The role of shocks and the velocity gradient in the relative orientation of the magnetic field and dense gas clouds
Context. Magnetic fields are known to exhibit different relative orientations with density structures in different density regimes. However, the physical mechanisms behind these relative orientations remain unclear.Aims. We investigate the role of the flow features on the relative orientation between the magnetic field and cold neutral medium (CNM) clouds, as well as that of molecular clouds (MCs) as a corollary.Methods. We performed three- and two-dimensional (3D+2D) magnetohydrodynamic (MHD) simulations of warm gas streams in the thermally bistable atomic interstellar medium (ISM) colliding with velocities of the order of the velocity dispersion in the ISM to form CNM clouds. In these simulations, we followed the evolution of magnetic field lines to identify and elucidate the physical processes behind their evolution.Results. The collision produces a fast MHD shock, as well as a condensation front roughly one cooling length behind it, on each side of the collision front. A compressive, decelerating velocity field arises between the shock and the condensation fronts, and a cold dense layer forms behind the condensation front. The magnetic field lines, initially oriented parallel to the flow direction, are perturbed by the fast MHD shock, across which the magnetic field fluctuations parallel to the shock front are amplified. The downstream perturbations of the magnetic field lines are further amplified by the compressive downstream velocity gradient between the shock and the condensation front caused by the settlement of the gas onto the dense layer. This process causes the magnetic field to become progressively aligned with the dense layer, leading to the formation of a shear flow around it, due to the field’s backreaction on the flow. By extension, we suggest that a tidal stretching velocity gradient, such as that produced in gas infalling into a self-gravitating structure, must straighten the field lines along the accretion flow, orienting them perpendicular to the density structures. We also find that the initially super-Alfvénic upstream flow becomes trans-Alfvénic between the shock and the condensation front, and then sub-Alfvénic inside the condensation. Finally, in 2D simulations with a curved collision front, the presence of the magnetic field inhibits the generation of turbulence by the shear around the dense layer.Conclusions. Our results provide a feasible physical mechanism for orienting the magnetic field parallel to CNM clouds through the action of fast MHD shocks and compressive velocity fields.
Memo
- 原子ガス→分子ガスや、分子雲内部など、細長い高密度構造では磁場は平行から垂直へ向きを変える
- WNMは熱的不安定を起こすような強力な冷却によって密度ジャンプを伴ってCNMとなり、これはガスを蓄積し続け分子を形成するのに十分な自己遮蔽性を持つようになり、自己重力に支配されて分子雲の祖先となる
- 磁場と密度構造の向きΦは以下で表される(Soler & Hennebelle 2017)
- 暖かい原子ガスの衝突で生じる冷たい分子ガスの衝撃面に対し、外側にある磁場は最初は垂直だが、衝撃面に近づくにつれて曲がり、一部は平行に近い角度になる
- 密度範囲全体で、磁場はガスに対しcosΦ = 0(垂直)となる
- ガスの密度が増加するほど、磁場はガスに対し平行でなくなる
- スーパーファストMHDショックでは衝撃面に対し平行な磁場が増大するという特徴がある(Delmont&Keppens 2011)
- By = By(x), Bx =const, ux = ux(x), with ∂ux/∂x < 0, uy, uz → 0では以下のように表されるので、磁場成分Byは常に下流の圧縮速度勾配によって増幅され、この増幅は、CNM雲が形成される凝縮面に対して磁場が平行になる結果をもたらす
\frac{DB_y}{Dt} = -B_y \frac{\partial u_x}{\partial x}, ~ \frac{\partial u_x}{\partial x} < 0
- 自己重力によるByに対する寄与では上式で∂ux/∂x > 0となり、二つの寄与を合わせると衝撃面で0° < Φ < 90°となる
- 密な層を横切るせん断流によって生じる渦度に対し、磁気張力が乱流の生成を抑える可能性がある