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1.
在Biot波动理论及饱和多孔热弹性波动理论基础上,引入三个松弛因子,建立了广义饱和多孔热弹性波动理论。通过对SV波在界面上的反射问题进行分析,得到了p1、p2、T及S波反射系数表达式,并利用算例对比分析了基于广义饱和多孔热弹性波动理论(G-TE)与L-S、G-L热弹性波动理论的SV波界面上反射系数的差异,讨论了松弛因子对反射系数的影响。结果表明:G-TE理论、L-S理论、G-L理论模型对p1、p2、S波反射幅值计算结果有较大的影响,且影响规律各不相同。松弛因子对p2波的影响较大,对p1波和S波的影响较小。  相似文献   

2.
单层平板吸波体界面反射模型的带宽理论研究   总被引:2,自引:0,他引:2  
为了优化和指导吸波体设计,介绍了单层平板吸波体界面反射模型,推导了模型所揭示的吸波体内部能量流动关系。在此基础上,导出吸波体反射吸收带宽计算公式,由界面反射模型得出影响吸收带宽的因素,包括吸波层厚度、1/4波长厚度在峰值频率处的变化率、指定的反射波能量、前界面反射波能量及后界面反射波能量等。利用推导的能量关系及带宽公式,对3个同轴样品进行分析计算,结果表明计算值与实验值吻合较好,带宽公式推导正确。  相似文献   

3.
分析了斜入射角条件下F-P干涉腔的透过率特性;结合单层介质膜和单层金属膜的反射特性随入射角的变化规律,得出了反射特性参数为恒定值时微腔、低反F-P干涉腔透过率的计算误差;仿真结果表明,在光束斜入射条件下,特别是在大入射角下,单层介质膜的反射率指数增大,单层金属膜的反射率和反射相移也指数增大,但其吸收系数指数减小,造成微腔、低反F-P干涉腔透过率曲线与反射特性参数为恒定值时相比均明显向下偏移,且偏移量逐渐增大。  相似文献   

4.
为研究非对称结构战斗部的破片飞散特性,利用斜激波理论对爆轰波作用于壳体表面的过程进行研究,并利用自由面速度倍增定律对波在自由面反射后质点速度的计算进行简化,得到了破片飞散角的计算模型。利用D型战斗部试验数据对计算模型进行验证,结果表明,斜激波理论计算得到的破片飞散与试验结果吻合很好;当入射角较小时,壳体飞散角与入射角成线性关系。  相似文献   

5.
为了避免采用金属频率选择表面制备的天线罩中存在的热残余应力和弱黏接界面等问题,采用与聚合物基复合材料罩壁结构相容性好的碳纤维增强聚合物基复合材料制备频率选择表面,利用自由空间法对试样的电磁传输性能进行测试,并采用数值分析模型对碳纤维复合材料频率选择表面的电磁传输机制和电磁传输影响因子进行分析。结果表明:碳纤维复合材料频率选择表面具有频率选择功能,但谐振频率处的电磁传输损耗较大;通过改变复合材料频率选择表面的单元缝隙率、厚度、电导率以及介电常数可以实现对其电磁传输性能的调节。  相似文献   

6.
热射流起爆过程的数值模拟   总被引:1,自引:0,他引:1       下载免费PDF全文
采用改进的化学非平衡流解耦方法处理Euler反应流方程,并以H2/air 9组分21方程模型对竖直喷注的热射流起爆过程进行了二维数值模拟。对流项采用五阶WENO离散格式,时间推进采用二阶Runge-Kutta方法。详细分析了热射流以不同速度、入射位置、入射宽度和入射倾角喷射时在爆震管内形成的流场,总结了射流参数状态影响起爆的一般规律;解释了激波、火焰的相互作用对"热点"的形成以及转变为爆震的影响,特别是激波反射对"热点"形成的促进作用。结果表明,爆震波通常由火焰面和固壁附近狭长未燃区域中的"热点"产生。"热点"向爆震波发展的过程是过驱爆震阶段,存在三波结构。为了实现快速起爆,应当增大射流入射速度、贴近侧壁并以适当入射角度喷射热射流。  相似文献   

