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751.
Investigation of Surface Integrity on TC17 Titanium Alloy Treated by Square-spot Laser Shock Peening 总被引:2,自引:0,他引:2
Laser shock peening(LSP) is an innovative surface treatment method,which has been shown to greatly improve the fatigue life of many metallic components.This work investigates surface integrity of TC17 titanium alloy treated by LSP with innovative square laser spot.Nd:glass laser with duration of 30 ns and spot size of 4 mm×4 mm is applied.The surface morphology and surface residual stress of the TC17 titanium alloy,treated with varying peening parameters such as laser power density and overlapping ratio,have been studied in detail.The results show that laser pulse energy greatly influences surface morphology and surface residual stress around single-spot treated areas,and compressive residual stresses are saturated as laser pulse energy is over 55 J.There are significantly different surface morphologies and residual stress distributions at the overlapped areas with different overlapping ratios.A relative smooth surface is produced with uniform compressive residual stress distribution at an overlapping ratio of 8 %.The experiment of residual stress relaxation is implemented by measuring residual stress at the center of four overlapped spots and by four point bending fatigue test at the frequency of 105 Hz.The compressive residual stresses induced by LSP are found to relax quite slowly under cyclic fatigue loading. 相似文献
752.
倒置梯形涡流发生器与非对称超声速来流相互作用的短隔离段流动数值研究 总被引:3,自引:0,他引:3
为了有效地缩短超燃冲压发动机隔离段长度,在前期研究的等宽度平直斜楔基础上,用数值模拟的方法,研究了一种侧壁面后掠的倒置梯形涡流发生器,涡流发生器放置在隔离段进口厚附面层一侧。研究结果表明:加装倒置梯形涡流发生器后可在进出口压比相同的情况下,将隔离段长度减小40%左右,比等宽度平直斜楔多缩短5%;激波串长度随后掠角呈非线性变化,在一适当的后掠角下,激波串长度最小,它的总压恢复系数与等宽度平直斜楔处于同等水平。 相似文献
753.
754.
管内激波串振荡和壁面脉动压力特性 总被引:1,自引:0,他引:1
分析了管内激波串振荡引起的壁面压力脉动特性。采用直联风洞实验方式结合动态压力测量技术获得了矩形管道内不同激波串位置下的壁面压力分布数据,对所得压力脉动幅值、功率谱密度曲线等结果进行分析,探讨激波串流动非定常特点与引起压力脉动的机制。 相似文献
755.
采用考虑转捩的γ-Reθ湍流模型研究了高超声速复杂流动,结合PSE(parabolic stability equa-tion)稳定性分析方法和e-N方法,通过给出边界层最不稳定点的参数,用以控制γ-Reθ的转捩经验关联式,减少对经验参数的依赖.计算了锥体高超声速流场,得到的壁面换热量和边界层转捩位置与实验吻合较好.计算了平板激波/边界层干扰和高超声速拐角压缩流场,得到了准确的波系结构、压力分布和分离区的大小.结果表明,该方法与传统湍流模型相比具有较大的优越性. 相似文献
756.
MHD Flow Control of Oblique Shock Waves Around Ramps in Low-temperature Supersonic Flows 总被引:1,自引:0,他引:1
This article is devoted to experimental study on the control of the oblique shock wave around the ramp in a low-temperature supersonic flow by means of the magnetohydrodynamic(MHD) flow control technique. The purpose of the experiments is to take advantage of MHD interaction to weaken the oblique shock wave strength by changing the boundary flow characteristics around the ramp. Plasma columns are generated by pulsed direct current(DC) discharge, the magnetic fields are generated by Nd-Fe-B rare-earth permanent magnets and the oblique shock waves in supersonic flow are generated by the ramp. The Lorentz body force effect of MHD interaction on the plasma-induced airflow velocity is verified through particle image velocimetry(PIV) measurements. The experimental results from the supersonic wind tunnel indicate that the MHD flow control can drastically change the flow characteristics of the airflow around the ramp and decrease the ratio of the Pitot pressure after shock wave to that before it by up to 19. 66%, which leads to the decline in oblique shock wave strength. The oblique shock waves in front of the ramp move upstream by the action of the Lorentz body force. The discharge characteristics are analyzed and the MHD interaction time and consumed energy are determined with the help of the pulsed DC discharge images. The interaction parameter corresponding to the boundary layer velocity can reach 1. 3 from the momentum conservation equation. The velocity of the plasma column in the magnetic field is much faster than that in the absence of magnetic field force. The plasma can strike the neutral gas molecules to transfer momentum and accelerate the flow around the ramp. 相似文献
757.
758.
759.
后掠与无后掠压缩角模型产生的激波/边界层干扰的非定常特性 总被引:1,自引:0,他引:1
介绍了10个压缩角模型在M数为2.011、2.504、3.015时产生的激波/边界层干扰的非定常特性的试验研究结果.压缩角模型的流向压缩角分别为15°、20°、24°,后掠角分别为0°、20°、40°、60°.实验结果表明(a)所有无后掠压缩角和大多数20°后掠压缩角产生柱形干扰,而大后掠压缩角则产生锥形干扰;降低来流M数或增大模型后掠角有利于从柱形干扰转变为锥形干扰.(b)间隙区内的压力脉动出现低频峰值,此峰值随着模型后掠角增大或流向压缩角减小而减小;然而随着来流M数增大,此峰值在柱形干扰区减小,而在锥形干扰区略增大.对于锥形干扰,无粘激波的平均激波强度是控制其干扰特性的主要因素. 相似文献
760.