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The Density Spike in Cosmic-Ray-Modified Shocks: Formation, Evolution, and Instability

机译:宇宙射线修改后的冲击中的密度峰值:形成,演化和不稳定性

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We examine the formation and evolution of the density enhancement (density spike) that appears downstream of strong, cosmic-ray-modified shocks. This feature results from temporary overcompression of the flow by the combined cosmic-ray shock precursor and gas subshock. Formation of the density spike is expected whenever shock modification by cosmic-ray pressure increases strongly. That occurrence may be anticipated for newly generated strong shocks, or for strong shocks or cosmic-ray-modified shocks encountering a region of higher external density, for example. The predicted mass density within the spike increases with the shock Mach number and with shocks more dominated by cosmic-ray pressure. For very strong shocks, the total compression compared to the upstream gas may approach D(γg + 1)/(γg - 1) during the formation period, where γg is the gas adiabatic index and D is the compression ratio through the precursor. As the full shock reaches equilibrium, the spike detaches, lags behind the modified shock transition, and is further compressed, so that the density can exceed the limit quoted above. We find this spike to be linearly unstable under a modified Rayleigh-Taylor instability criterion at the early stage of its formation. Our linear analysis shows that the flow is unstable when the gradients of total pressure (gas pressure + cosmic-ray pressure) and gas density have opposite signs. We confirm this numerically using two independent codes based on the two-fluid model for cosmic-ray transport. These two-dimensional simulations show that the instability grows impulsively at early stages and then slows down as the gradients of total pressure and gas density decrease. Flow within the density spike becomes disordered through the instability. It seems likely that this can significantly increase the local magnetic field beyond compressional effects. Observational discovery of this unstable density spike behind shocks, possibly through radio emission enhanced by the amplified magnetic fields, would provide evidence for the existence of strongly cosmic-ray-modified shock structures.
机译:我们研究了在强的,宇宙射线修饰的冲击的下游出现的密度增强(密度峰值)的形成和演化。此功能是由于宇宙射线激波前兆和气体冲击相结合而使气流暂时过压所致。每当通过宇宙射线压力引起的冲击改变强烈增加时,就有望形成密度峰值。例如,对于新产生的强烈震动,或者遇到较高外部密度区域的强烈震动或宇宙射线改性的震动​​,可能会发生这种情况。尖峰内的预测质量密度随着冲击马赫数增加,并且冲击更多地受到宇宙射线压力的支配。对于非常强烈的冲击,在形成期间,与上游气体相比,总压缩比可能接近D(γg+1)/(γg-1),其中γg是气体绝热指数,D是通过前驱体的压缩比。当整个冲击达到平衡时,尖峰分离,滞后于修改后的冲击过渡,并被进一步压缩,因此密度可以超过上面引用的极限。我们发现,在修改后的瑞利-泰勒不稳定性准则的早期,该峰值是线性不稳定的。我们的线性分析表明,当总压力(气压+宇宙射线压力)和气体密度的梯度具有相反的符号时,流动不稳定。我们使用基于双流体模型的两个独立代码对宇宙射线传输进行数值确认。这些二维模拟表明,不稳定性在早期阶段呈脉冲状增长,然后随着总压力和气体密度梯度的降低而减慢。密度峰值内的流动由于不稳定性而变得混乱。似乎这可能会大大增加局部磁场,而不会产生压缩效应。观察到的震荡背后不稳定密度峰值的发现,可能是由于放大磁场增强了无线电发射,为存在强烈的宇宙射线修饰的震荡结构提供了证据。

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