首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 62 毫秒
1.
水下爆炸过程是一个非常复杂的过程,大体上分为3个阶段:炸药的爆轰、冲击波的传播、气泡脉动。爆炸所产生的冲击波、气泡和脉动水流,都能使目标受到一定程度的破坏。在多数情况下,冲击波的破坏起着决定性的作用,脉动水流和气泡(爆轰产物)一般引起附加的破坏作用。  相似文献   

2.
将爆轰产物状态方程与气泡运动方程相结合,提出了一种水下爆炸气泡脉动周期的数值计算方法,能够快速计算不同炸药水下爆炸的气泡脉动周期。结果表明:采用JWL状态方程与采用γ律状态方程的气泡周期计算方法相比,前者计算TNT炸药水下爆炸气泡脉动周期的误差更小,计算误差小于3%;通过对比RS211炸药水下爆炸实验结果,进一步验证了该数值计算方法对含铝炸药水下爆炸气泡脉动周期的计算同样具有良好的适用性。  相似文献   

3.
含铝炸药水下爆炸性能的实验研究   总被引:3,自引:0,他引:3       下载免费PDF全文
对RS211、HL-1、HL-2这3种含铝炸药和TNT炸药进行了水下爆炸实验,测量了4种炸药水下爆炸冲击波压力剖面和气泡脉动周期,获得了4种炸药水下爆炸冲击波的峰值超压、冲量、能量和气泡能。实验结果表明,在所研究的范围内,与TNT炸药相比,含铝炸药的冲击波能量有明显增加,约为TNT炸药的1.20~1.35倍,气泡能有显著增加,约为TNT炸药的1.50~2.30倍,表明在炸药中加入铝粉对于提高炸药水中爆炸威力是有益的。  相似文献   

4.
为研究铝箔膜炸药的爆炸性能,将铝箔膜与RDX炸药均匀混合并压制成型,得到高铝含量的铝箔膜炸药,与铝粉炸药形成对比,进行水下爆炸实验。通过实验测得两种炸药在不同距离处的冲击波压力时程,分析冲击波压力峰值、冲量、比冲击波能、气泡脉动周期、比气泡能和总能量等主要参数的差异。研究表明:铝箔膜炸药压力峰值的衰减速率低于铝粉炸药,冲量和比冲击波能与铝粉炸药相当;由于铝箔膜的比表面积比铝粉小,纯度相对较高,气泡脉动周期相对较长,因此铝箔膜炸药的比气泡能乃至总能量均略高于铝粉炸药。  相似文献   

5.
将纯铝用熔喷法制成铝纤维添加到炸药中,得到新型非理想混合炸药,通过水中爆炸实验,测试不同位置铝纤维炸药的压力时程曲线。对压力时程曲线进行分析,计算得到水下不同位置铝纤维炸药的冲击波压力峰值、冲量、冲击波能和气泡能。结果表明:铝纤维炸药的压力时程曲线可采用指数函数与双曲线函数进行分段描述,而用正态分布函数拟合气泡脉动压力曲线的效果不理想;铝纤维炸药水下爆炸比气泡能与总能量的比值为52%~58%,说明向基体炸药RDX中添加铝纤维对总能量有影响;总能量与爆热的比值为75%~85%,小于理论近似值(100%),说明铝纤维炸药爆炸时铝纤维反应不完全且破碎铝纤维消耗了一定的能量。  相似文献   

6.
为了系统地研究铝氧比对含铝炸药水下爆炸载荷及能量输出结构的影响,在验证数值模型有效性的基础上,针对铝氧比分别为0、0.16、0.36、0.63的RDX基含铝炸药,利用耦合欧拉-拉格朗日方法模拟了其水下爆炸连续的全过程,考虑了冲击波载荷和气泡载荷之间的耦合作用,从冲击波、气泡和能量输出结构三方面对影响效应进行评估。计算结果表明:随着铝氧比的增大,含铝炸药水下爆炸冲击波衰减时间常数、冲击波冲量、气泡脉动周期、气泡最大半径以及比气泡能都增大;铝氧比为0.36时,冲击波峰值压力、冲击波能流密度和比冲击波能达到最大。铝粉的加入对气泡能的提高相对于冲击波能更加显著。  相似文献   

