全文获取类型
收费全文 | 2702篇 |
免费 | 307篇 |
国内免费 | 106篇 |
专业分类
化学 | 691篇 |
晶体学 | 14篇 |
力学 | 678篇 |
综合类 | 29篇 |
数学 | 385篇 |
物理学 | 1318篇 |
出版年
2025年 | 8篇 |
2024年 | 27篇 |
2023年 | 41篇 |
2022年 | 50篇 |
2021年 | 63篇 |
2020年 | 63篇 |
2019年 | 72篇 |
2018年 | 59篇 |
2017年 | 62篇 |
2016年 | 53篇 |
2015年 | 49篇 |
2014年 | 114篇 |
2013年 | 198篇 |
2012年 | 130篇 |
2011年 | 139篇 |
2010年 | 134篇 |
2009年 | 169篇 |
2008年 | 183篇 |
2007年 | 170篇 |
2006年 | 187篇 |
2005年 | 146篇 |
2004年 | 153篇 |
2003年 | 112篇 |
2002年 | 99篇 |
2001年 | 78篇 |
2000年 | 66篇 |
1999年 | 53篇 |
1998年 | 69篇 |
1997年 | 56篇 |
1996年 | 48篇 |
1995年 | 47篇 |
1994年 | 35篇 |
1993年 | 21篇 |
1992年 | 26篇 |
1991年 | 26篇 |
1990年 | 26篇 |
1989年 | 17篇 |
1988年 | 17篇 |
1987年 | 9篇 |
1986年 | 8篇 |
1985年 | 9篇 |
1984年 | 6篇 |
1983年 | 5篇 |
1982年 | 5篇 |
1981年 | 1篇 |
1980年 | 1篇 |
1978年 | 3篇 |
1977年 | 1篇 |
1973年 | 1篇 |
排序方式: 共有3115条查询结果,搜索用时 0 毫秒
131.
本文提出了随机点场理论用于研究含有随机夹杂的统计非均匀介质。本文不同于其它作者,一般均将随机理论建立在Eshelby的等效夹杂原理之上,而这里是建立在Kunin的微结构理论基础之上。作为理论的一个应用,本文对复合材料的有效模量及夹杂内部及周围微观场进行了计算。 相似文献
132.
This is the first of two papers presenting a systematic development of a continuum model of a porous medium and of transport
processes occurring in it. The concept of a Representative Elementary Volume (REV) as opposed to any arbitrary volume of averaging
quantities at the micro-scale, is quantified. A universal criterion for selecting the size of an REV as a function of measurable
characteristics of a porous medium and selected tolerance levels of estimation errors, is developed. The rules of spatial
averaging are extended by including the effects of both the configuration of the solid matrix and of interphase transfer phenomena
within an REV. 相似文献
133.
We study the simultaneous one-dimensional flow of water and oil in a heterogeneous medium modelled by the Buckley-Leverett equation. It is shown both by analytical solutions and by numerical experiments that this hyperbolic model is unstable in the following sense: Perturbations in physical parameters in a tiny region of the reservoir may lead to a totally different picture of the flow. This means that simulation results obtained by solving the hyperbolic Buckley-Leverett equation may be unreliable.Symbols and Notation
f
fractional flow function varying withs andx
-
value off outsideI
-
value off insideI
-
local approximation off around¯x
-
f
–,f
+
values of
-
f
j
n
value off atS
j
n
andx
j
-
g
acceleration due to gravity [ms–2]
-
I
interval containing a low permeable rock
-
k
dimensionless absolute permeability
-
k
*
absolute permeability [m2]
-
k
c
*
characteristic absolute permeability [m2]
-
k
ro
relative oil permeability
-
k
rw
relative water permeability
-
L
*
characteristic length [m]
-
L
1
the space of absolutely integrable functions
-
L
the space of bounded functions
-
P
c
dimensionless capillary pressure function
-
P
c
*
capillary pressure function [Pa]
-
P
c
*
characteristic pressure [Pa]
-
S
similarity solution
-
S
j
n
numerical approximation tos(xj, tn)
-
S
1, S2,S
3
constant values ofs
-
s
water saturation
-
value ofs at
-
s
L
left state ofs (wrt.
)
-
s
R
right state ofs (wrt.
