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1.
本文分析了重力作用压头对低温热水计量采暖系统共用立管形式的影响,通过运用基尔霍夫定律分析了下分异程式双管系统和下分同程式双管系统的水力平衡状况,得出了下分异程式双管系统更适用于低温热水采暖系统的结论,并确定了立管经济比摩阻的范围和下分异程式双管可以负担的楼层数。  相似文献   
2.
The magnetospheric imaging instrument (MIMI) is a neutral and charged particle detection system on the Cassini orbiter spacecraft designed to perform both global imaging and in-situ measurements to study the overall configuration and dynamics of Saturn’s magnetosphere and its interactions with the solar wind, Saturn’s atmosphere, Titan, and the icy satellites. The processes responsible for Saturn’s aurora will be investigated; a search will be performed for substorms at Saturn; and the origins of magnetospheric hot plasmas will be determined. Further, the Jovian magnetosphere and Io torus will be imaged during Jupiter flyby. The investigative approach is twofold. (1) Perform remote sensing of the magnetospheric energetic (E > 7 keV) ion plasmas by detecting and imaging charge-exchange neutrals, created when magnetospheric ions capture electrons from ambient neutral gas. Such escaping neutrals were detected by the Voyager l spacecraft outside Saturn’s magnetosphere and can be used like photons to form images of the emitting regions, as has been demonstrated at Earth. (2) Determine through in-situ measurements the 3-D particle distribution functions including ion composition and charge states (E > 3 keV/e). The combination of in-situ measurements with global images, together with analysis and interpretation techniques that include direct “forward modeling’’ and deconvolution by tomography, is expected to yield a global assessment of magnetospheric structure and dynamics, including (a) magnetospheric ring currents and hot plasma populations, (b) magnetic field distortions, (c) electric field configuration, (d) particle injection boundaries associated with magnetic storms and substorms, and (e) the connection of the magnetosphere to ionospheric altitudes. Titan and its torus will stand out in energetic neutral images throughout the Cassini orbit, and thus serve as a continuous remote probe of ion flux variations near 20R S (e.g., magnetopause crossings and substorm plasma injections). The Titan exosphere and its cometary interaction with magnetospheric plasmas will be imaged in detail on each flyby. The three principal sensors of MIMI consists of an ion and neutral camera (INCA), a charge–energy–mass-spectrometer (CHEMS) essentially identical to our instrument flown on the ISTP/Geotail spacecraft, and the low energy magnetospheric measurements system (LEMMS), an advanced design of one of our sensors flown on the Galileo spacecraft. The INCA head is a large geometry factor (G ∼ 2.4 cm2 sr) foil time-of-flight (TOF) camera that separately registers the incident direction of either energetic neutral atoms (ENA) or ion species (≥5 full width half maximum) over the range 7 keV/nuc < E < 3 MeV/nuc. CHEMS uses electrostatic deflection, TOF, and energy measurement to determine ion energy, charge state, mass, and 3-D anisotropy in the range 3 ≤ E ≤ 220 keV/e with good (∼0.05 cm2 sr) sensitivity. LEMMS is a two-ended telescope that measures ions in the range 0.03 ≤ E ≤ 18 MeV and electrons 0.015 ≤ E≤ 0.884 MeV in the forward direction (G ∼ 0.02 cm2 sr), while high energy electrons (0.1–5 MeV) and ions (1.6–160 MeV) are measured from the back direction (G ∼ 0.4 cm2 sr). The latter are relevant to inner magnetosphere studies of diffusion processes and satellite microsignatures as well as cosmic ray albedo neutron decay (CRAND). Our analyses of Voyager energetic neutral particle and Lyman-α measurements show that INCA will provide statistically significant global magnetospheric images from a distance of ∼60 R S every 2–3 h (every ∼10 min from ∼20 R S). Moreover, during Titan flybys, INCA will provide images of the interaction of the Titan exosphere with the Saturn magnetosphere every 1.5 min. Time resolution for charged particle measurements can be < 0.1 s, which is more than adequate for microsignature studies. Data obtained during Venus-2 flyby and Earth swingby in June and August 1999, respectively, and Jupiter flyby in December 2000 to January 2001 show that the instrument is performing well, has made important and heretofore unobtainable measurements in interplanetary space at Jupiter, and will likely obtain high-quality data throughout each orbit of the Cassini mission at Saturn. Sample data from each of the three sensors during the August 18 Earth swingby are shown, including the first ENA image of part of the ring current obtained by an instrument specifically designed for this purpose. Similarily, measurements in cis-Jovian space include the first detailed charge state determination of Iogenic ions and several ENA images of that planet’s magnetosphere.This revised version was published online in July 2005 with a corrected cover date.  相似文献   
3.
硝酸羟胺(HAN)/1 乙基 3 甲基咪唑硫酸乙酯([Emim][EtSO4])混合离子液体推进剂具有绿色无毒、高性能、易电离的特点,既可以应用于化学推进模式,又可以应用于电推进模式,是肼类推进剂的一种理想的替代品.利用热重分析 差示扫描量热法(TGA DSC)研究了HAN/[Emim][EtSO4]离子液体推进剂的热分解和催化分解过程.研究了其在升温速率为5 K/min~15 K/min时,热分解和催化分解情况下的失重过程和放热过程.失重结果表明,该离子液体推进剂分解过程中,放热曲线表明,分解过程存在两个显著的放热过程使用催化剂可以显著地降低推进剂的分解温度和残余质量.最后,研制了推力为200 mN的模型发动机,热试车结果表明,HAN/[Emim][EtSO4]离子液体推进剂可以在催化点火条件下实现稳定启动,在空间推进领域具有良好应用前景.  相似文献   
4.