7.
一种水中爆炸气泡脉动实验研究方法   总被引:1,自引:0,他引:1       下载免费PDF全文
 在2 m×2 m×2 m的实验水箱中开展小当量PETN炸药水中爆炸气泡脉动实验时,利用弹性波从声阻抗高的物质传入声阻抗低的物质时的“减震缓冲”原理,采用在水箱壁贴低声阻抗材料的方法,有效降低了水箱壁反射冲击波对气泡脉动过程的影响,获得了清晰的气泡脉动过程图像、气泡水射流形成过程图像和气泡脉动压力曲线。将水箱实验结果与8 kg TNT当量爆炸水池实验结果对比,得到的最大相对误差仅为5.1%,验证了水箱实验方法的准确性,为炸药水中爆炸气泡脉动现象研究提供了一种简便有效的实验方法。  相似文献   

8.
杨莉  汪玉  黄超  汪斌 《高压物理学报》2012,26(5):545-550
通过开展装药沉底爆炸原理性实验研究,得到了不同水底条件对装药沉底爆炸气泡运动和冲击波压力的影响规律:沉底装药水下爆炸气泡通常呈半球形,依附在水底并同时急剧膨胀达到最大半径,随后气泡做收缩运动并连带水底介质颗粒迅速上浮,同时形状发生显著变化,如在石底和泥底时气泡在水底射流的作用下呈蘑菇状上浮,砂底时气泡则呈现出柱状上浮、未出现明显脉动运动即已坍塌破裂;沉底爆炸与水底介质发生强烈耦合作用而形成不同程度的反射波,通常水下石底的反射冲击波较泥底和砂底更强烈,且一般迭加后的冲击波峰值压力高于入射波阵面压力;不同水底介质条件下,装药与水底发生的强烈耦合作用均对水底造成强冲击破坏。  相似文献   

9.
为研究港池环境近水面水下爆炸载荷及其对码头结构的损伤特性,设计了一种典型码头结构,并构建港池环境,运用LS-DYNA程序开展水下爆炸数值模拟研究,对爆炸现象、荷载特性、结构动态响应和能量吸收特性4个方面进行了详细研究,分析了边界、比例爆距等参数的影响规律。结果表明:爆炸气泡脉动主要受到码头结构边界和水面的影响,水底和有限港池内的流体运动对其亦有一定影响;冲击波荷载以比例爆深为中心呈垂向对称分布,气泡脉动荷载主要分布于比例爆深以下位置;结构变形和毁伤主要在冲击波传播阶段形成,气泡脉动和射流的二次毁伤效果较弱;混凝土和沉箱内填土是主要能量吸收部分。  相似文献   

10.
 采用高速摄影方法在实验水箱中获得了长径比为3.35~6.75的柱形PETN炸药水中爆炸气泡脉动的图像,进而结合真实的爆轰过程和Rayleigh气泡运动方程,研究了气泡的形态演变规律。研究结果表明,柱形装药在水中爆炸时,形成的初始气泡的形状为非球对称形,这种非对称特征随长径比的增加而增大。气泡表面的运动也表现出明显的非球对称特征,气泡表面在装药径向的膨胀运动呈指数衰减,在装药轴向两端的膨胀运动更接近于分段线性衰减。气泡表面的不对称运动与柱形装药水下爆炸的能量输出结构不均有关,与冲击波的有效能量分布规律是相似的。  相似文献   

