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71.
The propagation of rough and smooth wall pre-existing turbulent fluid fractures is investigated. The laminar fluid fracture is included as a special case for comparison. Lubrication theory is assumed to apply in the fracture and turbulence is introduced through the wall shear stress. The Perkins–Kern–Nordgren approximation is made in which the fluid pressure is proportional to the half-width of the fracture. The fracture half-width satisfies a non-linear diffusion equation. By using a linear combination of the Lie point symmetries of the non-linear diffusion equation a group invariant solution for the fracture length, volume and half-width is derived. The evolution of the length, half-width and mean flow velocity is analysed for a range of working conditions at the fracture entry. It is found that the mean flow velocity increases approximately linearly along the fracture.  相似文献   
72.
Effects of High Temperature Storage (HTS) and bonding toward microstructure change of intermetallic compound (IMC) at the wire bonding interface of 3 types of bond pad (Al, AlSiCu and NiPdAu) were presented in this paper. Optical and electron microscope analyses revealed that the IMC growth rate of samples under 175 and 200 °C HTS increased in the order of Al > AlSiCu > NiPdAu. Besides, higher HTS and bonding temperatures also promoted higher IMC thickness. The compositional study showed that higher HTS and bonding temperature developed rapid interdiffusion in bonding interface. In the mechanical ball shear test, a decrease of the shear force of Al and AlSiCu bond pads after 500 h HTS was believed due to poorly developed IMC at bonding interface. On the other hand, shear force degradation at 1000 h was due to excessive growth of IMC that in turn causes the formation of defects. For NiPdAu bond pad, increasing trend of shear force with HTS duration at 175 °C implied a good reliability of the Cu wire bonding. The rapid microscopic inspection on Cu wired Al bond pad under HTS 175 °C showed the IMC development from the periphery to the center of the ball bond. However, after 500 h voids started to develop until the crack was observed at 1000 h.  相似文献   
73.
The transverse and longitudinal mechanical properties of aramid fibers like Kevlar? 29 (K29) fibers are strongly linked to their highly oriented structure. Mechanical characterization at the single fiber scale is challenging especially when the diameter is as small as 15 µm. Longitudinal tensile tests on single K29 fibers and single fiber transverse compression test (SFTCT) have been developed. Our approach consists of coupling morphological observations and mechanical experiments with SFTCT analysis by comparing analytical solutions and finite element modeling. New insights on the analysis of the transverse direction response are highlighted. Systematic loading/unloading compression tests enable to experimentally determine a transverse elastic limit. Taking account of the strong anisotropy of the fiber, the transverse mechanical response sheds light on a skin/core architecture. More importantly, results suggest that the skin of the fiber, typically representing a shell of one micrometer in thickness, has a transverse apparent modulus of 0.2 GPa. That is around more than fifteen times lower than the transverse modulus of 3.0 GPa in the core. By comparison, the measured longitudinal modulus is about 84 GPa. The stress distribution in the fiber is explored and the critical areas for damage initiation are discussed. © 2015 Wiley Periodicals, Inc. J. Polym. Sci., Part B: Polym. Phys. 2016 , 54, 374–384  相似文献   
74.
Globular proteins exhibit dielectrophoresis (DEP) responses in experiments where the applied field gradient factor ∇E2 appears far too small, according to standard DEP theory, to overcome dispersive forces associated with the thermal energy kT of disorder. To address this a DEP force equation is proposed that replaces a previous empirical relationship between the macroscopic and microscopic forms of the Clausius–Mossotti factor. This equation relates the DEP response of a protein directly to the dielectric increment δε+ and decrement δε that characterize its β-dispersion at radio frequencies, and also indirectly to its intrinsic dipole moment by way of providing a measure of the protein's effective volume. A parameter Γpw, taken as a measure of cross-correlated dipole interactions between the protein and its water molecules of hydration, is included in this equation. For 9 of the 12 proteins, for which an evaluation can presently be made, Γpw has a value of ≈4600 ± 120. These conclusions follow an analysis of the failure of macroscopic dielectric mixture (effective medium) theories to predict the dielectric properties of solvated proteins. The implication of a polarizability greatly exceeding the intrinsic value for a protein might reflect the formation of relaxor ferroelectric nanodomains in its hydration shell.  相似文献   
75.
Thermomechanical cycles including programming, cooling, unloading and heating to trigger the 1WE were examined for a shape memory polymer (SMP), Tecoflex® (TFX EG-72D). Cycles were performed at 60°C with 50% and 225% strains and the recovery time of 10 min. Strains evolving with time were estimated during the thermomechanical treatments for the total 44 cycles using 50% strains and the total 50 cycles using 225% strains. Recovery ratios for 50% strains and 225% were also estimated. It turns out that programming, cooling, unloading and heating to trigger the 1WE causes an increase of irreversible strain and is associated with a corresponding decrease of the intensity of the 1WE in particular during the first thermomechanical cycles. In parallel scanning electron microscopic study using secondary electron imaging shows a very slight wavy surface structure evolved during cycling.  相似文献   
76.
The recent advances in digital photoelasticity have made it possible to use it conveniently for the stress analysis of articles and components made of glass. Depending on the application, the retardation levels to be measured range from a few nanometres to several thousand nanometres, which necessitates different techniques and associated equipments. This paper reviews the recent advances in the photoelasticity of glass with a focus on the techniques/methods developed in the last decade. A brief introduction to the residual stress in glass is provided initially to bring out its tensorial nature. The subsequent sections are organised thematically rather than chronologically, for better readability and easy access of information.  相似文献   
77.
