全文获取类型
收费全文 | 2003篇 |
免费 | 75篇 |
国内免费 | 20篇 |
专业分类
化学 | 227篇 |
晶体学 | 4篇 |
力学 | 247篇 |
综合类 | 29篇 |
数学 | 1193篇 |
物理学 | 398篇 |
出版年
2024年 | 2篇 |
2023年 | 10篇 |
2022年 | 10篇 |
2021年 | 30篇 |
2020年 | 49篇 |
2019年 | 41篇 |
2018年 | 27篇 |
2017年 | 62篇 |
2016年 | 51篇 |
2015年 | 25篇 |
2014年 | 54篇 |
2013年 | 155篇 |
2012年 | 67篇 |
2011年 | 69篇 |
2010年 | 54篇 |
2009年 | 89篇 |
2008年 | 69篇 |
2007年 | 94篇 |
2006年 | 75篇 |
2005年 | 95篇 |
2004年 | 83篇 |
2003年 | 83篇 |
2002年 | 81篇 |
2001年 | 65篇 |
2000年 | 53篇 |
1999年 | 68篇 |
1998年 | 47篇 |
1997年 | 30篇 |
1996年 | 30篇 |
1995年 | 52篇 |
1994年 | 28篇 |
1993年 | 28篇 |
1992年 | 19篇 |
1991年 | 12篇 |
1990年 | 11篇 |
1989年 | 14篇 |
1988年 | 13篇 |
1987年 | 8篇 |
1986年 | 11篇 |
1985年 | 56篇 |
1984年 | 60篇 |
1983年 | 49篇 |
1982年 | 32篇 |
1981年 | 2篇 |
1979年 | 6篇 |
1978年 | 6篇 |
1977年 | 9篇 |
1976年 | 6篇 |
1975年 | 4篇 |
1974年 | 4篇 |
排序方式: 共有2098条查询结果,搜索用时 15 毫秒
31.
R. Horst 《Journal of Optimization Theory and Applications》1989,61(1):143-146
This technical comment refers to the discussion of strong consistency of several bounding procedures in Lemma 2.1 and Proposition 2.1 of Ref. 1. A necessary clarification is given of the notion of convergence q in Lemma 2.1, and a derivation of Proposition 2.1 is presented that includes a new and simple consistency proof of the classical bounding by convex envelopes used in many branch-and-bound procedures. 相似文献
32.
J. A. Poulis C. H. Massen E. Robens G. Reichenauer 《Journal of Thermal Analysis and Calorimetry》2004,76(2):583-592
On the basis of a molecular model for adsorption kinetics Jäntti introduced a method to calculate equilibriums shortly after a change of the pressure of the sorptive gas. In the present paper we show that this method is useful in many more situations than those intended originally. 相似文献
33.
Stéphane Roux 《Journal of statistical physics》1987,48(1-2):201-213
We introduce a family of stochastic processes which are a natural extension of Brownian motion to a tensor form. This allows us to solve a Dirichlet problem of linear elasticity obeying Lamé's equation, [1–(d– 1)]2V(x)+ [·V(x)]=0. 相似文献
34.
35.
Pulverized coal plasma gasification 总被引:11,自引:0,他引:11
R. A. Kalinenko A. P. Kuznetsov A. A. Levitsky V. E. Messerle Yu. A. Mirokhin L. S. Polak Z. B. Sakipov A. B. Ustimenko 《Plasma Chemistry and Plasma Processing》1993,13(1):141-167
A number of experiments on the plasma-vapor gasification of brown coals of three types have been carried out using an experimental plant with an electric-arc reactor of the combined type. On the basis of the material and heat balances, process parameters have been obtained: the degree of carbon gasification (c), the level of sulfur conversion into the gas phase (s), the synthesis gas concentration (CO+Hz) in the gaseous products, and the specific power consumption for the gasification process. The degree of gasification was 90.5-95.0%, the concentration of the synthesis gas amounted to 84.7–85.7%, and the level of sulfur conversion into the gas phase was 94.3–96.7%. Numerical study of the process of plasma gasification of coals was carried out using a mathematical model of motion, heating, and gasification of polydisperse coal particles in an electric-arc reactor of the combined type with an internal heat source (arc). The initial conditions for a conjugate system of nonlinear differential equations of the gas dynamics and kinetics of a pulverized coal stream interacting with the electric arc and oxidizer (water vapor) agree with the initial conditions of the experiments. The computation results satisfactorily correlate with the experimental data. The mathematical model can be used for the determination of reagent residence time and geometrical dimensions of the plasma reactor for the gasification of coals.Nomenclature
c
i
volume concentration of components (kmol m–3)
-
x
longitudinal coordinate (m)
-
f
i
source members, determined by variation of the ith component due to chemical reactions in unit volume in unit time (kmol m–3s–1)
-
velocity (m s–1)
-
M
s
ash mass in one particle (kg)
-
C
D
particle drag coefficient
-
3.14
-
r
s
particle radius (m)
-
d
particle diameter (m)
-
density (kg m–3)
-
C
p
heat capacity of components (J molt– K–1)
-
Q
j
thermal effect of reaction (J kmol–1)
- Ej
activation energy of reaction
-
N
l
volume concentration of particles of thelth fraction (m–3)