11.
王会  贾富国  韩燕龙  张亚雄  曹斌 《物理学报》2017,66(1):14501-014501
料仓卸料过程中的颗粒脉动会引起料仓振动甚至导致结构失效.为了明晰颗粒脉动特征,本文进行了椭球颗粒在不同半锥角深仓的模拟卸料实验,将料仓圆筒部划分为4个固定区域以研究区域内颗粒的运动信息,分析了料仓圆筒部颗粒系统的运动特征.研究结果表明:整个卸料过程颗粒速度始终处于波动变化中,卸料前期表现为大振幅、周期性的剧烈脉动,卸料后期平均速度的变化则是小振幅无规律的波动;剧烈脉动时段各区域的颗粒层平均受力的变化规律与颗粒速度脉动特征相似,越接近储料顶端颗粒脉动振幅越大,表现出更规律的周期性脉动,相邻颗粒层间的脉动波形相似且周期相同,剧烈脉动过程中顶面颗粒呈周期性的自由落体运动,该时段内顶层颗粒每一次的自由落体运动都会引起该范围内颗粒间接触力消失;料仓半锥角越小时剧烈脉动频率越高、振幅越大且脉动持续时间也越长,卸料速度越稳定,且颗粒速度不会出现带有上升趋势的波动.研究结果可为卸料设备的安全设计提供参考.  相似文献   

12.
Lingling Zhang 《中国物理 B》2022,31(4):44303-044303
The pulsations and translations of cavitation bubbles obey combined ordinary differential equations, and their nonlinearities are studied by the bifurcation diagram and the phase diagram in a strong ultrasonic field. Bubble pulsation can change regularly or irregularly with changing driving pressure in the time domain. The bifurcation diagrams of the pulsation versus driving pressure show that the pulsations and translations of bubbles have nonlinear characteristics, and the nonlinear translations of bubbles can disorder the pulsations for certain parameters. Disorder of the pulsation can also be caused by nonlinear pulsation itself. In addition, the phase diagrams also show that the nonlinear translations make a large contribution to the pulsations. The same result can also be obtained when the ambient radii of two bubbles are different.  相似文献   

13.
Ying Han 《中国物理 B》2022,31(7):74208-074208
We have numerically and experimentally observed the soliton pulsation with obvious breathing behavior in the anomalous fiber laser mode-locked by a nonlinear polarization rotation technique. The numerical study of the soliton pulsation with breathing behavior was analyzed through the split-step Fourier method at first, and it was found that the phase difference caused by the polarization controller would affect the breathing characteristics. Then, taking advantage of the dispersive Fourier transform technique, we confirmed the breathing characteristic of soliton pulsation in the same fiber laser as the simulation model experimentally. These results complement the research on the breathing characteristic of soliton pulsation.  相似文献   

14.
四频差动激光陀螺中的粒子数脉动效应   总被引:1,自引:0,他引:1  
杨建强  王国臣 《应用光学》2009,30(4):692-696
为研究激光陀螺精细模耦合作用,考虑了增益介质中的粒子数脉动效应.从激光器物理原理出发,分析了粒子数脉动效应的产生机制,结合四频差动激光陀螺特点,得出粒子数脉动效应是一种精细模耦合效应,不同激光模式间的拍频使增益介质中粒子数布居差产生调制,进而对模耦合产生影响.数值计算了粒子数脉动在耦合效应中的大小.计算结果表明:粒子数脉动效应和其他耦合效应随腔频变化基本一致,在大多数腔频范围内数值较小,为其他耦合效应的4%以下;在某些腔频范围(如0.37<ξ<0.46,0.02<ξ<0.06,0.86<ξ<0.88)有较大数值,为其他耦合效应的80%以上,在激光陀螺的模耦合分析中不可忽略.  相似文献   

15.
电子束在等离子体微波器件中的脉动   总被引:1,自引:0,他引:1       下载免费PDF全文
 对填充等离子体漂移空间小脉动电子束进行了近似分析,对大脉动电子束进行了较精确的计算,结果表明虽然α区和β区束的脉动性能各不相同,但幅度和波长均受限于电子入射的初始条件和等离子体参数,当其它条件给定后存在一最佳等离子体填充密度。  相似文献   

