全文获取类型
收费全文 | 929篇 |
免费 | 194篇 |
国内免费 | 40篇 |
专业分类
化学 | 118篇 |
晶体学 | 68篇 |
力学 | 548篇 |
综合类 | 9篇 |
数学 | 74篇 |
物理学 | 346篇 |
出版年
2024年 | 3篇 |
2023年 | 10篇 |
2022年 | 34篇 |
2021年 | 18篇 |
2020年 | 26篇 |
2019年 | 24篇 |
2018年 | 24篇 |
2017年 | 40篇 |
2016年 | 44篇 |
2015年 | 19篇 |
2014年 | 32篇 |
2013年 | 55篇 |
2012年 | 59篇 |
2011年 | 57篇 |
2010年 | 40篇 |
2009年 | 50篇 |
2008年 | 48篇 |
2007年 | 57篇 |
2006年 | 55篇 |
2005年 | 66篇 |
2004年 | 61篇 |
2003年 | 63篇 |
2002年 | 37篇 |
2001年 | 40篇 |
2000年 | 37篇 |
1999年 | 46篇 |
1998年 | 34篇 |
1997年 | 26篇 |
1996年 | 6篇 |
1995年 | 11篇 |
1994年 | 5篇 |
1993年 | 3篇 |
1992年 | 4篇 |
1990年 | 2篇 |
1988年 | 1篇 |
1987年 | 7篇 |
1985年 | 1篇 |
1984年 | 4篇 |
1983年 | 4篇 |
1982年 | 3篇 |
1981年 | 2篇 |
1980年 | 2篇 |
1979年 | 1篇 |
1978年 | 1篇 |
1957年 | 1篇 |
排序方式: 共有1163条查询结果,搜索用时 31 毫秒
1.
2.
The influence of the sample orientation on the effective value of the hydrostatic piezoelectric coefficients d
h
(i)
of Sn2P2S6 crystals has been studied. The hydrostatic piezoelectric coefficients d
h
(1)
and d′
h
(3)
, were measured, d
h
(1)
=(244±3) pC/N and d′
h
(3)
=(92±1) pC/N. The hydrostatic piezoelectric coefficient d
h
(3)
for orthogonal axis system was calculated to be d
h
(3)
=(87±2) pC/N. The, optimal orientation of the sample has been found as (Xy l)−20°-cut. Maximal value of the effective hydrostatic piezoelectric coefficient d
h
(1)
equals 260 pC/N. Double rotated samples were also studied. The orientation of the samples insensitive to the pressure has
been found. The theoretical mean value of hydrostatic piezoelectric coefficient (d
h
)
mean
corresponding to randomly oriented Sn2P2S6 grains in a poled composite has been calculated to be (d
h
)
mean
=136 pC/N. 相似文献
3.
Arman Melkumyan 《Zeitschrift für Angewandte Mathematik und Physik (ZAMP)》2007,58(2):330-349
The problem of electric and acoustic waves diffraction by a half-plane crack in a transversal isotropic piezoelectric medium
is investigated. The crack is assumed to be electric permeable and free of tractions. The so-called “quasi-hyperbolic approximation”
[15] is adopted. Applying Laplace transformations and Wiener–Hopf technique a closed form solution is obtained. By the means
of Cagniard–de Hoop method a detailed dynamic full electroacoustic wavefield’s investigation is conducted. Mode conversion
between electric and acoustic waves, effect of electroacoustic head wave, Bleustein–Gulyaev surface wave and the wavefield
structure depending on the type of the incident wave (acoustic or electric) and its angle of incidence are analyzed in details.
The dynamic field intensity factors at the crack tip depending on the angle of incidence and on time are derived explicitly.
Numerical analysis is presented. 相似文献
4.
