全文获取类型
收费全文 | 9607篇 |
免费 | 901篇 |
国内免费 | 652篇 |
专业分类
化学 | 4213篇 |
晶体学 | 123篇 |
力学 | 3143篇 |
综合类 | 73篇 |
数学 | 1016篇 |
物理学 | 2592篇 |
出版年
2024年 | 29篇 |
2023年 | 111篇 |
2022年 | 200篇 |
2021年 | 207篇 |
2020年 | 303篇 |
2019年 | 266篇 |
2018年 | 256篇 |
2017年 | 359篇 |
2016年 | 427篇 |
2015年 | 310篇 |
2014年 | 398篇 |
2013年 | 867篇 |
2012年 | 470篇 |
2011年 | 507篇 |
2010年 | 444篇 |
2009年 | 519篇 |
2008年 | 495篇 |
2007年 | 512篇 |
2006年 | 476篇 |
2005年 | 510篇 |
2004年 | 396篇 |
2003年 | 393篇 |
2002年 | 322篇 |
2001年 | 277篇 |
2000年 | 238篇 |
1999年 | 211篇 |
1998年 | 188篇 |
1997年 | 179篇 |
1996年 | 137篇 |
1995年 | 186篇 |
1994年 | 135篇 |
1993年 | 110篇 |
1992年 | 88篇 |
1991年 | 89篇 |
1990年 | 68篇 |
1989年 | 59篇 |
1988年 | 75篇 |
1987年 | 59篇 |
1986年 | 56篇 |
1985年 | 47篇 |
1984年 | 38篇 |
1983年 | 14篇 |
1982年 | 50篇 |
1981年 | 19篇 |
1980年 | 9篇 |
1979年 | 15篇 |
1978年 | 10篇 |
1976年 | 4篇 |
1973年 | 4篇 |
1971年 | 10篇 |
排序方式: 共有10000条查询结果,搜索用时 9 毫秒
91.
92.
Describing Hydrodynamic Particle Removal from Surfaces Using the Particle Reynolds Number 总被引:1,自引:0,他引:1
The fundamental processes related to the removal of fine particles from surfaces in a hydrodynamic flow field are not adequately understood. A critical particle Reynolds number approach is proposed to assess these mechanisms for fine particles when surface roughness is small compared to particle diameter. At and above the critical particle Reynolds number, particle removal occurs, while below the critical value, particles remain attached to a surface. The system under consideration consists of glass particles adhering to a glass surface in laminar channel flow. Our results indicate rolling is the removal mechanism, which is in agreement with the literature. Theoretical results of the critical particle Reynolds number model for rolling removal are in general agreement with experimental data when particle size distribution, particle and surface roughness, and system Hamaker constant are taken into account. 相似文献
93.
94.
95.
John D. Ramshaw 《Journal of statistical physics》1989,56(1-2):149-158
Phase space density representations of inviscid fluid dynamics were recently discussed by Abarbanel and Rouhi. Here it is shown that such representations may be simply derived and interpreted by means of the Liouville equation corresponding to the dynamical system of ordinary differential equations that describes fluid particle trajectories. The Hamiltonian and Poisson bracket for the phase space density then emerge as immediate consequences of the corresponding structure of the dynamics. For barotropic fluids, this approach leads by direct construction to the formulation presented by Abarbanel and Rouhi. Extensions of this formulation to inhomogeneous incompressible fluids and to fluids in which the state equation involves an additional transported scalar variable are constructed by augmenting the single-particle dynamics and phase space to include the relevant additional variable. 相似文献
96.
97.
98.
In this paper, we have investigated the motion of a heated viscoelastic fluid layer in a rectangular tank that is subjected to a horizontal periodic oscillation. The mathematical model of the current problem is communicated with the linearized Navier–Stokes equation of the viscoelastic fluid and heat equation together with the boundary conditions that are solved by means of Laplace transform. Time domain solutions are consequently computed by using Durbin's numerical inverse Laplace transform scheme. Various numerical results are provided and thereby illustrated graphically to show the effects of the physical parameters on the free-surface elevation time histories and heat distribution. The numerical applications revealed that increasing the Reynolds number as well as the relaxation time parameter leads to a wider range of variation of the free-surface elevation, especially for the short time history. 相似文献
99.
100.
Ali Rahmatpour Mahdi Abdollahi Mehrdad Shojaee 《Journal of Macromolecular Science: Physics》2013,52(3):523-531
A blend/clay nanocomposites of 50/50 (wt%) NR/SBR was prepared via mixing the latex of a 50/50 NR/SBR blend with an aqueous clay dispersion and co‐coagulating the mixture. The structure of the nanocomposite was characterized by transmission electron microscopy (TEM) and X-ray diffraction (XRD). Nanocomposites containing less than 10 phr clay showed a fully exfoliated structure. After increasing the clay content to 10 phr, both nonexfoliated (stacked layers) and exfoliated structures were observed in the nanocomposites. The results of mechanical tests showed that the nanocomposites presented better mechanical properties than clay‐free NR/SBR blend vulcanizate. Furthermore, tensile strength, tensile strain at break, and hardness (shore A) increased with increasing clay content, up to 6 phr, and then remained almost constant. 相似文献