全文获取类型
收费全文 | 4474篇 |
免费 | 677篇 |
国内免费 | 750篇 |
专业分类
化学 | 1881篇 |
晶体学 | 32篇 |
力学 | 880篇 |
综合类 | 58篇 |
数学 | 423篇 |
物理学 | 2627篇 |
出版年
2024年 | 8篇 |
2023年 | 50篇 |
2022年 | 117篇 |
2021年 | 128篇 |
2020年 | 107篇 |
2019年 | 123篇 |
2018年 | 149篇 |
2017年 | 160篇 |
2016年 | 198篇 |
2015年 | 180篇 |
2014年 | 263篇 |
2013年 | 401篇 |
2012年 | 253篇 |
2011年 | 315篇 |
2010年 | 255篇 |
2009年 | 290篇 |
2008年 | 285篇 |
2007年 | 294篇 |
2006年 | 287篇 |
2005年 | 254篇 |
2004年 | 241篇 |
2003年 | 193篇 |
2002年 | 194篇 |
2001年 | 155篇 |
2000年 | 136篇 |
1999年 | 142篇 |
1998年 | 127篇 |
1997年 | 99篇 |
1996年 | 78篇 |
1995年 | 81篇 |
1994年 | 75篇 |
1993年 | 42篇 |
1992年 | 35篇 |
1991年 | 34篇 |
1990年 | 16篇 |
1989年 | 26篇 |
1988年 | 19篇 |
1987年 | 14篇 |
1986年 | 6篇 |
1985年 | 14篇 |
1984年 | 9篇 |
1982年 | 16篇 |
1981年 | 7篇 |
1980年 | 2篇 |
1979年 | 7篇 |
1978年 | 7篇 |
1977年 | 2篇 |
1976年 | 2篇 |
1973年 | 2篇 |
1959年 | 1篇 |
排序方式: 共有5901条查询结果,搜索用时 15 毫秒
41.
42.
多电解质溶液中带电胶体粒子的电势分布由球形Poisson-Boltzmann方程(PBE)描述.PBE是一个非线性的微分方程,且难以求得其解析解.本文采用非线性P-B积分方程,计算电势分布的数值解.首先,根据静电场和热力学系统中的物理定理,导出描述电势分布的P-B积分方程(PBIE);其次,用迭代方法求PBIE的数值解.最后,计算了在3-1型电解液中无量纲半径κa分别为0.12和0.22,无量纲表面电势ξ分别为1,2,4,6时球形胶体粒子外部的电势值.为了检验数值解的精度,计算了表面电荷密度,并与Loeb(1961)和Oshima(1995)等人的结果比较,本文结果的相对误差小于1%,优于Oshima的结果. 相似文献
43.
碳酸氢铵沉淀法制备氧化钇粉体时反应条件对产物粒度的影响 总被引:7,自引:1,他引:7
研究了碳酸氢铵沉淀法的反应条件对氧化钇粒度的影响,探讨了粒度变化规律。发现在沉淀反应中,晶型碳酸钇铵的形成与否是影响氧化钇粒度的关键因素。在较低的反应温度下,当碳酸氢铵和氯化钇的浓度大于0.25mol·L-1,摩尔比大于5,陈化时间大于60min时得到碳酸钇铵沉淀,经煅烧可获得粒度(D50)大于1μm的氧化钇。当反应物浓度较低、摩尔比小,陈化时间较短时得到无定型碳酸钇沉淀,煅烧沉淀可获得粒度(D50)小于0.5μm的氧化钇。实验证明选择适当的沉淀反应条件,可制备D50在0.3~10μm范围内的不同粒度级别的氧化钇粉体。 相似文献
44.
Nicole Fietkau Fran?ois G Chevallier Li Jiang Timothy G J Jones Richard G Compton 《Chemphyschem》2006,7(10):2162-2167
The size of a glass sphere positioned in the center of a microdisk electrode is determined by using a simple electrochemical procedure and is confirmed, additionally, by a microscopical measurement of the sphere at the time of the electrochemical measurement. The cyclic voltammetric response of the naked electrode and of the electrode with the sphere positioned in its center is recorded over a wide range of scan rates (0.002-1.5 V s(-1)). The size of the sphere is then determined by comparison of the experimental voltammogram with simulations for each individual scan rate. 相似文献
45.
