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91.
高文义 《有色金属材料与工程》2006,27(2):27-31
碳化硅砖和碳化硅砖与普通碳砖复合侧块,在上世纪末期我国铝电解槽上开始推广应用。使用后各厂家普遍发现碳化硅砖及碳化硅砖与普通碳块复合侧块均出现不同程度的断裂、上抬和脱落现象,该文对断裂、上抬和脱落原因进行了分析,并提出了改进措施。 相似文献
92.
P. Ravirajan S.A. Haque J.R. Durrant D.D.C. Bradley J. Nelson 《Advanced functional materials》2005,15(4):609-618
We report a study of the effects of polymer optoelectronic properties on the performance of photovoltaic devices consisting of nanocrystalline TiO2 and a conjugated polymer. Three different poly(2‐methoxy‐5‐(2′‐ethylhexoxy)‐1,4‐phenylenevinylene) (MEH‐PPV)‐based polymers and a fluorene–bithiophene copolymer are compared. We use photoluminescence quenching, time‐of‐flight mobility measurements, and optical spectroscopy to characterize the exciton‐transport, charge‐transport, and light‐harvesting properties, respectively, of the polymers, and correlate these material properties with photovoltaic‐device performance. We find that photocurrent is primarily limited by the photogeneration rate and by the quality of the interfaces, rather than by hole transport in the polymer. We have also studied the photovoltaic performance of these TiO2/polymer devices as a function of the fabrication route and device design. Including a dip‐coating step before spin‐coating the polymer leads to excellent polymer penetration into highly structured TiO2 networks, as was confirmed through transient optical measurements of the photoinduced charge‐transfer yield and recombination kinetics. Device performance is further improved for all material combinations studied, by introducing a layer of poly(ethylene dioxythiophene) (PEDOT) doped with poly(styrene sulfonic acid) (PSS) under the top contact. Optimized devices incorporating the additional dip‐coated and PEDOT:PSS layers produced a short‐circuit current density of about 1 mA cm–2, a fill factor of 0.50, and an open‐circuit voltage of 0.86 V under simulated AM 1.5 illumination (100 mW cm–2, 1 sun). The corresponding power conversion efficiency under 1 sun was ≥ 0.4 %. 相似文献
93.
陈克云 A.L.Epstein F.M.Chen D.C.P.Chen K.H.Lee G.L.Hung J.Y.Hong K.Y.Hong S.Ballard D.Payne M.E.Siegel J.Halls 《核技术》1989,(4)
不同浓度的~(131)I-Lym-2 MoAb与ARH-77和CEM细胞进行结合试验,结果表明:随浓度增大,结合值均升高;实验组裸鼠模型9只获得动力学数据。实验组和对照组注射~(131)I-Lym-2 MoAb后144h解剖,进行生物学分布(%D/g)测定,实验组肿瘤为16.88±12.64,肌肉为0.72±0.56。结果表明,~(131)I-131-Lym-2MoAb对临床B细胞淋巴瘤的放射免疫分析、显像有良好的效果。 相似文献
94.
A new method for characterization of stratified thermal energy stores (TES) that integrates both the first law and the second law concerns is presented here. The first law concern is incorporated into a quantity called energy response factor and the second law concern into an entropy generation ratio. A product of these two quantities is at the heart of the TES efficiency definitions. This approach removes the overemphasis of the existing methods either on the first or the second law of thermodynamics which often biases the characterization results. The information about the evolution of the temperature field of the system in time is the prerequisite of the new method. It may be obtained from experiments or from suitable numerical simulations. The current method can be easily integrated into computational fluid dynamic (CFD) simulations and thus facilitate CFD-based design analysis. As an example of such CFD-integrated analysis, a large-scale hot water seasonal heat store is numerically studied to identify the effects of aspect ratio, containment shape, internal structures, and containment size on their efficiency. The results suggest the effectiveness of the new method in deriving useful design insights. 相似文献
95.
讨论了热载流子注入对MOS结构C─V和I─V特性的影响。指出热载流子效应引起载流子陷落和界面态的产生,导致C─V特性曲线畸变、平带电压漂移和恒定电压下SiO2漏电流随时间漂移。本文论述了这些漂移的机理,提出了漂移的tn物理模型,从而很好地解释了实验所观察到的现象。 相似文献
96.
本文用不热形变栅状直丝化学气相沉积(CVD)法生长金刚石膜,在Si及WC-Co硬质合金衬底上金刚石膜晶面显露规律随衬底温度和甲烷浓度而异,经适当表面处理及选择合适的工艺条件,当生长初期衬底上就呈现出良好晶形的沉积膜,衬底与膜之间的粘结力能得到提高。Raman谱分析表明此膜仅具有特征金刚石1332cm ̄(-1)峰,通过SEM观察揭示出盒刚石膜可在表面、侧面及棱上生长,并与衬底有良好的联结。 相似文献
97.
