共查询到19条相似文献,搜索用时 93 毫秒
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为研究垂直边界面对水下爆炸气泡脉动的影响,根据势流理论建立了垂直边界面奈件下水下爆炸气泡运动的理论模型,编制计算程序进行求解。对水下爆炸气泡脉动运动的特点、流场的速度及压力的分布、气泡引起的栽荷形式进行了分析,结果表明,此模型能够反映水下爆炸气泡和周围流体介质的运动规律,并能进行定量的计算。 相似文献
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基于MSC.DYTRAN非线性有限元软件建立炸药爆轰与冲击波传播的一维有限元模型,通过与冲击波压力峰值经验公式对比,验证模型的正确性。将一维数值计算结果映射到三维流场中以确定气泡运动的初始条件,开发定义流场初始条件与边界条件的子程序,对近刚性壁面气泡运动过程进行仿真分析,通过与实验结果的对比,验证三维数值计算模型的正确性。以此为基础,研究刚性面角度以及距离参数对气泡运动、射流角度、速度的影响规律,计算模型、方法及结果对相关的工程研究和计算具有一定参考价值。 相似文献
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《中国测试》2019,(12):138-145
数值模拟是研究水下爆炸非常重要的一种方式,但由于爆炸试验条件的限制,许多数值计算缺少试验背景,从而降低了数值结果的普适性。该文以离心机水下爆炸试验为基础,验证水下爆炸理论基础-相似准则在数值计算上的合理性,通过多模型工况下的计算结果对比,研究影响水下爆炸数值计算精度的相关参数,并提出取值建议,最后将数值计算结果与水下爆炸试验结果相结合,共同验证在水下爆炸中冲击波及气泡脉动规律。结果表明:水的多项式状态方程计算出的冲击波峰值较Shock状态方程小,水的状态方程对气泡脉动影响不大;当一次项人工粘性系数小于0.02时,峰值增加已不明显。人工粘性系数对气泡脉动影响不大;二维模型下,测点的爆距越大,要到达计算精度要求,需要的网格尺寸越小。三维模型下,当网格尺寸取与炸药半径相近的尺寸时,能很好地模拟气泡脉动的全周期,且与试验数据的误差最小。 相似文献
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为了研究舰船在水下近场爆炸作用下的整体毁伤模式,根据相似原则设计了两种箱形梁模型,将TNT炸药置于模型中部正下方爆炸,通过改变爆距和药量来研究试验模型在不同爆炸工况下的整体运动特性,并利用高速摄影仪观察模型的动态响应过程.试验研究发现:在梁模型一阶湿频率与气泡脉动频率相近的条件下,气泡脉动会激起结构明显的整体弯曲运动;当爆距与最大气泡半径之比为1~1.5时,梁结构会发生中垂破坏,形成一个或两个塑性绞;当爆距与最大气泡半径之比为2~4时,梁结构会发生鞭状运动响应;水下爆炸气泡对水面结构的整体毁伤作用大于初始冲击波。 相似文献
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William G. Szymczak Steven L. Means Joel C.W. Rogers 《Journal of Engineering Mathematics》2004,48(3-4):375-389
The impact of a water jet onto a water surface can entrain air-bubbles whose pulsations provide acoustic sources. Such impacts can occur during the breaking of a wave, or on a smaller scale, when a raindrop strikes a puddle of water. A better understanding of this phenomenon can lead to improved characterizations of the ambient noise and acoustic detection algorithms. Liquid on liquid impacts correspond to a breakdown of classical hydrodynamic theory which assumes that the free surface remains smooth and topologically invariant. A computational model using a generalized theory of hydrodynamics designed to rigorously treat liquid collisions is described in this paper. Numerical simulations are compared to experiments of a liquid cylinder impacting a still-water surface The simulations provide details not only of the initial formation of the air-entrained bubble at the time of the cavity collapse, but also the subsequent pulsations of this bubble until it rises back to the free surface. Computed initial bubble sizes and natural frequencies are compared to the experimental results for different cylinder lengths. 相似文献
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The motions of a gas bubble in proximity to a free surface with and without buoyancy force, as well as in shallow water are simulated based on a numerical time integration coupled with three-dimensional boundary integral spatial solution. The fluid is assumed to be inviscid, incompressible, and the flow irrotational. The unsteady Bernoulli equation is applied on the free surface and bubble surface as one of the boundary conditions