7.
在海浪波数测量无误差的假设下,证明了最小二乘法是高斯白噪声背景下海表面流的最大似然估计和最小方差无偏估计的有效方法;推导了估计误差克拉美-罗限的闭式解。在此基础上,分析了影响估计质量的相关因素,结果表明:海表面流估计误差由反演所用真实海浪谱值点数、频率测量误差、海浪波数波向及其分布特性等决定;为提高海表面流估计精度,需要尽可能多地获取具有一定波数和波向扩展性的真实海浪回波谱值点。  相似文献   

8.
电缆负载射频电磁辐射响应规律研究   总被引:2,自引:0,他引:2  
采用基于有限积分法的电磁仿真软件CST建立等幅正弦波辐照条件下同轴电缆电磁耦合响应模型,研究终端负载电阻及电缆长度对终端响应电压的影响规律。结果表明,随着终端负载电阻的增大,响应电压逐渐增大,而后趋于稳定;不同频率条件下,电缆长度在一个波长范围内,电缆负载响应电压幅值先是随着电缆长度的增加而变大;达到最大值后,随着长度的增加,响应幅值反而减小。  相似文献   

9.
1.引言高能激光脉冲辐照金属材料时,烧蚀掉表面一薄层材料。汽化金属迅速喷出,由于动量守恒,在固态材料中引起一个热激波。热激波传播到自由表面,形成反射稀疏波。材料中的峰值负压强P_-可能达到材料的抗拉强度二而出现层裂破坏。我们提  相似文献   

10.
为研究管道弯头对非轴对称弯曲波传播特性的影响,采用数值模拟方法研究了不同方向F(1,1)模态导波在弯头处的模态转换和散射特性。研究结果表明:不同方向的F(1,1)模态导波会产生不同的模态转换,其与弯头拱背-拱腹的夹角越大,模态转换程度越大,而夹角为0°时无模态转换产生;弯头会改变F(1,1)模态导波的方向并对散射F(1,1)模态导波幅值产生影响;不同于轴对称导波,影响弯曲波在弯头处反射和透射系数的因素除了弯曲半径和频率外,还有弯曲波激励角度。  相似文献   

11.
《防务技术》2020,16(2):493-501
In order to improve the underwater acoustic target strength of corner reflectors, according to the principle of acoustic impedance mismatch of the boundary layer, the method of using air cavity to increase the underwater acoustic target strength of corner reflectors is proposed. The acoustic reflection coefficients of underwater air layer and single layer metal sheet are calculated and compared. The results show that the reflection coefficient of single layer metal sheet is greatly affected by frequency and incidence angle, and the reflection coefficient of air layer in water is large and little affected by frequency and incidence angle. On this basis, a new kind of airfilled cavity corner reflector is designed. The acoustic scattering characteristics of underwater airfilled cavity corner reflector are calculated cumulatively, and the results are compared with the monolayer metal sheet corner reflector. The simulation results show that the acoustic reflection effect of the airfilled cavity corner reflector is better. In order to verify the correctness of the method, the test was carried out in the silencing tank. The experimental results show that the simulation results are in good agreement with the experimental results, and the airfilled cavity can improve on acoustic reflection performance of the underwater corner reflector.  相似文献   

12.
为探究有限水深环境下自由面兴波在远场的传播特性,应用线性水动力学的基本理论,从有限水深Kelvin源格林函数的积分表达式中提取相函数,采用同相分析法求得亚临界和超临界速度区下远场传播波系的等相线。结果表明,水深傅汝德数Fh1时远场传播波包括横波和散波两个波系,F_h1时远场波系仅由散波构成,点源兴波的影响范围可由Kelvin角的大小确定,当F_h趋近于1时Kelvin角迅速增大至90°。依据船型要素、两船相对位置和池壁几何参数,并计及船模的定常兴波经池壁反射作用后对自身和另一船模的干扰,提出了有限水深条件下并行航行两船模池壁效应的判别方法,并结合实例检查分析了某试验工况下的池壁效应。  相似文献   

13.
采用船舶单自由度横摇运动方程,以及纵摇与垂荡耦合摇荡运动方程,数值模拟了规则波浪中船舶操纵响应不规则摇荡运动现象。假定波浪中船舶遭遇频率具有谐波分量形式,定义了遭遇频率常量、强度和散射频率,提出了船舶遭遇频率频散概念,推导了遭遇频率的频散关系,分析得到了航速和浪向角度变化引起的两种频散机制。散射机制表明:顶浪航行时航速散射效率最高,正横浪航行时航向角散射效率最高。  相似文献   

