共查询到19条相似文献,搜索用时 93 毫秒
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利用纹影技术研究了炸药爆轰后驱动物质的变形过程。为了便于观察,待测物质选取为变形比较大的介质水。实验观察表明,在炸药爆轰作用下,筒状水的膨胀首先由雷管起爆端开始,形成了倾斜状、波浪形的界面。结果表明:阵面的波动破裂均从外界面开始,界面的不稳定性可能是导致其失稳并破碎的主要原因。实验还观察到炸药爆轰后不同延迟时间的物体从大块变成小块的发展过程。研究中克服了炸药爆轰产物发光对图像的影响,以及爆炸振动对光路的影响。研制了一种简易的触发探针,解决了外光源和炸药爆轰的同步问题。 相似文献
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爆炸是自然界中经常发生的一种物理与化学的过程,在爆炸过程中,以极高的速度释放出能量.爆炸产物对周围介质作功,产生破坏作用,如破坏弹体形成杀伤破片,爆破矿山抛掷土石,在介质中形成冲击波、应力波等.爆炸的主要特征是在爆炸中心周围的介质中产生压力突跃,这种压力上升前沿只有几个微秒.爆炸力学学科就是要从定性、定量两方面来描述爆炸过程的力学,这是一门边缘性学科,它涉及爆轰物理学,其内容包括炸药的化学反应特征,炸药的爆轰过程及爆轰参数的理论与工程计算方法等;爆炸气体力学,其内容包括爆炸产物在其形成的特定流场中各个参量:压力场,密度场的计算. 相似文献
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用两相流模型对悬浮RDX炸药粉尘爆轰波进行了数值模拟。RDX炸药颗粒在爆轰波阵面后的高温高速气流中加速并升温,颗粒表面发生熔化。参考液滴在高速气流作用下剥离的效应,假设炸药熔化部分在高速气流的作用下发生剥离,破碎成极小的颗粒,瞬时发生分解反应,释放出能量支持爆轰波传播。数值模拟了在不同粒径和浓度的悬浮RDX炸药粉尘中爆轰波的发展与传播过程,得到了爆轰波流场中气-固两相的物理量分布,并确定了爆轰波参数。在较低的RDX粉尘浓度条件下,爆轰波阵面压力的峰值曲线出现振荡。当RDX粉尘浓度在80~150 g/m3时,数值模拟得到的爆轰波阵面压力峰值曲线的振荡是规则的;当RDX粉尘浓度为70 g/m3时,爆轰波阵面压力峰值曲线出现不规则振荡。 相似文献
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通过理论计算和水下爆炸实验,初步研究了MgH2敏化储氢型乳化炸药的爆炸特性和爆轰反应机理。结果表明:与玻璃微球敏化的乳化炸药相比,MgH2敏化的乳化炸药水下爆炸的冲击波超压、比冲量、比冲击波能、比气泡能及水下爆炸比总能量显著增加,其中冲击波超压和水下爆炸总能量分别增加了20.5%和31.0%。MgH2储氢型乳化炸药的爆轰机理与玻璃微球敏化乳化炸药不同,MgH2在乳化炸药中起到了敏化剂和含能材料的双重作用,即MgH2在乳化基质中水解产生均匀分布的氢气泡,起到了敏化作用,同时氢气参与爆炸反应,提高了炸药的爆炸能量和做功能力。 相似文献
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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
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A. A. Sulimov B. S. Ermolaev S. B. Turuntaev A. A. Borisov M. K. Sukoyan 《Russian Journal of Physical Chemistry B, Focus on Physics》2014,8(3):338-344
The results of experimental investigations and thermodynamic calculations of the detonation of explosive proppant, an RDX-containing water-saturating sand, are reported. The material studied is of interest for use as an explosive additive to propping material injected into hydraulic fractures of oil-bearing beds. The tests were conducted in duralumin casings with cylindrical or planar inner channels. The dependences of the detonation velocity on the RDX content in the mixture in the range of 14 to 74 wt %, RDX and sand particle size, and initial temperature are examined. The critical detonation diameter of the charge decreases with increasing content RDX in the mixture, being only several millimeters at RDX contents of 30 wt % and above. Polydisperse RDX provides a high detonability of such mixtures; use of narrow particle size RDX fractions, especially coarse (0.4–0.7 mm), significantly increases the critical detonation diameter. As the initial temperature of the mixture is increased from 20 to 90°C, the critical detonation width decreases severalfold. The detonation of mixtures in a convergent planar channel occurs at a constant rate, which differs little from the detonation velocity measured in a cylindrical channel. Reaching the place where the opening of the channel is less than the critical width, detonation fails abruptly. Thermodynamic calculations of the detonation characteristics of the explosive proppant are performed using the BKWS equation of state under the assumption that the sand component behaves as an inert additive, being in mechanical equilibrium with the detonation products of the RDX-water mixture. A satisfactory agreement with the experimental data on the detonation velocity and its dependence on the RDX content is demonstrated. This makes it possible to conclude that RDX mixed with water-saturated sand detonates within a narrow reaction zone without significant convective heat transfer to the inert additive. 相似文献
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B. D. Yankovskii V. V. Milyavskii 《Russian Journal of Physical Chemistry B, Focus on Physics》2013,7(2):142-148
