共查询到18条相似文献,搜索用时 92 毫秒
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为了降低爆轰产物及爆轰参数的求解难度,通过对质量守恒方程的基本可行解进行线性组合,得到了爆轰产物的平衡组成,并在此基础上进一步获得了爆轰参数。其主要实现方法为:由最小自由能原理对基本可行解进行筛选,然后根据最大放热原则确定初始解,并在最小自由能原则的引导下,由初始解和基本可行解的线性组合获得爆轰产物的平衡组成,以上操作步骤均由自编程序完成。应用支持向量机(SVM)线性模型对BKW状态方程参数进行了调整,并详细介绍了其主要步骤。使用此方法预测了PETN、CL-20和含铝炸药的爆轰产物及爆轰参数,经参数调整后,发现预测结果与实验值吻合良好;通过与单质炸药爆轰实验数据对比,发现调整BKW状态方程参数时,应当尽可能使用爆轰产物中气体含量相近的含能材料对SVM模型进行训练;若预测含铝炸药,应当使用铝氧比接近待测炸药的样品来训练SVM模型。 相似文献
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几种呋咱类含能化合物的合成、热行为及理论爆轰性能预估 总被引:2,自引:0,他引:2
用双氧水、钨酸钠及甲磺酸氧化3,4-二氨基呋咱(DAF)合成了3-氨基-4-硝基呋咱;用100%硝酸硝化DAF得到3,4-二硝胺基呋咱;用NaNO_2、H_2SO_4及NaN_3DAF重氮、取代DAF得到3-氨基-4-叠氮基呋咱;用30%的双氧水、钨酸钠及甲磺酸氧化3-氨基-4-叠氮基呋咱,得到3-叠氮基-4-硝基呋咱及3,3′-二叠氮基-4,4′-氧化偶氮呋咱。用TG-DSC研究了这些化合物的热行为。采用B3LYP/6-31G*方法预估了化合物的理论密度、标准生成、爆速、爆压。结果表明,氧化偶氮基的引入增强了呋咱类化合物的热稳定性;叠氮基的引入提高了化合物的生成焓。3-氨基-4-硝基呋咱中氨基转化为叠氮基,生成焓由183.26kJ/mol增至571.40 kJ/mol;硝胺基的引入显著提高了含能化合物的密度、爆速和爆压。 相似文献
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为研究装药密度对3,4-二硝基呋咱基氧化呋咱(DNTF)驱动性能的影响,采用不同的凝固工艺制备了两种密度的DNTF装药试样,并开展了Φ25mm圆筒试验,获得了圆筒壁膨胀位移与时间的关系,计算了爆轰产物在特定相对比容下的比动能及装药的格尼系数,并依据圆筒试验数据拟合了两种装药密度下DNTF爆炸产物的JWL状态方程。结果表明,常温常压凝固工艺条件下,DNTF装药密度仅为1.58g/cm3;在80℃、0.6MPa工艺条件下,装药密度升至1.80g/cm3,较常温常压下提高了13.9%;在装药密度为1.58g/cm3下,DNTF的格尼系数为2.97mm/μs,爆轰产物相对比容为7.0时的比动能为1.471kJ/g;在装药密度为1.80g/cm3下,DNTF的格尼系数增至3.03mm/μs,爆轰产物比动能增至1.716kJ/g,分别较常温常压下提高了2%和16.7%。表明DNTF装药密度的提升不仅能够显著提升单位体积装药的驱动性能,也有利于单位质量装药驱动性能的进一步增强。 相似文献
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为了提高乳化炸药的爆炸威力,研制出了一种MgH2型复合敏化储氢乳化炸药。该乳化炸药采用包覆后的MgH2与玻璃微球复合敏化,两种材料分别起到含能添加剂和敏化剂的作用。通过研究“热点”数量和包覆材料对炸药爆轰性能的影响,确定了MgH2型复合敏化储氢乳化炸药的配方。利用水下爆炸实验和猛度实验,研究了MgH2型复合敏化储氢乳化炸药的爆轰特征参数和水下爆炸特性。实验结果表明,MgH2型复合敏化储氢乳化炸药的铅柱压缩量为24.3 mm,达到军用炸药的猛度;与传统玻璃微球型乳化炸药相比,其水下爆炸峰值压力虽然下降了4.90%,但比冲击波能、比气泡能和总能量分别提高了7.83%、22.94%和18.32%。MgH2型复合敏化储氢乳化炸药的猛度和做功能力得到了显著提高。 相似文献
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V. P. Kopyshev A. B. Medvedev V. V. Khrustalev 《Combustion, Explosion, and Shock Waves》2006,42(1):76-87
A semi-empirical model is proposed for the equation of state of high explosives in a range of pressures and temperatures typical
of detonation processes. A possibility of formation of solid phases (e.g., graphite or diamond) in the gas is implied. The
model can be used to calculate all thermodynamic quantities for arbitrary molecular compositions and to calculate the thermodynamically
equilibrium molecular (and phase) composition. An iterative scheme of calculations is proposed. The model contains several
empirical functions whose form can be changed without violating the overall calculation scheme. A particular set of these
functions is considered as an illustration. Some results calculated for a number of high explosives containing four elements
(C, H, N, and O) are presented. The calculated results are compared with available experimental data.