14.
通过实验数据与理论计算结果的对比,分析了气流对振动系统的阻尼作用;并以实验声源为基础,以等效电路方法分析了调制气流声源振动系统的弹性系数、磁感应强度、音圈质量、电阻、电感以及绕线方式等参数对音圈振幅的影响;根据调制气流声源的用途差异,提出了用于语音广播和产生大功率低频声波时振动系统各参数的选择方法.  相似文献   

15.
The formation mechanism of an EFP(explosively formed projectile) using a double curvature liner under the overpressure effect generated by a regular oblique reflection was investigated in this paper.Based on the detonation wave propagation theory,the change of the incident angle of the detonation wave collision at different positions and the distribution area of the overpressure on the surface of the liner were calculated.Three-dimensional numerical simulations of the formation process of the EFP with tail as well as the ability to penetrate 45# steel were performed using LS-DYNA software,and the EFP ve-locity,the penetration ability,and the forming were assessed via experiments and x-ray photographs.The experimental results coincides with those of the simulations.Results indicate that the collision of the detonation wave was controlled to be a regular oblique reflection acting on the liner by setting the di-mensions of the unit charge and maintaining the pressure at the collision point region at more than 2.4 times the CJ detonation when the incident angle approached the critical angle.The distance from the liner midline to the boundary of the area within which the pressure ratio of the regular oblique reflection pressure to the CJ detonation pressure was greater than 2.5,2,and 1.5was approximately 0.66 mm,1.32 mm,and 3.3 mm,respectively.It is noted that pressure gradient caused the liner to turn inside out in the middle to form the head of the EFP and close the two tails of the EFP at approximately 120μs.The penetration depth of the EFP into a 45# steel target exceeded 30 mm,and there was radial expansion between the head and tail of the EFE increasing the penetration resistance of the EFP.Therefore,the structural size of the unit charge and the liner can be further optimized to reduce resistance to increase the penetration ability of the EFP.  相似文献   

16.
航空轮胎用橡胶弹性体在服役过程中遭受严苛的动态循环工况。为了研究弹性体在此工况下的力学响应特征和损伤机理,提出基于应力波作用的Mullins效应动态加载实验方法。根据应力波传导与作用特征,采用Hopkinson压杆加载思路,设计和配置了各单元尺寸参数,进而搭建可用于橡胶弹性体材料动态循环加载的实验系统,并开展了航空轮胎用丁苯橡胶的动态循环加载试验。基于试验信号分析发现:加载系统实现了弹性体材料Mullins效应动态应变递增的试验加载。最后开展加载测试参数的影响因素分析,结果表明通过优化系统各单元可实现Mullins效应的动态加、卸载参数的控制。  相似文献   

17.
Recent researches focused on developing robust blast load mitigation systems due to the threats of terrorist attacks. One of the main embraced strategies is the structural systems that use mitigation techniques. They are developed from a combination of structural elements and described herein as conventional systems. Among the promising techniques is that redirect the waves propagation through hollow tubes. The blast wave propagation through tubes provides an efficient system since it combines many blast wave phenomena, such as reflection, diffraction, and interaction. In this research, a novel blast load mitigation system, employed as a protection fence, is developed using a technique similar to the technique of the bent tube in manipulating the shock-wave. The relative performance of the novel system to the conventional system is evaluated based on mitigation percent criteria. Performances of both systems are calculated through numerical simulation. The proposed novel system proved to satisfy high performance in mitigating the generated blast waves from charges weight up to 500 kg TNT at relatively small standoff distances (5 m and 8 m). It mitigates at least 94% of the blast waves, which means that only 6% of that blast impulse is considered as the applied load on the targeted structure.  相似文献   

18.
一种随机海洋波模型及其数字仿真   总被引:1,自引:0,他引:1       下载免费PDF全文
介绍了一种随机海洋波谱模型,分析了波谱模型中的波幅计算的三种频率谱函数。针对不同海风条件(风速和风向),对模型进行了仿真和比较。数字仿真结果表明:该模型较好地反映了随机海洋表面的动力学特性,运用该模型可以得到随机变化海浪的逼真的仿真图像  相似文献   

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