A nomographic method for predicting the detonation velocity of a porous explosive mixture prepared from RDX powder and water is proposed. It is shown that, in contrast to the existing calculation methods for predicting the detonation velocity, the use of the proposed nomogram greatly simplifies the procedure and requires knowledge of only two parameters: the mass fraction of RDX and the density of the mixture in the charge. At the same time, the nomogram is a coordinate system that enables to place and to compare on one field experimental data obtained at different parameters of the charge. It is shown that RDX powder-water hand-prepared charges can have a detonation velocity of 6–8 km/s. The detonation velocity of cylindrical water-containing charges 10–36 mm in diameter and 120–1000 mm in length with RDX mass fractions of 0.6–1.0 is measured. 相似文献
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Scott I. Jackson Charles B. Kiyanda Mark Short 《Proceedings of the Combustion Institute》2011,33(2):2219-2226
Detonations in explosive mixtures of ammonium-nitrate-fuel-oil (ANFO) confined by aluminum allow for transport of detonation energy ahead of the detonation front due to the aluminum sound-speed exceeding the detonation velocity. The net effect of this energy transport on the detonation is unclear. It could enhance the detonation by precompressing the explosive near the wall. Alternatively, it could decrease the explosive performance by crushing porosity required for initiation by shock compression or destroying confinement ahead of the detonation. At present, these phenomena are not well understood. But with slowly detonating, non-ideal high explosive (NIHE) systems becoming increasing prevalent, proper understanding and prediction of the performance of these metal-confined NIHE systems is desirable. Experiments are discussed that measured the effect of ANFO detonation energy transported upstream of the front by a 76-mm-inner-diameter aluminum confining tube. Detonation velocity, detonation front-shape, and aluminum response are recorded as a function of confiner wall thickness and length. Detonation shape profiles display little curvature near the confining surface, which is attributed to energy transported upstream modifying the flow. Average detonation velocities were seen to increase with increasing confiner thickness, while wavefront curvature decreased due to the stiffer, subsonic confinement. Significant radial sidewall tube motion was observed immediately ahead of the detonation. Axial motion was also detected, which interfered with the front-shape measurements in some cases. It was concluded that the confiner was able to transport energy ahead of the detonation and that this transport has a definite effect on the detonation by modifying its characteristic shape. 相似文献
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对爆磁压缩发生器中爆炸管2维动力学简化模型进行了模拟计算,分析表明:径向膨胀速度会随径向位置(或者时间)的变化而变化,因此膨胀角也会随径向位置(或者时间)发生变化。对各时间点(或位置点)处的膨胀速度进行了平均,求得理论上的平均膨胀速度,再将该平均膨胀速度与实验测量值进行了比较。模拟结果给出了径向膨胀速度受到端头效应影响的情况,这可为改进实验结果提供参考。由于径向速度与轴向速度的比值一般在5以上,用作爆炸管的物质质量越大,这一比值就越大,因此选择密度较大的金属材料作为爆炸管,可减少滑移。应用2D简化模型计算出的膨胀角数值,与Gurney模型以及1D模型进行了比较,它们之间的差别可能主要来自2D效应。 相似文献
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A. A. Sulimov B. S. Ermolaev M. K. Sukoyan 《Russian Journal of Physical Chemistry B, Focus on Physics》2012,6(3):397-403
The pressure at the front and the pressure impulse of blast waves generated in a cylindrical tube by the expanding products
of the nonideal detonation of low-porosity charges prepared by pressing of fine-grained powders of aluminum, Teflon, and RDX
were measured. The measured parameters are compared to the same parameters of blast waves produced by the detonation of TNT
charges of identical mass. The relative quantities were used to evaluate the effectiveness of blast waves with respect to
those generated by TNT. Mixed compositions differing in the shape (brand) of the aluminum powder particles and the ratio between