Polycrystalline diamond compacts (PDC) were synthesized using diamond powder of average crystal size 3-20 μm by the Ni 70 Mn 25 Co 5 alloy infiltration technique at high temperature and high pressure (HPHT).The surface residual stress of polycrystalline diamond (PCD) layer was measured using micro-Raman spectroscopy with hydrostatic stress model and X-ray diffraction (XRD).Measurements of the stress levels of PCDs show that the residual compressive stresses range from 0.12 to 0.22 GPa,which increase with th...  相似文献   
78.
《Electroanalysis》2017,29(3):806-813
An electrochemical quartz crystal microbalance (EQCM) is described, which measures the shifts of frequency and bandwidth on multiple harmonics with a time‐resolution of 10 milliseconds. The technique requires the process under study to be repetitive. Examples are square wave amperometry and cyclovoltammetry. Data acquisition is fast because the raw data consist of traces of the electrical admittance at fixed frequencies . A few (∼10) such time traces are acquired sequentially at a set of frequencies evenly spaced around the crystal's resonance. Since all time‐traces are triggered by the same repetitive process, plots of the conductance G i , t ) and the susceptance B i , t ) from constant time delays, t , versus frequency can be produced a posteriori. The shifts, ΔG i ) and ΔB i ) quantify a difference between two resonance curves, pertaining to the sample's reference state and the state at time t . Fitting a difference of two resonance curves to these data, one obtains shifts of frequency, Δf (t ) and shifts of bandwidth, ΔΓ(t ), versus time. This procedure is repeated for the different overtones. Given the repetitive nature of the process, one may accumulate and average, which lowers the noise down to a few tens of mHz. The capabilities of this instrument are demonstrated with two examples, which are copper deposition/dissolution and electro‐responsivity of a polymer film containing weakly acidic side groups.  相似文献   
79.
在前人工作的基础上,运用一元三次方程的理论直接求解应力状态的特征方程,得到了实用的主应力计算公式.  相似文献   
80.
荒漠地区由于气候干燥,降水稀少,水分常成为制约植被生长的因素之一,水分胁迫对植物长势和产量的影响比任何其他胁迫都要大。随着高光谱技术的发展,国内外已有众多学者利用高光谱数据研究植被遭受胁迫作用,然而这些研究对象多集中于甜菜、棉花、玉米、水稻等作物,针对干旱区盐生植被遭受胁迫作用的研究较少。梭梭作为荒漠、半荒漠地区的典型盐生植被之一,具有极高的经济和生态效益。选择梭梭作为研究对象,培育一年生梭梭,并设置三个水分梯度,形成受不同水分量胁迫的梭梭。使用原始光谱、红边位置参数,结合植被指数及二维相关光谱研究其叶片光谱特征,为干旱区利用高光谱遥感监测盐生植被提供借鉴。结果表明:(1)分析梭梭叶片反射光谱曲线发现,在可见光至中红外各波段范围内,受不同水分量胁迫作用的梭梭叶片光谱反射率有显著差异。在可见光(350~610 nm)波段,各水分处理的梭梭叶片反射率依次为100 mL>500 mL>200 mL,这是由于100和200 mL水分促进梭梭内部叶绿素合成,使该波段反射率降低,而过多的水分(500 mL)对梭梭内部的叶绿素合成没有更大的促进作用。在红光区(611~738 nm),随着水分量的增多,受不同水分量胁迫的梭梭叶片光谱反射率依次减小。在738~1 181和1 228~1 296 nm波段,受不同水分量胁迫作用的梭梭叶片光谱反射率为:200 mL>100 mL>500 mL;在1 182~1 227 nm波段,受不同水分量胁迫作用的梭梭叶片光谱反射率为:100 mL>200 mL>500 mL。这是由于植被细胞结构对近红外区域的反射率影响较大,因而受不同水分胁迫作用的梭梭叶片光谱反射率有显著差异。在1 300~1 365和1 392~1 800 nm波段,受各水分胁迫作用的梭梭叶片反射率为:100 mL>200 mL>500 mL。这表明在500 mL水分胁迫量范围内,水分越多,叶子的细胞液、细胞膜对水分的吸收能力越强,使得反射率下降。通过对原始光谱求取一阶导数并提取红边位置参数发现,各水分处理下的梭梭叶片一阶微分光谱曲线中红边位置未发生移动。这是由于梭梭在长期的干旱环境影响下,形成了特殊的适应机制,水分对其红边位置影响不敏感。(2)选取若干植被指数分析各水分处理下的梭梭光谱指数变化。当水分胁迫量由100 mL增至200 mL时,WI/NDWI,MSI和NDII指数值变化显著,可用于研究水分胁迫下梭梭的光谱特征。(3)使用二维相关光谱技术分析受各水分胁迫作用的梭梭光谱特征,得出在100 mL水分胁迫下,在536,643,1 219和1 653 nm波段处,吸收峰对水分的微扰敏感;在200 mL水分胁迫下,在846和1 083 nm波段处,吸收峰对水分的微扰敏感;在500 mL水分胁迫下,在835和1 067 nm波段处,吸收峰对水分的微扰敏感。总之,在近红外波段,与100 mL水分量相比,梭梭受200和500 mL水分量胁迫时,吸收峰对水分的微扰敏感度上升。由100 mL水分胁迫下梭梭的二维同步相关谱图可知,1 044和1 665 nm,1 072和903 nm,903和1 264 nm,1 230和1 061 nm波段处形成正交叉峰,表明这些波段处光谱强度随水分的干扰同时变化。  相似文献   
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