可重复使用热防护材料应用与研究进展   总被引:2,自引:0,他引:2  
可重复使用热防护系统是为高速重复使用飞行器而发展的关键性技术,涵盖了地球大气环境及非地球大气环境下的弹道式再入、高马赫数巡航等应用场景。根据现有高马赫数飞行器热防护现状,对高马赫数飞行器的主要热防护系统类型、特点和使用场景进行了简要介绍。在此基础上,结合国外里程碑式可重复使用飞行器(X-15、SR-71、航天飞机、X-33、X-37B、Spaceliner等),梳理了可重复使用热防护材料的应用与研究进展,论述了代表性可重复使用热防护材料的发展、性能、研制进度、特点及应用前景。对国外在可重复使用热防护材料研制中的设计及发展思路,以及所存在的主要问题进行了总结归纳,为可重复使用热防护材料未来的发展提供了思路。  相似文献   
5.
以M38合金作基材,先电镀Pd-20wt%Ni合金,再采用传统低温高活性(LTHA)固渗铝工艺,用NaCl作活性剂渗铝制得Pd-Ni-Al涂层。XRD和EPMA分析结果表明,涂层为固溶Ni的β-PdAl单相结构;在900℃Na  相似文献   
6.
高效离子电热水器的设计   总被引:1,自引:0,他引:1  
描述一种由AT89C2051单片机控制的高效离子电热水器,该热水器使用安全,即开即热,转换效率高。  相似文献   
7.
To illustrate the interaction of Grand Unified Theories (GUTs), supersymmetry (SUSY), and cosmology, a worked example is carried out. This example is the dark matter problem, or “What is the dominant matter of the Universe?” It is shown that if GUTs are assumed then the primordial perturbations are probably adiabatic, if inflation is assumed then Ω = 1 and GUTs first name is probably SUSY. If Ω = 1, big bang nucleosynthesis tells us that the bulk of the matter is non-baryonic. SUSY-GUTs gives us some possible candidate inos to which massive neutrinos, axion or planetary mass black holes can be added. These candidates can be classified hot (or warm) or cold types of dark matter. It is shown that hot gives Ω = 1 and naturally gives large scale structure but does not give small scale structure or galaxy formation times, whereas cold gives small scale structure and formation times but cannot easily yield Ω = 1. It is concluded that either a hybrid of both hot and cold or non-random phases for the perturbations may be needed.  相似文献   
8.
7075Al/SiCp复合材料热压缩变形的研究   总被引:1,自引:0,他引:1  
采用圆柱试样在Gleeble-1500热模拟机上对7075Al/SiCp复合材料进行高温压缩变形实验,变形温度为300-500℃,应变速率为0.001-1s^-1。结果表明:7075Al/SiCp复合材料的流变应力大小受变形温度和应变速率的强烈影响,流变应力随应变的增加而逐渐增加,出现一峰值后逐渐下降;流变应力随变形温度的升高,应变速率的降低而降低。可用Zener—Hollomon参数的双曲正弦形式来描述7075Al/SiCp复合材料高温压缩变形流变应力,其变形激活能Q为279.659KJ/mol。  相似文献   
9.
张颖哲  倪大明  Incheol LEE  林大楷  杨志刚 《航空学报》2018,39(12):122446-122446
为深入了解涡扇发动机喷流噪声特性,验证喷流噪声降噪方法,建立发动机喷流噪声数据库,在法国国家航天航空研究中心的CEPRA19声学风洞开展了缩比发动机喷嘴热喷流噪声试验测试工作。针对发动机热喷流模拟系统,设计加工了面积比(外涵喷嘴面积与内涵喷嘴面积之比)为5和7的两种喷嘴构型试验模型。通过减小高温区域单个零件长度尺寸和零件壁厚的方法,降低热膨胀对模型尺寸的影响。在声学风洞中完成了不同工况条件下两种面积比圆形喷嘴和锯齿形喷嘴的远场噪声特性测试。通过对远场测量噪声频谱进行分析,发现随着来流速度的增大喷流噪声会减小,采用锯齿形喷嘴设计在中低频喷流噪声水平降低,在高频噪声水平有所增加。  相似文献   
10.
风洞模型-支撑系统涡激振动测量与分析   总被引:1,自引:1,他引:0       下载免费PDF全文
以0.55m×0.4m低湍流航空声学风洞某模型及其支撑系统为研究对象,采用基于加速度传感器直接测量支撑系统和热线间接测量模型尾流相结合的方法,测量并分析了风洞模型-支撑系统的涡激振动模态,给出了测量方案和数据处理方法。采用基于加速度传感器的功率谱分析方法,获得了模型-支撑系统的三阶振动频率分别为31.1、120.9和221.4Hz;采用基于加速度传感器的频域滤波和频域积分方法,提高了有效信号的信噪比,获得了模型-支撑系统振动的振型和振动节点位置;采用热线测量模型尾流分离涡脱落频率的方法,获得了模型一阶和二阶振动的尾流涡激频率分别为31.1和124.1 Hz,并从测量尾流速度脉动量获得了模型振幅变化和抖振边界信息。实验结果表明,采用热线测量模型尾流从而分析模型振动的方法,有利于小尺度的模型振动测量,而且相对于加速度传感器装于模型表面的直接测量方法而言,对试验模型的绕流流场干扰较小,为测量风洞试验模型的涡激振动模态提供了一种方法。  相似文献   
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