Andreas Ruh 《Corrosion Science》2006,48(3):679-695
Thermogravimetric (TG) experiments have been carried out to study the kinetics of hot corrosion of Fe, Cr and Ni, covered by a molten KCl-ZnCl2 mixture of a composition close to the eutectic (50 mol% KCl-50 mol% ZnCl2). Furthermore binary and ternary phase diagrams were calculated in order to describe the corrosion process. The tests were conducted at a temperature of 320 °C in an atmosphere consisting of argon and oxygen. For iron different stages are observed in a TG curve. They can be attributed to the different reaction steps of iron chloride formation (incubation phase), oxide precipitation (linear stage) and scale formation (parabolic or logarithmic stage). Based on these observations a model, described by Spiegel [A. Spiegel, Molten Salt Forum 7 (2003) 253], is confirmed. For Cr and Ni these stages are not observed. At 8 vol% O2 only slight oxidation of Cr and Ni was observed accompanied by evaporation of the salt deposit. At 16 vol% O2 the rate of oxidation increases and the experiments yield a curve that is either parabolic or logarithmic for both Ni and Cr. As a result it is shown that the solubility of iron chloride in the KCl-ZnCl2 melt is higher than the solubility of nickel chloride and chromium (III) chloride in the KCl-ZnCl2 melt. This enables a higher diffusibility of iron chloride to the upper region of the melt where a higher oxygen partial pressure (p(O2)) is present leading to a higher oxidation rate of iron. 相似文献
98.
本文首先介绍国内和日本、德国、俄罗斯等国冷轧薄钢板及镀锌薄钢板的牌号、标记识别及生产地及与我国家标准薄钢板牌号的相互之间的关系,并比较具体地介绍冷轧板的实效性、镀锌薄钢板的锌层特性等诸多方面的状况。从而帮助我们在设计、制造家电产品中,比较正确地选择合适的板材。 相似文献
99.
Fuel cell-based automobiles have gained attention in the last few years due to growing public concern about urban air pollution
and consequent environmental problems. From an analysis of the power and energy requirements of a modern car, it is estimated
that a base sustainable power ofca. 50 kW supplemented with short bursts up to 80 kW will suffice in most driving requirements. The energy demand depends greatly
on driving characteristics but under normal usage is expected to be 200 Wh/km. The advantages and disadvantages of candidate
fuel-cell systems and various fuels are considered together with the issue of whether the fuel should be converted directly
in the fuel cell or should be reformed to hydrogen onboard the vehicle. For fuel cell vehicles to compete successfully with
conventional internal-combustion engine vehicles, it appears that direct conversion fuel cells using probably hydrogen, but
possibly methanol, are the only realistic contenders for road transportation applications. Among the available fuel cell technologies,
polymer-electrolyte fuel cells directly fueled with hydrogen appear to be the best option for powering fuel cell vehicles
as there is every prospect that these will exceed the performance of the internal-combustion engine vehicles but for their
first cost. A target cost of $ 50/kW would be mandatory to make polymer-electrolyte fuel cells competitive with the internal
combustion engines and can only be achieved with design changes that would substantially reduce the quantity of materials
used. At present, prominent car manufacturers are deploying important research and development efforts to develop fuel cell
vehicles and are projecting to start production by 2005. 相似文献
100.
A. Kadashchuk A. Andreev H. Sitter N.S. Sariciftci Y. Skryshevski Y. Piryatinski I. Blonsky D. Meissner 《Advanced functional materials》2004,14(10):970-978
We report on photoluminescence (PL) and thermally stimulated luminescence (TSL) in highly ordered nanostructures of para‐sexiphenyl (PSP) grown by hot wall epitaxy (HWE). A low‐energy broad band is observed in the PL spectra that can be attributed to the emission from molecular aggregates. While the intrinsic exciton emission in steady‐state PL dominates at low temperatures, the emission from aggregates increases with elevating temperature and its magnitude depends sensitively on film preparation conditions. Time‐resolved PL measurements showed that the aggregate emission decays with a life‐time of ≈ 4 ns, which is approximately an order of magnitude larger than the lifetime of singlet excitons. TSL data suggests the presence of an energetically disordered distribution of localized states for charge carriers in PSP films, which results from an intrinsic disorder in this material. A low‐temperature TSL peak with the maximum at around 30 K evidences for a weak energy disorder in PSP films, and has been interpreted in terms of a hopping model of TSL in disordered organic materials. 相似文献