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141.
研究了从声散射场的远场分布的信息来再现声阻抗障碍物形状的反问题,建立了求解这类反问题的一种非线性最优化模型,并提出了数值实现该非线性最优化模型的一种两步调整迭代算法.两步过程的应用使在确定未知障碍物形状的非线性最优化步中未知函数的个数达到了最少,而在调整迭代过程中,通过利用前一迭代步所得重构信息,使重构精度得到了相当大的改进.所建立的反演算法的一个特别吸引人的性质是,只需要远场分布的一个Fourier系数即可对未知声阻抗障碍物作几何物形的设别.对大量具有各种几何形状的二维障碍物的数值算例保证了本算法是实用和有效的. 相似文献
142.
研究了无取向硅钢W23G,W10,W14和取向硅钢Q8G4种材料在不同形变量下的磁声发射(MAE)和巴克豪森噪音(BN),结果表明MAE随形变量增大而减少,BN随形变量的增大而增大.测量了形变量为10.4%的W18和W23G在100,200,300,…,700°C各退火1h的MAE与BN值.其中MAE值随退火温度的升高逐渐增大,BN值在高于500°C退火时明显下降.并对上述实验结果进行了详细讨论. 相似文献
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146.
PROPAGATION OF SURFACE ACOUSTIC WAVES IN PRESTRESSED ANISOTROPIC LAYERED PIEZOELECTRIC STRUCTURES 总被引:1,自引:0,他引:1
Liu Hua Kuang Zhenbang Cai Zhengming 《Acta Mechanica Solida Sinica》2003,16(1):16-23
The propagation of surface acoustic waves in layered piezoelectric structures withinitial stresses is investigated.The phase velocity equations are obtained for electrically free andshorted cases,respectively.Effects of the initial stresses on the phase velocity and the electrome-chanical coupling coefficient for the fundamental mode of the layered piezoelectric structures arediscussed.Numerical results for the c-axis oriented fihn of LiNbO_3 on a sapphire substrate aregiven.It is found that the fractional change in phase velocity is a linear function with the ini-tial stresses,and the electromechanical coupling factor increases with an increase of the absolutevalues of the compressive initial stresses.The results are useful for the design of surface acousticwave devices. 相似文献
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148.
A. Gedeon 《Applied physics. B, Lasers and optics》1973,2(1):15-22
Efficient focussing of surface acoustic waves has been achieved using a properly shaped gold film deposit on the −22.3° rotated
Y-cut surface of quartz. The acoustic wave field was studied with laser probing techniques. A more than threefold increase
in intensity and a tenfold decrease in beam width was observed at the focal point. The focussing action was obtained with
the elastic wave equivalent of the Fresnel phase-reversal zone plate of optics. The multiple foci of this device allowed a
simultaneous generation of acoustic waves in nearly all directions on the surface. Consequently, the surface wave velocity
anisotropy could be determined completely. The experimental results are in very good agreement with the calculated velocity
anisotropy. Electromagnetic diffraction theory is adopted to the two dimensional anisotropic system to analyse the performance
of the focussing device. 相似文献
149.
The residual stresses in a shrink-fit specimen were measured ultrasonically, using shear-horizonal (SH) waves transmitted and received by noncontacting electromagnetic acoustic transducers. The presence of stress induces a small change in the velocity of the SH-waves. The difference in velocities of orthogonally polarized SH-waves (acoustic birefringence) was measured with a simple time-interval averaging system; this velocity difference can be related to the difference of principal stresses. The presence of material anisotropy (texture) in the specimen also causes relative velocity changes comparable to stress-induced changes. A simple method was used to remove the anisotropy-dependent component of the total relative velocity change, thereby allowing a determination of residual stress. This method consisted of measuring the birefringence in unstressed reference specimens and subtracting it from the birefringence measured at stressed locations. For the specimen used here, good agreement between theoretical and experimental values of stress was obtained. 相似文献
150.
Polystyrene particles of 9 μm diameter were acoustically concentrated along the axis of a water-filled cylindrical waveguide containing a 3 MHz standing wave field. Modulation of the acoustic field enabled transport of the concentrated particles in the axial direction. Four modulations were investigated; 1, a fixed frequency difference introduced between two transducers; 2, ramping the transducer frequency; 3, tone burst, i.e. sound that is pulsed on and off, allowing intermittent sedimentation under gravity; and 4, switching the sound off to allow continuous sedimentation. The most efficient transport (leaving the fewest particles in suspension) of clumps to one end of the container was achieved with method 1 above. In this system the maximum speed of transport of the axial clumps was 24 mm s-1. A theory developed here for the transport of particles in a pseudo (i.e. slowly moving) standing wave field predicts an upper limit, which increases with particle size, for the speed of an entrained body. For a single 9 μm diameter particle in a field with a spatial peak pressure amplitude of 0.4 MPa this speed would be 0.5 mm s-1. The higher experimental speeds observed here emphasize the value of acoustically concentrating particles into relatively large clumps prior to initiating transport. 相似文献