%(体积分数)甲醇溶液超声提取15 min,提取液用水定容至50.0mL,离心,取上清液,经0.22μm微孔滤膜过滤,采用液相色谱-四极杆-静电轨道阱高分辨质谱法测定滤液中11种磷酸二酯酶抑制剂的含量。以Waters HSS T3色谱柱为固定相,以不同体积比的0.1%(体积分数)甲酸溶液和乙腈的混合液为流动相进行梯度洗脱,质谱分析中采用电喷雾离子源正离子模式和全扫描模式。11种磷酸二酯酶抑制剂的质量浓度均在2~100μg·L^-1内与其对应的峰面积呈线性关系,测定下限(10S/N)为0.02~0.5μg·L^-1。以空白样品为基体进行加标回收试验,所得回收率为75.7%~98.9%,测定值的相对标准偏差(n=6)为5.9%~14%。 相似文献