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Translated from Fizika Goreniya i Vzryva, Vol. 42, No. 1, pp. 87–99, January–February, 2006. 相似文献
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V. P. Kopyshev A. B. Medvedev V. V. Khrustalev 《Combustion, Explosion, and Shock Waves》2004,40(2):200-208
A viscosity model is proposed for mixed liquids and dense gases obeying a modified van der Waals equation of state. Estimates are given for the viscosity of the explosion productsof RDX, PETN, and nitromethane in the states occurring in detonation processes. 相似文献
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扩展了立方扰动硬链(CSPHC)状态方程在天然气工业中通常遇到物质的纯组分参数, 并建立了纯组分参数的普遍化关联式; 将过量Gibbs自由能混合规则引入CSPHC状态方程, 以应用于高度非对称体系与极性体系相平衡性质计算。结合MPHC活度系数模型及Wilson 活度系数模型, 对13组二元体系的汽液平衡性质获得较满意的结果。 相似文献
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Muhamed Suceska How‐Ghee Ang Hay Yee SereneChan 《Propellants, Explosives, Pyrotechnics》2013,38(1):103-112
Due to its simplicity, the Becker‐Kistiakowsky‐Wilson (BKW) equation of state has been used in many thermochemical codes in the calculation of detonation properties. Much work has been done in the calibration of the BKW EOS parameters to achieve agreement with experimental detonation velocities and pressures thus resulting in many different sets of BKW constants (α, β, κ and θ) and covolumes of detonation products, with varying levels of accuracy over broad density limits, i.e. broad pressure limits. The covolumes of the product gases in BKW EOS may be regarded as measures of intermolecular interactions, and their values should affect the predicted detonation properties, particularly at higher explosives densities. This work aims to study the effect of covolumes on calculated values of detonation parameters. Several sets of covolumes available from literature and derived by different methods (matching experimental Hugoniots of individual products, by stochastic optimization, and calculated from van der Waals radii), were studied. In addition, the covolumes of the product gases were also calculated by ab initio methods. The effect of covolumes is studied comparing detonation properties calculated using different sets of covolumes, and experimental data for a series of standard CHNO explosives. It was found that it is possible to reproduce experimental detonation velocities and pressures within reasonable accuracy (root mean square error of less than 5 % for all tested sets) using different set of covolumes, and simultaneously optimizing constants in BKW EOS. However, different values of covolumes strongly affect the composition of detonation products at the Chapman‐Jouguet state. It particularly applies to oxygen‐deficient explosives and at higher densities, where formic acid appears to be an important detonation product. 相似文献
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A new general equation of state is presented, which can be used to express not only common cubic equations of state, but also quartic equations of state and so on. Main advantage of the new equation over the previous general equations is that it is in simple form, and is easy to manipulate mathematically. 相似文献
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In our previous paper we extended the Tao and Mason equation of state (TM EOS) to refrigerant fluids, using the speed of sound data. This is a continuation for evaluating TM EOS in predicting PVT properties of heavy n-alkanes. Liquid density of long-chain n-alkane systems from C 9 to C 20 have been calculated using an analytical equation of state based on the statistical-mechanical perturbation theory. The second virial coefficients of these n-alkanes are scarce and there is no accurate potential energy function for their theoretical calculation. In this work the second virial coefficients are calculated using a corresponding state correlation based on surface tension and liquid density at the freezing point. The deviation of calculated densities of these alkanes is within 0.5% from experimental data. The densities of n-alkanes obtained from the TM EOS are compared with those calculated from Ihm-Song-Mason equation of state and the corresponding-states liquid densities (COSTALD). Our results are in favor of the preference of the TM EOS over other two equations of state. 相似文献