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101.
M. Kočvara 《Structural and Multidisciplinary Optimization》1997,14(4):256-263
We consider the minimum-compliance formulation of the truss topology problem with additional linear constraints on the displacements: the so-called displacement constraints. We propose a new bilevel programming approach to this problem. Our primal goal (upper-level) is to satisfy the displacement constraint as well as possible — we minimize the gap between the actual and prescribed displacement. Our second goal (lower level) is to minimize the compliance — we still want to find the stiffest structure satisfying the displacement constraints. On the lower level we solve a standard truss topology problem and hence we can solve it in the formulation suitable for the fast interior point alogrithms. The overall bilevel problem is solved by means of the so-called implicit programming approach. This approach leads to a nonsmooth optimization problem which is finally solved by a nonsmooth solver. 相似文献
102.
Henny M. Borsboom Tatjana Claasen-Vujčić Harry J. G. Gaykema Toon Mehlkopf 《Magma (New York, N.Y.)》1997,5(1):33-37
The birdcage resonator is frequently used in conventional MRI because of its excellent attributes. Its use in low-field MRI
is restricted to field strengths higher than, for example, 0.1 T, dependent on the size of the coil. This is because of the
intrinsically low inductance value of the birdcage coils. Furthermore, the sensitivity of the birdcage at low field strengths
is significantly lower when compared to, for example, the solenoid. Both problems can be overcome with the multiturn technique
and a novel wound birdcage coil. The quadrature mode wound birdcage coil presented in this paper can be used at frequencies
as low as 100 kHz. Its sensitivity is also increased when compared to the conventional strip-ring birdcage. Homogeneity effective
volume, and methods to increase the resonator bandwidth to match the signal bandwidth are left intact. The latter is a typical
low-field problem. 相似文献
103.
A model-based approach to reconstruction of 3D human arm motion from a monocular image sequence taken under orthographic
projection is presented. The reconstruction is divided into two stages. First, a 2D shape model is used to track the arm silhouettes
and second-order curves are used to model the arm based on an iteratively reweighted least square method. As a result, 2D
stick figures are extracted. In the second stage, the stick figures are backprojected into the scene. 3D postures are reconstructed
using the constraints of a 3D kinematic model of the human arm. The motion of the arm is then derived as a transition between
the arm postures. Applications of these results are foreseen in the analysis of human motion patterns.
Received: 26 January 1996 / Accepted: 17 July 1997 相似文献
104.
Martina Bečvářová 《NTM》2004,12(1):40-48
The paper describes the Czech project in the history of mathematics which was initiated at the Faculty of Mathematics and
Physics of Charles University in Prague at the end of the eighties of the 20th century. Its main aim is to map the development
of mathematical research in the Czech lands in the second half of the nineteenth and the first half of the twentieth century.
The main result of this project is the production of monographs. These chart out the life and work of some prominent Czech
personalities-mathematicians who have had substantial influence on the development of Czech mathematics. The aim of the project,
the structure of the monographs and the general method are discussed in the paper. 相似文献
105.
V. A. Baranov V. A. Kalinnikov V. V. Karpukhin N. V. Khomutov A. S. Korenchenko S. M. Korenchenko N. P. Kravchuk N. A. Kuchinskii D. A. Mzhaviya A. M. Rozhdestvenskii V. V. Sidorkin Z. B. Tsamalaidze T. Sakhelashvili E. Frlež D. Počanić W. Li R. C. Minehart L. C. Smith W. A. Stephens K. O. H. Ziock W. Bertl R. Horisberger S. Ritt R. Schnyder H. P. Wirtz B. G. Ritchie I. Supek T. Kozlowski 《Instruments and Experimental Techniques》2005,48(2):168-176
The construction and characteristics of the PIBETA spectrometer are described. This spectrometer is designed to implement a program of precise measurement of pion decay + 0 + e
+ + e at the Paul Scherrer Institute (Switzerland). A spherical calorimeter, consisting of 240 crystals of pure CsI scintillator and embracing a solid angle of 3, is the main detector of the setup. In addition, the spectrometer is composed of an active collimator (which also acts as a beam degrader), a segmented active plastic target, two multiwire cylindrical proportional chambers, a 20-element cylindrical plastic hodoscope, and veto counters of cosmic muons.__________Translated from Pribory i Tekhnika Eksperimenta, No. 2, 2005, pp. 39–48.Original Russian Text Copyright © 2005 by Baranov, Kalinnikov, Karpukhin, Khomutov, A. Korenchenko, S. Korenchenko, Kravchuk, Kuchinskii, Mzhaviya, Rozhdestvenskii, Sidorkin, Tsamalaidze, Sakhelashvili, Frlez, Poanic, Li, Minehart, Smith, Stephens, Ziock, Bertl, Horisberger, Ritt, Schnyder, Wirtz, Ritchie, Supek, Kozlowski. 相似文献
106.
The aim of this work was to show that with the use of the surface roughness parameters Ssk and Sku we can predict tribological behavior of contact surfaces and use these parameters to plan surface texturing. This article presents a continuation of our research on virtual texturing and experimental work on surface textures in the form of channels. For this investigation, steel samples were laser surface textured in the shape of dimples with different spacings between the dimples and different dimple depths. The experimental results confirmed that the parameters Ssk and Sku can be used to design the surface texturing, where a higher value of Sku and more negative Ssk lead to lower friction. 相似文献
107.
108.
We have performed ab initio calculations with equilibrium supercells of the Mg2Ni compound and its hydride Mg2NiH4 doped with elements X = Al, Ga, In, Si, Ge and Sn. Two concentrations of X in both structures have been set: (1) every 16th, and (2) every fourth Ni atom has been substituted by X. Total energy calculations yielded the Mg2NiH4 hydrogen absorption enthalpy ΔHabs according to the chemical reaction Mg2Ni + 2H2 → Mg2NiH4. Reduction of the hydrogen absorption enthalpy was reported for both concentrations of X. When doping the Mg2NiH4 hydride with X = In in a low concentration (1), the value of hydrogen desorption enthalpy decreases from 68.22 to 55.96 kJ(mol H2)?1. Doping with X = In in a high concentration (2) further decreases the hydrogen desorption enthalpy to 5.50 kJ(mol H2)?1. Further, the electronic structure of Mg2(Ni–In)H4 hydride with a low In concentration indicates weaker Ni–H bonds in comparison with the pristine Mg2NiH4. Attraction between H and In atoms induced enhanced bonding between Mg and H atoms compared to the pristine Mg2NiH4. 相似文献
109.