of the Laplace equation for the potential. Improvements have been made in the mesh generation of the free surface and rigid boundary, the modeling of the toroidal bubble after the jet impact and the investigation into the combined effects on the motion of a bubble in the presence of the rigid bottom and free surface. The growth and collapse of a gas bubble together with the formation of the toroidal bubble after the jet impact are simulated. The shapes and positions of the bubble, the trajectories and velocities of the poles of the bubble as well as the pressure distributions in the fluid under different standoff distances and buoyancy parameters are obtained to better illuminate the mechanism underlying the motions of gas bubble and free surface. When a bubble is initiated sufficiently close to a free surface, the free surface spike and the second accelerating phenomenon of the free surface during the collapse phase can be observed. The buoyancy force has significant effects on the jet formation and development within the bubble and it may reverse the direction of the liquid jet when exceeding the effect of the Bjerknes force induced by the free surface. The large contortions in the shallow water and the formation of the high-pressure region between the bubble and the free surface are captured when the bubble is close enough to the rigid bottom and the free surface. 相似文献
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利用AUTODYN软件模拟PETN药柱和TNT球形装药水下爆炸气泡脉动的过程,分析了脉动周期与最大半径随装药量、爆炸深度的变化规律。结果表明:当炸药所处的爆炸深度一定时,气泡膨胀最大半径与初始半径的比值、气泡脉动周期与初始半径的比值均为一个定值;一定质量的TNT装药水下爆炸时,气泡最大半径随爆炸深度呈指数形式变化且该变化规律与装药量无关;在不考虑重力的影响下,装药的爆炸深度一定时,当装药的初始半径成倍增加时,气泡脉动最大半径亦成相同倍数增加。 相似文献
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壁面与自由液面联合作用下,气泡的动态特性与单独一个边界条件作用时相比要复杂很多,难于从理论角度分析探讨。为深入探究壁面与自由液面联合作用下的气泡动态特性,采用安全性高且实验效果理想的200V直流电压电火花气泡发生装置生成气泡,依次改变气泡发生位置距壁面及自由液面的距离,同时采用高速运动分析系统对不同工况下的实验结果进行采集与分析,得到了壁面与自由液面联合作用下的气泡形态变化,同时通过对大量实验数据的总结归纳,得到壁面与自由液面联合作用对气泡脉动周期、迁移轨迹及气泡内射流方向的影响规律,从而为相关的理论与数值研究提供参考。 相似文献
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J. M. Boulton-Stone 《Journal of Engineering Mathematics》1993,27(1):73-87
A boundary integral technique is used in conjunction with a conformal map to examine the motion of a two-dimensional bubble near a free surface. For small times, the results are shown to compare well with a first-order perturbation expansion for the problem of the response of a free surface to a deeply submerged dipole. For a large bubble, far from the free surface the bubble deformation is found to agree with previous theoretical and experimental results for a two-dimensional bubble in an infinite fluid. 相似文献
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不同海拔高度进行水下爆破工程时,因水体表面气压随海拔的升高而线性降低,其装药爆炸产生的气泡脉动过程及气泡大小将会发生一定的变化。通过爆炸载荷的测试以及高速摄影2种测试方法对气泡脉动进行了研究。结果表明:在海拔0~4 500 m范围内随着气压降低,气泡脉动周期按二阶多项式规律显著增大,2种方法所得数值误差小于3.8%,数据一致性较好;在海拔0~3 500 m范围内气泡最大半径随海拔升高而线性变大,而4 000 m和4 500 m有突跃变化。将研究结果与水下爆炸气泡周期理论公式进行了比较,并对理论公式在低气压这一特定条件下进行修正,得出的气泡脉动周期系数由原来的2.11修正为1.995,而气泡最大半径系数是一个与海拔有关的一次函数。 相似文献
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