论文标题
3D碰撞磁化弓形冲击在脉冲驱动的等离子体流动中的结构
The structure of 3D collisional magnetized bow shocks in pulsed-power-driven plasma flow
论文作者
论文摘要
我们研究了高度碰撞的磁化铝等离子体中的3D弓冲击,该血浆是在喜pie设施上爆炸线阵列的消融阶段产生的(1.4 mA,240 ns)。从电线阵列中消融等离子体会产生径向散开的超音速($ M_S \ SIM 7 $),Super-Alfvénic($ M_A> 1 $)的磁化流,带有冷冻磁力($ r_m \ gg 1 $)。这些流与流动中的电感探针相撞,这既是产生磁化弓形冲击的障碍物,又是对流磁场的诊断。沿两条正交线的激光干涉法用于测量线集成电子密度。在探针前形成了独立的弓形冲击,平行于磁场的平面比正常的平面平行的开口角更大。由于等离子体的电阻扩散长度与探针大小相当,因此磁场从冲击锋处将离子流体分离并产生流体动力冲击,其结构由声音马赫数确定,而不是流量的磁性马赫数。使用电阻性磁水动力学(MHD)代码Gorgon进行的3D模拟证实了这张照片,但预测不足的各向异性在实验性弓形冲击的形状中观察到,这表明非MHD机制可能对于修饰冲击结构可能很重要。
We investigate 3D bow shocks in a highly collisional magnetized aluminum plasma, generated during the ablation phase of an exploding wire array on the MAGPIE facility (1.4 MA, 240 ns). Ablation of plasma from the wire array generates radially diverging, supersonic ($M_S \sim 7$), super-Alfvénic ($M_A > 1$) magnetized flows with frozen-in magnetic flux ($R_M \gg 1$). These flows collide with an inductive probe placed in the flow, which serves both as the obstacle that generates the magnetized bow shock, and as a diagnostic of the advected magnetic field. Laser interferometry along two orthogonal lines of sight is used to measure the line-integrated electron density. A detached bow shock forms ahead of the probe, with a larger opening angle in the plane parallel to the magnetic field than in the plane normal to it. Since the resistive diffusion length of the plasma is comparable to the probe size, the magnetic field decouples from the ion fluid at the shock front and generates a hydrodynamic shock, whose structure is determined by the sonic Mach number, rather than the magnetosonic Mach number of the flow. 3D simulations performed using the resistive magnetohydrodynamic (MHD) code GORGON confirm this picture, but under-predict the anisotropy observed in the shape of the experimental bow shock, suggesting that non-MHD mechanisms may be important for modifying the shock structure.