激光熔蚀过程中等离子体冲击波压缩层能量演化

从冲击波基本性质出发,在冲击波压缩层内物质密度均匀的前提下,结合流体力学守恒方程得到冲击波压缩层的机械能通用表达式。继而,分析了激光等离子体球面衰减冲击波情况下冲击波压缩层机械能演变,发现压缩层内的机械能随着冲击波的外向传播出现增大;进而提出波后等离子体区域可能存在其他储能机制,该能量在不断向外界输送能量。最后通过铝靶熔蚀实验,证实了等离子体区域内存在电场能。     

激光聚变冲击波点火的热斑形成机制

通过对冲击波点火内爆过程的数值模拟分析点火热斑压缩及形成机制。分析了传统中心点火的内爆过程,热斑主要经历冲击波压缩和惯性压缩过程,点火主要通过惯性压缩来实现。并仔细分析了冲击波点火的内爆压缩过程,从内爆角度来看冲击波点火并不是压缩和点火分开的两步过程,点火冲击波实际参与压缩过程,点火冲击波对热斑的直接影响很有限,热斑仍然主要通过壳层的惯性压缩实现点火。利用惯性压缩的定标关系及冲击波碰撞对壳层影响规律分析了热斑增压的物理机制,冲击波点火是通过点火冲击波与回冲击波的碰撞来提高壳层的密度,从而实现热斑压力的提升。     

电作用量在磁驱动固体套筒内爆设计分析中的应用

磁驱动固体套筒内爆作为标准柱面冲击/准等熵汇聚压缩加载方式,在流体动力学、材料物性和聚变能源等领域具有广泛应用前景.在特定加载条件下,套筒飞层材料、半径和厚度的选择决定了套筒内爆力学行为,而电流烧蚀限制了所能选择的参数范围.通过薄壁套筒假定引入作为动力学参量的电作用量概念,利用不可压缩零维模型给出了低线电流密度下薄壁套筒尺寸优化设计方法和套筒飞层材料选择的原则;将修正后的电阻率-电作用量模型嵌入自编的一维弹塑性磁流体力学程序SOL1D进行模拟计算,分别与FP-1装置及ZR装置上的实验结果进行比对,表明在大径厚比和低线电流密度加载下,利用电作用量估算内爆速度及利用电爆炸丝实验获取的各阶段电作用量判断套筒物理状态是有效的.     

圆柱形水下爆炸实验容器壁部强度设计研究

 基于薄壁壳理论和水下爆炸理论,对圆柱形水下爆炸实验容器在爆炸冲击波作用下弹性范围内的壁部应变进行了理论分析和实验研究。导出了圆柱形水下爆炸实验容器在爆炸冲击波作用下壁部弹性应变与容器直径、壁厚及内部爆炸药量之间的关系,并对计算结果进行了实验验证。实验表明公式求解结果与实验结果具有较好的一致性。     

Structural response of cylindrically curved laminated composite shells subjected to blast loading

This paper is concerned with the theoretical analysis and correlation with the numerical results of the displacement time histories of the cylindrically curved laminated composite shells exposed to normal blast shock waves. The laminated composite shell is clamped at its all edges. The dynamic equation of the cylindrical shell used in this study is valid under the assumptions made in Love's theory of thin elastic shells. The constitutive equations of laminated composite shells are given in the frame of effective modulus theory. The governing equation of the cylindrical shell is solved by the Runge-Kutta method. In addition, a finite element modeling and analysis are presented and compared with the theoretical results. The peak deflections and response frequencies obtained from theoretical and numerical analyses are in agreement. The effects of material properties and geometrical properties are examined on the dynamic behaviour.     

Cylindrical <Emphasis Type="Italic">Z</Emphasis>-pinch in gas. I. Determination of dependences between discharge integral characteristics

The previously unknown dependences between integral characteristics of the cylindrical Z-pinch in argon were experimentally studied at the stage of its current shell formation and at the initial stage of its plasma pinch compression. Based on these dependences, the power balance at the above stages was determined taking into account the discharge magnetic field energy, electrodynamic force work, gas ionization energy, Joule and shock heating of plasma.     