)
-
s
s for a fixed value of in Section 3
-
T
value oft
-
t
dimensionless time coordinate
-
t
*
time coordinate [s]
-
t
c
*
characteristic time [s]
-
t
n
temporal grid point,t
n=n t
-
v
*
total filtration (Darcy) velocity [ms–1]
-
W, , v
dimensionless numbers defined by Equations (4), (5) and (6)
-
x
dimensionless spatial coordinate [m]
-
x
*
spatial coordinate [m]
-
x
j
spatial grid piont,x
j=j x
-
discontinuity curve in (x, t) space
-
right limiting value of¯x
-
left limiting value of¯x
-
angle between flow direction and horizontal direction
- t
temporal grid spacing
- x
spatial grid spacing
-
length ofI
-
parameter measuring the capillary effects
-
argument ofS
-
o
dimensionless dynamic oil viscosity
- w
dimensionless dynamic water viscosity
-
c
*
characteristic viscosity [kg m–1s–1]
-
o
*
dynamic oil viscosity [kg m–1s–1]
-
w
*
dynamic water viscosity [k gm–1s–1]
-
o
dimensionless density of oil
-
w
dimensionless density of water
-
c
*
characteristic density [kgm–3]
-
o
*
density of oil [kgm–3]
-
w
*
density of water [kgm–3]
-
porosity
-
dimensionless diffusion function varying withs andx
-
*
dimensionless function varying with s andx
* [kg–1m3s]
-
j
n
value of atS
j
n
andx
j
This research has been supported by VISTA, a research cooperation between the Norwegian Academy of Science and Letters and Den norske stats oljeselskap a.s. (Statoil). 相似文献
134.
Paul Hölscher 《Transport in Porous Media》1992,9(1-2):73-84
The behaviour of the soil under a dynamically loaded pile toe is studied. The soil is modelled as a fluid saturated porous continuum. The constitutive behaviour of the solid skeleton is described by the elasto-plastic model of Drücker-Prager. The wave propagation is simulated with a dynamical finite-element program.A two-phase model of soil gives useful information about effective stress and pore pressure in the soil. In saturated soil the main wave under the pile toe propagates more downards than in dry soil, due to the higher compressional stiffness in saturated soil. The plastic zone under the pile toe propagates with the velocity of the fast compressional wave. The pore fluid influences the plasticity strongly and can be expected to affect pile driving too.The distribution of effective stress and pore pressure under the pile toe depends on the permeability of the soil and cannot be calculated uniquely from a single-phase calculation. Therefore, a nonlinear soil cannot be modelled correctly as a conventional single-phase material. 相似文献
135.
压电介质二维边界积分方程中的基本解 总被引:8,自引:0,他引:8
由于压电介质的变形-电场耦合效应及压电响应的各向异性,使解析求解压电介质问题的工作变量十分复杂,若采用边界元数值方法求解,必须具备积分方程中的基本解,本文根据电磁场方程及连续介质力学的耦合性质论层出了二维无限域中分别在单位力及单位电荷载作用下的位移场,电势场、应力场和电位移场的解,从而确立了边界积分方程中所必需的八个基本解。 相似文献
136.
颗粒介质的弹塑性动态本构关系研究 总被引:3,自引:0,他引:3
本文运用多刚体系统动力学和微结构连续力学的理论方法,考虑了颗粒体的拓扑结构及颗粒体之间的局部非线性相互作用,通过引进恢复系数,导出了适合于大变形运动(包括平动与转动)情况下,颗粒体间的滑移和分离的客观弹塑性本构关系。 相似文献
137.
138.
Doubly nonlinear parabolic-type equations as dynamical systems 总被引:1,自引:0,他引:1
In this paper, we study a class of doubly nonlinear parabolic PDEs, where, in addition to some weak nonlinearities, also some mild nonlinearities of porous media type are allowed inside the time derivative. In order to formulate the equations as dynamical systems, some existence and uniqueness results are proved. Then the existence of a compact attractor is shown for a class of nonlinear PDEs that include doubly nonlinear porous medium-type equations. Under stronger smoothness assumptions on the nonlinearities, the finiteness of the fractal dimension of the attractor is also obtained. 相似文献
139.
A new mathematical model is proposed for time-independent laminar flow through a rigid isotropic and consolidated porous medium of spatially varying porosity. The model is based upon volumetric averaging concepts. Explicit assumptions regarding the mean geometric properties of the porous microstructure lead to a relationship between tortuosity and porosity. Microscopic inertial effects are introduced through consideration of flow development within the pores. A momentum transport equation is derived in terms of the fluid properties, the porous medium porosity and a characteristic length of the microstructure. In the limiting cases of porosity unity and zero, the model yields the required Navier-Stokes equation for free flow and no flow in a solid, respectively. 相似文献
140.
We consider the homogenization of a time-dependent heat transfer problem in a highly heteregeneous periodic medium made of two connected components having finite heat capacities cα(x) and heat conductivities aα(x), α=1,2, of order one, separated by a third material with thickness of order ε the size of the basic periodicity cell, but with conductivity λa3(x) where a3=O(1) and λ tends to zero with ε. Assuming only that ci(x)?0 a.e., such that the problem can degenerate (parabolic-elliptic), we identify the homogenized problem following the values of δ=limε→0ε2/λ. To cite this article: M. Mabrouk, A. Boughammoura, C. R. Mecanique 331 (2003). 相似文献