-
T
temperature (K)
-
emissivity factor of coal particles
-
5.67 × 10–8, blackbody emissivity coefficient (W m–2 K–4)
-
P
pressure (Pa)
-
S
reactor cross section (m2)
-
D
reactor diameter (m)
-
V
reactor volume (m3)
-
L
R
reactor length (m)
-
F
W
friction force on the wall (N)
-
f
g
friction coefficient
-
residence time (s)
- Nu
Nusselt number
- Re
Reynolds number
- Pr
Prandtl number
-
thermal conductivity of gas (J m– s–1 K–1)
-
R
8.3 × 103, universal gas constant (J kmol K–1)
- µ
i
molecular mass of component (kg kmol–1)
-
dynamic viscosity coefficient of gas (kg m–1 s–1)
-
thermal efficiency of plasma reactor
- qarc
specific heat flow from arc (W m–3)
-
P
1
heat supplied in vapor at T = 405 K (W)
-
P
2
heat loss to wall (W)
-
P
3
heat loss in the gas and slag separator chamber (W)
-
P
4
heat loss in the synthesis gas oxidation chamber (W)
-
P
5
heat loss in the slag catcher (W)
-
P
6
heat carried away in the off-gas (W)
- P
heat input of arc (W)
-
P
arc
electric power of arc (W)
- Qsp
specific power consumption (kw Hr kg–1)
-
d
w
specific heat flow to wall (W m–2)
-
c
degree of carbon gasification (%)
-
s
level of sulfur conversion into gas phase (%) 相似文献
36.
Zeolite-based monoliths (Cu/ZSM-5 on cordierite) are prepared and used to catalyze direct decomposition of nitrogen monoxide. Two-dimensional heterogeneous model is applied to describe the behavior of the monolith reactor, with the emphasis on the features introduced due to coupling of flow, mass transfer and chemical reaction. The proposed model has been verified by comparing computer simulation data with laboratory experimental data. It is shown that both inter- and intraphase diffusion limitations have to be considered when modeling complex reactor configuration, such as monolith reactors, especially when monolith with thicker catalytic layer are used at higher temperatures. 相似文献
37.
The considered mathematical model of the decomposition of valerate presents three unknown kinetic parameters, two unknown
stoichiometric coefficients, and three unknown initial concentrations for biomass. Applying a structural identifiability study,
we concluded that it is necessary to perform simultaneous batch experiments with differenitial conditions for estimating these
parameters. Four simultaneous batch experiments were conducted at 55°C, characterized by four different initial acetate concentrations.
Product inhibition of valerate degradation by acetate was considered. Practical identification was done optimizing the sum
of the multiple determination coefficients for all measured state viariables and for all experiments simultaneously. The estimated
values of kinetic parameters and stoichiometric coefficients were characterized by the parameter correlation matrix, the confidence
interval, and the student's t-test at 9% significance level with positive results except for the saturation constant, for which more eperiments for improving
its identifiability should be conducted. In this article, we discussekinetic parameter estimation methods. 相似文献
38.
39.
Analytical solutions of the diffusion equations to obtain the diffusant concentrations in the macro- and micropores which constitute the pore system of a zeolite bed are presented. The parameter which determines the influence of each pore type on the evolution of the adsorbate/adsorbant system towards the equilibrium state is described. Examples are given to illustrate a qualitative and quantitative study based on the curves obtained from these equations. 相似文献
40.
Keith R. Roby 《Theoretical chemistry accounts》1974,33(2):105-113
The mathematical basis of LCAO MO theory is studied, both within the Hartree-Fock approximation and in more exact formulations. The basic LCAO expansion for molecular orbitals ¦> in terms of atomic orbitals ¦x> is conveniently written ¦> = ¦x>
S
–1
B where S is the overlap matrix for atomic orbitals and B is the matrix of atomic orbital-molecular orbital overlaps. It is suggested that matrices P and Q, defined by P=B B and Q=BnB where n is the matrix of molecular orbital occupation numbers, are appropriate to the interpretation of molecular calculations in terms of atomic orbital components, electronic populations and the degree of bonding. Implications for Hartree-Fock calculations are investigated. 相似文献