Electrical and aerodynamic behavior of arc under shock conditions

Arc-shock interaction in a supersonic nozzle has been investigated for a current range from 200 to 1500 A and for three pressure ratios. The adverse pressure gradient associated with the shock causes flow separation and a broadening of arc cross section. Compared with the shock position in the absence of the arc, the shock center is moved toward upstream and to a region close to the wall. The shock is no longer plane. The center of the shock is not very sensitive to the current, but the shock strength reduces when the current is increased, V-I characteristics under shock conditions are slightly modified     

INTERACTION OF A SPHERICAL SHOCK WAVE AND A SUBMERGED FLUID-FILLED CIRCULAR CYLINDRICAL SHELL

The complete three-dimensional interaction between a spherical shock wave and a submerged fluid-filled elastic circular cylindrical shell is considered. A hybrid analytical-numerical solving procedure is established. An exact analytical solution in the form of double Fourier series with time-depending coefficients is obtained for the hydrodynamic pressure. Displacements of a shell are approached analytically to reduce the problem to a set of systems of ordinary differential equations, which are treated numerically. Detailed analysis of the interaction is performed with emphasis given to the stress-strain state. A few important features of the interaction process have been found. In particular, it has been shown that the interior fluid not only substantially affects the magnitude of displacements and stresses, but also dramatically changes the nature of the interaction. It has been found that the absolute maximum of stresses can neither be caused by a direct action of a shock wave nor by a constructive superpose of elastic waves in the shell, but by the pressure wave propagating in the interior fluid. This fact seems to be of essential importance for engineering applications, especially when safety is a primary design concern. Another important result is that the maximum stresses are attained at large times, which makes use of early time asymptotics leading to incorrect results. The proposed semi-analytical approach seems to be computationally attractive and suitable for extensive numerical simulations.     

Hydrodynamic fields induced by the shock response of a fluid-filled submerged cylindrical shell containing a rigid co-axial core

The hydrodynamic fields induced by the response to an external shock wave of a system consisting of a submerged fluid-filled cylindrical shell and a rigid cylindrical co-axial core are considered. The primary focus of the study is on the complexity brought into the interaction by the presence of the core, and on the analysis of the multitude of the respective shock wave propagation and reflection phenomena. It is shown that when the core is small, its overall impact on the interaction is insignificant, although the hydrodynamic patterns observed exhibit some interesting features even in that case. As the radius of the core increases, its effect on the interaction becomes more and more pronounced, with the internal wave pattern eventually becoming dramatically different from what is observed in the no-core case. As a part of this investigation, the exact reasons for the significant reduction of the tensile stress reported for a larger core in earlier studies are identified. Finally, when the core becomes sufficiently large to dominate the internal volume, the fluid between the shell and the core starts to behave as a fluid layer, and exhibits some properties similar to those of a waveguide.     

Evolution of the reflection and focusing patterns and stress states in two-fluid cylindrical shell systems subjected to an external shock wave

Several most important features of the hydrodynamic field induced inside a circular cylindrical shell filled with and submerged into different fluids when it is subjected to an external shock wave are considered. This investigation is a follow-up of an earlier study of the two-fluid shell-shock interaction [S. Iakovlev, Interaction between an external shock wave and a cylindrical shell filled with and submerged into different fluids, Journal of Sound and Vibration 322 (2009) 401-437], and it addresses a number of practically important issues not covered in that work. The focus of this study is on the evolution of the respective hydrodynamic patterns in response to the continuous change of the parameters of the fluids, in particular the speed of sound. Along with the analysis of the hydrodynamic patterns it is also demonstrated that when one is concerned with the highest pressure attained inside the shell, the most dangerous combination of the parameters occurs when the ratio of the internal and external acoustic speeds is close to 0.48, with the respective pressure exceeding the maximum incident pressure by more than 110 percent. The effect that the hydrodynamic features discussed have on the stress state of the shell is addressed as well, and it is observed that the maximum tensile stress is significantly affected by the evolution of the considered hydrodynamic features, whereas the maximum compressive stress is not. It is also observed that the maximum tensile stress is very sensitive to the change of the ratio of the acoustic speeds in the internal and external fluids, with as little an increase of the latter as 13 percent resulting in more than doubling of the former in some cases.     