16.
Subordinating regular diffusion – namely, Brownian motion – to random time flows generated by Lévy noises may result in anomalous diffusion. Motivated by this phenomena, and by the recent interest in the phenomena of blinking in various physical systems, we explore the subordination of regular stochastic pulsation – namely, Poisson process – to random time flows generated by Lévy noises. We show that such subordination may yield, analogous to the case of diffusion, anomalous pulsation. Anomalous pulsation displays the following anomalous behaviors, which are impossible in the case of regular pulsation: (i) simultaneous emission of multiple pulses; (ii) non-linear local pulsation rates; (iii) clustering of pulsation epochs.  相似文献   

17.
The pulsation and translation of two cavitation bubbles are studied numerically in sound field. The results show that bubbles' pulsation driven by the sound makes them translate. Different pulsations lead to different translations. Two bubbles will be mutually attractive to each other if they pulsate in phase, while they will be repulsive if out of phase. Furthermore,the secondary Bjerknes force for small phase difference is attractive, and it becomes repulsive for other phase differences up to π phase difference due to the nonlinear effect, although the attractive strength between two bubbles is much larger than the repulsive strength. Finally, one bubble pulsation and the other bubble stationary make the bubbles repel each other.  相似文献   

18.
This paper mainly focuses on the nonlinear pulsation of a bubble near the rigid wall. Dynamics of near-wall bubble and free bubble are discussed and compared in details. Investigation reveals as the driving acoustic pressure amplitude increases, nonlinear pulsation of bubble becomes intense gradually. Besides, decreasing the viscosity of host liquid is advantageous for the nonlinear pulsation of bubble. Bifurcation diagrams of bubble radius show acoustic reflection of the rigid wall makes the initial bifurcation appear at low driving acoustic amplitude and on bubble with small ambient radius, and makes the bifurcation still exist for bubble in high-viscosity liquids. That indicates the rigid wall will produce enhancement on the nonlinearity of nearby bubble. As the bubble approaches the wall, the enhancement becomes strong. Moreover, research on the influence of driving frequency shows the rigid wall makes the frequency band corresponding to chaos around the resonant frequency of free bubble shift downward.  相似文献   

19.
孙军强  黄德修 《光学学报》1996,16(9):237-1240
在实验中观察到了掺铒光纤激光器中自脉冲,并通过加反馈的方法控制了自脉冲。在理论上利用带反馈的两激光器的耦合模型,成功地解释了自脉冲的产生及其控制的物理机制。结果表明,掺铒光纤激光器中两正交偏振态的反馈及其耦合对光脉冲的形成及控制的重要性。  相似文献   

20.
In this paper, the cavitation performance and corresponding pressure pulsation, noise and vibration induced by the choked cavitating flow in a Venturi reactor are investigated experimentally under different cavitation conditions by using high-speed camera and high frequency sensors. Based on the instantaneous continuous cavitation images, the Proper Orthogonal Decomposition (POD), a tool to analyze the large-scale cavitation flow structure, is applied to investigate the choked cavitating flow dynamics. The POD results show that two mechanisms, re-entrant jet flow mechanism and shock wave mechanism, govern the shedding and collapse of cavitation cloud at different pressure ratios. These mechanisms contribute to the variation of pressure pulsation, noise and vibration at different pressure ratios. The pressure pulsation spectrum behaves differently in various cavitation regions induced by the choked cavitating flow. Due to the existence of low pressure in re-entrant region, the influence of high frequency fluctuation on pressure pulsation caused by re-entrant flow is small. Moreover, with the increase of pressure ratio, the induced noise and vibration intensity decreases gradually, then increases and reaches a maximum value. Finally, it drops to a low and stable level. Despite different inlet pressures, the intensity of cavitation noise and vibration reaches the maximum value at the same pressure ratio. Specifically, the FFT analysis of noise and vibration signals indicates that low frequency component prevails at small pressure ratio owing to the re-entrant jet mechanism, while high frequency component prevails at large pressure ratio owing to the shock wave mechanism. The relationship between the choked cavitation dynamics and the induced pressure pulsation, noise and vibration in the Venturi reactor is highlighted. The results can provide guidance for the optimal operation condition of the Venturi reactor for cavitation applications such as water treatment.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号