the components at 30% RDX are studied. It is shown that, for the investigated compositions, the pressure at the leading front
of the wave exceeds the pressure achieved during TNT explosion on average by 10–30%, almost independently of the distance
traveled along the tube in the range from 0.8 to 3.8 m. The dependence of the wave amplitude on the particle shape and aluminum
content was weak. In the same range of distances, the relative pulse pressure increases strongly, from 0.5 to 2.1 and higher,
mainly due to an increase in the width of the wave. This result is of interest from the point of view of achieving a high
pressure impulse of the blast wave in an area remote from the charge. The obtained data suggest that RDX mainly reacts in
the detonation wave, with the chemical transformation of Teflon and aluminum in the detonation wave and near-to-charge zone
occurring, if at all, to a small extent. On the contrary, as the blast wave front moves through the channel, the burning of
aluminum in the fluoride formed during the decomposition of Teflon provides an appreciable support to the blast wave, causing
a significant increase in the pressure impulse. 相似文献
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A. A. Sulimov A. A. Borisov B. S. Ermolaev M. K. Sukoyan V. E. Khrapovskii P. V. Komissarov 《Russian Journal of Physical Chemistry B, Focus on Physics》2009,3(5):789-797
The results of experimental studies of the nonideal detonation of high-density, high-energy aluminum-ammonium perchlorate-organic
fuel-HE compositions and of the blast waves it generates in a channel filled with air are presented. Aluminum-enriched compositions
have high densities (up to 2 g/cm3) and high heats of explosion, nearly twice that for TNT. The studies were performed to work out scientific fundamentals of
controlling nonideal detonation and to explore the possibility of creating new high-energy high-density formulations with
an enhanced fugacity effect. The factors that enable controlling the nonideal detonation of such charges were determined.
It was demonstrated that, at RDX contents above 15%, the detonation velocity increases linearly with the charge density while
the critical detonation diameter decreases. Adjusting the density, HE content, ratio of the components makes it possible to
vary the detonation velocity in high-density charges over a wide range, from 4 to 7 km/s. The experimental data were compared
to the thermodynamically calculated velocity of ideal detonation. For the compositions under study, the pressure- time histories
of the blast wave generated in a cylindrical tube by the expanding detonation products at different distances from the charge
were measured. The results were compared to analogous data obtained under the same conditions for the detonation of the same
mass of TNT (100 g). The parameters of blast waves generated by the test compositions are markedly superior to those characteristic
of TNT: the pressure at the leading front of the wave and pressure impulse at a given distance from the charge were found
to be 1.5–2.0 (or even more) times those observed for TNT. The TNT equivalency at pressures 30–60 atm has similar values.
The TNT equivalencies in pressure and pressure impulse depend nonmonotonically on the distance from the charge, so far unclear
why. It was established that the interaction between excess fuel and air oxygen during the expansion of detonation products
contributes little to supporting the blast wave. 相似文献
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为了研究负载为mH量级的间接馈电两级级联柱-锥构型的爆磁压缩产生器的基本物理过程和能量转换机理,利用描述爆磁压缩物理过程的2维爆轰磁流体力学程序MFCG(Ⅴ),以实验模型结构参数为基础模拟计算了一系列模型,分析了磁压对金属套筒径向膨胀速度及膨胀过程的影响。计算结果表明:套筒的径向膨胀速度取决于爆轰压与磁压的共同作用,在爆磁压缩过程的绝大部分时间里,向外膨胀的爆轰压都远大于向内压缩的磁压,因而套筒的径向膨胀速度主要是由爆轰压决定;但是在功率放大级的后半段,也就是发生器电流增长最快阶段,磁压也迅速增长,它的增长大大降低了套筒的径向膨胀速度;在功率放大级的后期,磁压已经超过爆轰压,它对系统设计的影响已经不能完全忽略。 相似文献