Hae‐Jeong Lee Christopher L. Soles Da‐Wei Liu Barry J. Bauer Wen‐Li Wu 《Journal of Polymer Science.Polymer Physics》2002,40(19):2170-2177
X‐ray reflectivity has been used to determine the mass uptake of probe molecules in porous thin films supported on thick silicon wafers. The adsorption occurs by capillary condensation when the films are exposed to probe vapor at controlled partial vapor pressures. The probe solvent partial pressure was varied by mixing saturated air and dry air at constant temperature or by changing sample temperature at a constant vapor concentration. Pore size distribution in the films can be calculated from the probe uptake with typical porosimetric approaches such as the application of the Kelvin equation to convert partial pressure into pore size. For illustration, the pore size distribution of three different nanoporous thin films, the primary candidate of ultra‐low‐k interlevel dielectrics in the next generation of integrated circuit chips, was determined with this technique. These samples represent different generations of low‐k dielectrics developed by industry. © 2002 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 40: 2170–2177, 2002 相似文献
46.
We consider the equilibrium dynamics of a system consisting of a spin interacting with an ideal Fermi gas on the lattice , 3. We present two examples: when this system is unitarily equivalent to an ideal Fermi gas or to a spin in an ideal Fermi gas without interaction between them. 相似文献
47.
The effectivity of solvents as electron pair donors 总被引:1,自引:0,他引:1
Y. Marcus 《Journal of solution chemistry》1984,13(9):599-624
The effectivity of solvents as electron pair donors, their donicity as expressed by their donor numbers DN, is reexamined. The linear dependence of the enthalpy and the Gibbs free energy for the reaction of donor solvents with antimony pentachloride is affirmed. Extension of the DN scale by other measured quantities, via their linear correlations for sets of solvents where both kinds of data are known is applied to Drago's E-C scale, Kamlet's scale, and Koppel's B scale. This extension, added to previous extensions employing Selbin's DI, II and Popov's 23Na, produces a DN scale for 170 solvents. The relation of DN measured for isolated solvent molecules in 1,2-dichloroethane to DN values measured for bulk solvents is examined by means of the scaled particle theory and solute-solvent interaction terms. A scale of normalized donor numbers DN
N
is presented. These values are practically the same as the scale, and for those solvents for which DN values are presented here and values are lacking, they can serve in their place for those preferring to use the scale for donor solvents. 相似文献
48.
采用改进颗粒床模型的CFD方法模拟了实验室规模冷模装置内鼓泡床的流体流动时空特性。模拟结果表明表观气速是影响气固动态特征和压力波动的主要因素之一:随表观气速的增大,气泡数目增加,气泡体积增大,压力波动增强;气速越高时均压降越大;在内循环鼓泡流化床内固体颗粒呈“单室”流型。上述与实验观察相吻合的模拟结果将有助于放大和设计商业化的内循环流化床生物质气化炉。 相似文献
49.
A theory is developed for the potential distribution around a charged spherical colloidal particle carrying ionized groups on the particle surface in a medium containing its counterions (i.e., counterions produced from dissociation of the particle surface groups) and a small amount of added salts on the basis of the theory of Imai and Oosawa. Numerical solutions to the Poisson–Boltzmann equation for the potential distribution are obtained for the case of dilute (but not infinitely dilute) particle suspensions of volume fraction 1 for
a1 (where is the Debye–Hückel parameter and a is the particle radius). Here we have taken into account the effects of (i) counterions from the particle surface groups, and (ii) the finite particle volume fraction. These effects, which are usually neglected in the conventional Poisson–Boltzmann equation, are found to be important. It is found that, as in the case of completely salt-free media, there is a certain critical value of the particle charge (which is the same as that for the completely salt-free case). When the particle charge is lower than the critical value, the potential is given by a Coulomb potential. If the particle charge is higher than the critical value, then counterions are accumulated in the vicinity of the particle surface (counterion condensation) and the potential becomes less dependent on the particle charge. The above behaviors can be observed even for the case where the electrolyte concentration is higher than the concentration of counterions from the particle surface groups, if the conditions
1 and a1are both satisfied. 相似文献
50.
In this paper are described the main characteristics of the plasma spraying process of alumina deposits, i.e., the temperature and flow field of the plasma jets obtained with the classical spraying torches, the injection of the particles into the plasma jet, the particle surface temperature and velocities in the plasma (measured for calibrated alumina particles), and the coating generation. The measurements on the alumina particles are compared with the predictions of a mathematical model. The experimental and computed particle velocities are in rather good agreement. However, this is not the case for the particle surface temperature. Possible reasons for the discrepancy are proposed (influence of the carrier gas, thermophoretic forces, and poor penetration of the particles into the plasma core even for an injection velocity twice that of the optimal calculated one, as shown by recent measurements). Finally the correlations between the particle velocities and surface temperature, and the properties of the alumina coating (porosity, crystal structure, mechanical properties) are studied. 相似文献