基于纯冲击波聚心的准一维氘氘内爆物理实验

在神光Ⅲ原型装置上利用八路6400J/1ns激光注入1100μm×1850μm的黑腔内产生210eV的高温辐射场,均匀辐照填充氘氘燃料的靶丸实现内爆。实验中选择高气压薄壳靶丸实现纯冲击波聚心内爆。通过闪烁体探测器、中子条纹相机等多套诊断设备获取了中子产额、聚变反应时刻等关键内爆参数。结合一维数值模拟表明,实验测量的中子产额与干净一维数值模拟计算的中子产额之比达到90%;同时通过人为破坏内爆对称性等方式表明,该设计下内爆中子产生机制集中于冲击波聚心,其内爆性能受到高维因素影响极低,从而实现了准一维内爆。     

Ultimate energy of cosmic rays generated in supernova shells

It is shown that the ultimate energy of cosmic rays accelerated in a supernova shell due to the surfing acceleration mechanism is determined by the shell radius and the interstellar magnetic field. The ultimate energy of cosmic rays accelerated in the supernova shock does not exceed 10¹⁷ eV for typical values of the interstellar magnetic field in the vicinity of a supernova and the radii of observed supernova shells.     

Current discontinuities on superconducting cosmic strings

The propagation of current perturbations on superconducting cosmic strings is considered. The conditions for the existence of discontinuities similar to shock waves have been found. The formulas relating the string parameters and the discontinuity propagation speed are derived. The current growth law in a shock wave is deduced. The propagation speeds of shock waves with arbitrary amplitudes are calculated. The reason why there are no shock waves in the case of time-like currents (in the “electric” regime) is explained; this is attributable to the shock wave instability with respect to perturbations of the string world sheet.     

Analytical studies on the evolution processes of rarefied deuterium plasma shell Z-pinch by PIC and MHD simulations

In this paper, we analytically explore the magnetic field and mass density evolutions obtained in particle-in-cell(PIC)and magnetohydrodynamics(MHD) simulations of a rarefied deuterium shell Z-pinch and compare those results, and also we study the effects of artificially increased Spitzer resistivity on the magnetic field evolution and Z-pinch dynamic process in the MHD simulation. There are significant differences between the profiles of mass density in the PIC and MHD simulations before 45 ns of the Z-pinch in this study. However, after the shock formation in the PIC simulation,the mass density profile is similar to that in the MHD simulation in the case of using multiplier 2 to modify the Spitzer resistivity. Compared with the magnetic field profiles of the PIC simulation of the shell, the magnetic field diffusion has still not been sufficiently revealed in the MHD simulation even though their convergence ratios become the same by using larger multipliers in the resistivity. The MHD simulation results suggest that the magnetic field diffusion is greatly enhanced by increasing the Spitzer resistivity used, which, however, causes the implosion characteristic to change from shock compression to weak shock, even shockless evolution, and expedites the expansion of the shell. Too large a multiplier is not suggested to be used to modify the resistivity in some Z-pinch applications, such as the Z-pinch driven inertial confinement fusion(ICF) in a dynamic hohlraum. Two-fluid or Hall MHD model, even the PIC/fluid hybrid simulation would be considered as a suitable physical model when there exist the plasma regions with very low density in the simulated domain.     

间接驱动冷冻双壳层点火靶的设计和分析

双壳层靶中,由于燃料被高Z壳层包裹,其点火方式要求燃料整体点火,不同于单壳层中心热斑点火。结合点火条件和对于其中物理过程的认识,设计了间接驱动的冷冻双壳层点火靶。利用冷冻的氘氚(DT)燃料,可适当提高双壳层靶的燃料装量,获得和NIF装置条件下中心热斑点火靶相当的放能。间接驱动下,X射线烧蚀并驱动外壳层碰撞内壳层,把能量传递给内壳层,进而压缩和点燃冷冻的DT燃料。壳层碰撞过程是能量传递的关键,通过调整内外壳层的质量比,提高了碰撞效率,相应地降低了靶丸点火的能量需求。一维数值模拟分析了该点火靶的内爆过程及定性分析了其中的流体力学不稳定性。同时,也指出了泡沫中形成的辐射冲击波对内壳层的预热效应,即辐射冲击波的致稳效应,能够很好地抑制内壳层外界面处的不稳定性发展,进而会减弱高Z内壳层和燃料的混合。     

