从滑行到能量守恒:强爆炸相互作用阶段的新自相似解

Eric R. Coughlin
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引用次数: 0

摘要

包含高密度和冲压为主的喷出物的天体物理爆炸会经历一个相互作用阶段,在此期间会形成正向冲击(FS)、接触不连续(CD)和反向冲击(RS),并随着时间的推移而扩展。我们描述了适用于这一阶段的新的自相似解,在喷出物密度比环境密度大的极限情况下,这些解最为精确。这些解预言了FS、CD和RS在时间上以不同的速度膨胀,而不是作为单一的时间幂律膨胀,适用于由稳定风和同源膨胀喷出物驱动的爆炸,并且存在于环境密度剖面是幂律指数小于$\sim 3$的幂律时(特别是当FS不加速时)。我们发现这些解的预测结果与流体力学模拟结果在不连续性的时间行为和流体量的变化方面都非常吻合。自相似解适用于广泛的天体物理现象,而且--尽管细节将在未来的工作中描述--可以推广到包含任意洛伦兹因子的相对论速度。我们认为,这些解决方案准确地插值于爆炸的初始 "沸腾 "阶段和后来的能量守恒阶段(或者,如果喷出物是同源的,并且密度剖面足够陡峭,则插值于1982年Chevalier所描述的自相似阶段)之间、
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From coasting to energy-conserving: new self-similar solutions to the interaction phase of strong explosions
Astrophysical explosions that contain dense and ram-pressure-dominated ejecta evolve through an interaction phase, during which a forward shock (FS), contact discontinuity (CD), and reverse shock (RS) form and expand with time. We describe new self-similar solutions that apply to this phase and are most accurate in the limit that the ejecta density is large compared to the ambient density. These solutions predict that the FS, CD, and RS expand at different rates in time and not as single temporal power-laws, are valid for explosions driven by steady winds and homologously expanding ejecta, and exist when the ambient density profile is a power-law with power-law index shallower than $\sim 3$ (specifically when the FS does not accelerate). We find excellent agreement between the predictions of these solutions and hydrodynamical simulations, both for the temporal behavior of the discontinuities and for the variation of the fluid quantities. The self-similar solutions are applicable to a wide range of astrophysical phenomena and -- although the details are described in future work -- can be generalized to incorporate relativistic speeds with arbitrary Lorentz factors. We suggest that these solutions accurately interpolate between the initial ``coasting'' phase of the explosion and the later, energy-conserving phase (or, if the ejecta is homologous and the density profile is sufficiently steep, the self-similar phase described in Chevalier 1982),
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