We construct a model of a shell with piezoelectric elements (patches) that take into account the mutual influence of deformations and electric fields. Coupled problems for the shell with piezoelectric patches and an acoustic field, are studied and results on the existence and the uniqueness are obtained. For this system we consider an optimal control problem on noise attenuation and obtain results on the existence, the uniqueness, necessary and sufficient conditions of optimality. Copyright © 2003 John Wiley & Sons, Ltd. 相似文献
5.
6.
Tim R. Dargaville Julie M. Elliott Mathew Celina 《Journal of Polymer Science.Polymer Physics》2006,44(22):3253-3264
Films of piezoelectric PVDF and P(VDF‐TrFE) were exposed to vacuum UV (115–300 nm VUV) and γ‐radiation to investigate how these two forms of radiation affect the chemical, morphological, and piezoelectric properties of the polymers. The extent of crosslinking was almost identical in both polymers after γ‐irradiation, but surprisingly, was significantly higher for the TrFE copolymer after VUV‐irradiation. Changes in the melting behavior were also more significant in the TrFE copolymer after VUV‐irradiation due to both surface and bulk crosslinking, compared with only surface crosslinking for the PVDF films. The piezoelectric properties (measured using d33 piezoelectric coefficients and D‐E hysteresis loops) were unchanged in the PVDF homopolymer, while the TrFE copolymer exhibited more narrow D‐E loops after exposure to either γ‐ or VUV‐radiation. The more severe damage to the TrFE copolymer in comparison with the PVDF homopolymer after VUV‐irradiation is explained by different energy deposition characteristics. The short wavelength, highly energetic photons are undoubtedly absorbed in the surface layers of both polymers, and we propose that while the longer wavelength components of the VUV‐radiation are absorbed by the bulk of the TrFE copolymer causing crosslinking, they are transmitted harmlessly in the PVDF homopolymer. © 2006 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 44: 3253–3264, 2006 相似文献
7.
在镀银石英晶片上用压电免疫方法测定了0.5~50mg/L范围内的牛血清白蛋白的浓度,得到线性响应;并较全面地研究了压电晶片的回复性使用问题,以0.2mol/L甘氨酸-盐酸(pH=2.0)溶液洗脱时效果较好 相似文献
8.
动力学—压电石英晶体传感器测定水中微量汞的研究 总被引:4,自引:0,他引:4
基于涂银压电石英晶体对CN^-离子的灵敏响应,应用汞对六氰合铁酸钾与邻二氮杂菲反应的动力学催化作用,建立了动力学-PQC传感器单面触液测定微量汞的新方法。研究了PQC传感器对汞的响应机理,响应曲线,实验条件及共存离子干扰情况。 相似文献
9.
利用压电频移法测定水中的痕量亚硝酸盐 总被引:8,自引:0,他引:8
提出了利用压电频移法测定亚硝酸盐的方法。方法以碘离子与亚硝酸根之间的氧化还原反应为依据,通过测定由反应生成的碘所引起的压电晶体频率的变化,在被萃取水相中亚硝酸盐浓度为0.009 ̄2.3mg/L范围内,频移值与浓度成正比:ΔF=5.8+2.5×10^3C(mg/L),r=0.9901。方法简便,用于天然水中亚硝酸盐的测定,结果令人满意。 相似文献
10.
水热法合成K0.5Bi0.5TiO3纳米陶瓷粉体 总被引:3,自引:0,他引:3
K0.5Bi0.5TiO3(KBT)nanocrystalline particles were hydrothermally synthesized from Bi(NO3)3·5H2O, TiO2 and KOH. The crystal phase, chemical composition and microstructure were characterized by XRD, XRF, Raman scattering spectroscopy and TEM. The results indicated that the products were pure perovskite structured K0.5Bi0.5TiO3 with chemical stoichiometry and perovskite structure. The TEM observation revealed that the particles possessed a feature of cubic shape and a nano-scale of about 40 nm. The KBT ceramics sintered at 1 040 ℃ from hydrothermal powders show higher density and better electric properties than that prepared by a solid-state reaction method. 相似文献