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51.
本文采用二维电磁场有限元法及磁路的简化计算法对15cm×15cm磁悬挂天平系统(MSBS)的阻力线圈间距、磁场的分布情况进行了分析计算,并与测试结果进行了分析比较,给出了15cm×15cm磁悬挂天平系统(MSBS)的结构方案。 相似文献
52.
提出一种计算复杂目标高频区RCS的实用方法。首先采用3DStudioMax对装甲车进行三角面元模拟,然后运用路德维格积分[1]和物理绕射理论(PTD)计算目标的雷达散射截面积,通过对方柱RCS的计算,验证了所提方法的有效性,最后给出了C波段和X波段不同极化的装甲车和坦克RCS的方位分布图。 相似文献
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Nano-sized aluminum(Nano-Al)powders hold promise in enhancing the total energy of explosives and the metal acceleration ability at the same time.However,the near-detonation zone effects of reaction between Nano-Al with detonation products remain unclear.In this study,the overall reaction process of 170 nm Al with RDX explosive and its effect on detonation characteristics,detonation reaction zone,and the metal acceleration ability were comprehensively investigated through a variety of experiments such as the detonation velocity test,detonation pressure test,explosive/window interface velocity test and confined plate push test using high-resolution laser interferometry.Lithium fluoride(LiF),which has an inert behavior during the explosion,was used as a control to compare the contribution of the reaction of aluminum.A thermochemical approach that took into account the reactivity of aluminum and ensuing detonation products was adopted to calculate the additional energy release by afterburn.Combining the numerical simulations based on the calculated afterburn energy and experimental results,the param-eters in the detonation equation of state describing the Nano-Al reaction characteristics were calibrated.This study found that when the 170 nm Al content is from 0%to 15%,every 5%increase of aluminum resulted in about a 1.3%decrease in detonation velocity.Manganin pressure gauge measurement showed no significant enhancement in detonation pressure.The detonation reaction time and reaction zone length of RDX/Al/wax/80/15/5 explosive is 64 ns and 0.47 mm,which is respectively 14%and 8%higher than that of RDX/wax/95/5 explosive(57 ns and 0.39 mm).Explosive/window interface velocity curves show that 170 nm Al mainly reacted with the RDX detonation products after the detonation front.For the recording time of about 10 μs throughout the plate push test duration,the maximum plate velocity and plate acceleration time accelerated by RDX/Al/wax/80/15/5 explosive is 12%and 2.9 μs higher than that of RDX/LiF/wax/80/15/5,respectively,indicating that the aluminum reaction energy significantly increased the metal acceleration time and ability of the explosive.Numerical simulations with JWLM explosive equation of state show that when the detonation products expanded to 2 times the initial volume,over 80%of the aluminum had reacted,implying very high reactivity.These results are significant in attaining a clear understanding of the reaction mechanism of Nano-Al in the development of aluminized explosives. 相似文献
56.
根据质点弹道的特点, 描述了弹目间距、弹炮间距和相对弹道高 3个弹道环境信息的概念, 然后应用数学方法对弹目间距、弹炮间距和相对弹道高进行了理论计算推导, 建立了数学解算模型, 并用MATLAB程序进行了数值仿真计算, 通过分析其数值变化的规律和特点提出了其应用方向。 相似文献
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航空发动机可以对空气增压,并且增加气流温度,理论上存在应用于超声速引射系统的可能。分析了气源对引射器性能的影响以及引气对航空发动机的影响,介绍了3种航空发动机在超声速引射系统中可能的布局方案。针对某领域内的排气参数要求,分别对3种布局方案进行了计算分析。计算结果表明,当上游气体压强为0.044×105 Pa和0.029 3×105 Pa时,通过合理选择发动机的布局以及工作参数,发动机可以直接将上游气体排出或者作为驱动气源应用于超声速引射系统。 相似文献
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根据Agrawal理论,建立平行双线式电火工品的传输线模型,通过仿真计算分析外界电磁场和电火工品各物理参数对负载端感应电流大小的影响,为电火工品的射频安全性研究提供一定的参考. 相似文献
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为有效解决传统载荷设计方法中存在的诸多不足,提出一种适用于一类飞行器载荷设计的三分段法,即分段刚度、分段质量和分段气动。该方法能够很好地逼近飞行器的真实质量分布和气动载荷分布。针对简化飞行器,分别利用三分段法、理论计算法和质量分站法计算其模态参数和截面载荷。结果表明,三分段法和理论计算法在模型参数、计算原理上是一致的,基本可以认为是一种方法,因而它们的模态参数和截面载荷完全吻合;质量分站法所得左、右截面载荷不一致,且相差很大,还不符合真实载荷情况。总之,采用三分段法能够得到较为真实、合理的飞行器截面载荷分布,且工程应用简便,方法合理、可信,同时还可以在很大程度上降低飞行器载荷设计和结构设计的难度。 相似文献
60.
《防务技术》2020,16(1):96-106
The numerical simulation of a blast wave of a multilayer composite charge is investigated. A calculation model of the near-field explosion and far-field propagation of the shock wave of a composite charge is established using the AUTODYN finite element program. Results of the near-field and far-field calculations of the shock wave respectively converge at cell sizes of 0.25–0.5 cm and 1–3 cm. The Euler––flux-corrected transport solver is found to be suitable for the far-field calculation after mapping. A numerical simulation is conducted to study the formation, propagation, and interaction of the shock wave of the composite charge for different initiation modes. It is found that the initiation mode obviously affects the shock-wave waveform and pressure distribution of the composite charge. Additionally, it is found that the area of the overpressure distribution is greatest for internal and external simultaneous initiation, and the peak pressure of the shock wave exponentially decays, fitting the calculation formula of the peak overpressure attenuation under different initiation modes, which is obtained and verified by experiment. The difference between numerical and experimental results is less than 10%, and the peak overpressure of both internal and external initiation is 56.12% higher than that of central single-point initiation. 相似文献