Current distribution and giant magnetoimpedance in composite wires with helical magnetic anisotropy

The giant magnetoimpedance effect in composite wires consisting of a non-magnetic inner core and soft magnetic shell is studied theoretically. It is assumed that the magnetic shell has a helical anisotropy. The current and field distributions in the composite wire are found by means of a simultaneous solution of Maxwell equations and the Landau–Lifshitz equation. The expressions for the diagonal and off-diagonal impedance are obtained for low and high frequencies. The dependences of the impedance on the anisotropy axis angle and the shell thickness are analyzed. Maximum field sensitivity is shown to correspond to the case of the circular anisotropy in the magnetic shell. It is demonstrated that the optimum shell thickness to obtain maximum impedance ratio is equal to the effective skin depth in the magnetic material.     

Shock shells in Coulomb explosions of nanoclusters

We predict that Coulomb explosion of a nanoscale cluster, which is ionized by high-intensity laser radiation and has a naturally occurring spatial density profile, will invariably produce shock waves. In most typical situations, two shocks, a leading and a trailing one, form a shock shell that eventually encompasses the entire cluster. Being the first example of shock waves on the nanometer scale, this phenomenon promises interesting effects and applications, including high-rate nuclear reactions inside each individual cluster.     

Active control of cylindrical shell with magnetostrictive layer

This paper analyses the damping characteristics of a titanium shell with a magnetostrictive layer bonded to it. The magnetostrictive layer produces an actuating force required to control vibration in the shell, based on a negative velocity feedback control law. The control input is the current to the solenoid surrounding the shell. In the present study, a finite element formulation, physically consistent with the problem has been developed. Vibration reduction in the shell by changing the position of the magnetostrictive layer and its current carrying actuating coil pair along the shell is investigated.     

Model of pulsed electric discharge expansion in dense gas taking into account electron and radiative thermal conductivities. I. Expansion mechanism

Using an ionization sensor, it was found that weakly ionized plasma with an ionization degree larger than 10^?6 is formed under exposure to UV radiation of a high-current pulsed electric discharge in gas (air, nitrogen, xenon, and krypton) at atmospheric pressure at a distance of ～1.2–2.5 cm from the discharge boundary. It was shown that the structure of such discharge includes, in addition to the discharge channel, a dense shell and a shock wave, also a region of weakly ionized and excited gas before the shock wave front. The mechanism of discharge expansion in dense gas is ionization and heating of gas involved in the discharge due to absorption of the UV energy flux from the discharge channel and the flux of the thermal energy transferred from the discharge channel to the discharge shell due to electron thermal conductivity.     

现代壳模型

传统壳模型存在的一个主要问题是计算过于复杂以致无法进行.随着计算机计算能力的空前提高,现在已经可以进行极大规模的壳模型计算.然而,还不清楚这种计算对于深入理解物理问题是否有实际帮助.况且,对于组态空间可达1014—1018维的中重核,当前的计算机能力还达不到.因此对中重核仍需研究如何把巨大的模型空间截断到最佳的可操作子空间的问题.近来提出的配对壳模型给出了一个很有用的方法,其它截断模型可归入它的特殊情况.与此同时,从现实有效二体相互作用出发进行壳模型多体计算方面也正在取得巨大的进展. The current status on the theoretical investigations of the nuclear shell model is reviewed, and the fundamental problems in shell model studies are mentioned. Basically the shell model uses a very intuitive approach to study the nuclear many body dynamics in terms of valence particles. It assumes that the nucleons, belonging to a closed core, do not participate in the establishment of the nuclear spectrum. One of the main problems in the (traditional) shell model is to make a calculation...