We perform bifurcation analysis of a two-dimensional magnetic Rayleigh-B\'enard problem using a numerical technique called deflated continuation. Our aim is to study the influence of the magnetic field on the bifurcation diagram as the Chandrasekhar number $Q$ increases, and compare it to the standard (non-magnetic) Rayleigh-B\'enard problem. We compute steady states at a high Chandrasekhar number of $Q=10^3$ over a range of the Rayleigh number $0\leq \text{Ra}\leq 10^5$. These solutions are obtained by combining deflation with a continuation of steady states at low Chandrasekhar number, which allows us to explore the influence of the strength of the magnetic field as $Q$ increases from low coupling, where the magnetic effect is almost negligible, to strong coupling at $Q=10^3$. We discover a large profusion of states with rich dynamics and observe a complex bifurcation structure with several pitchfork, Hopf and saddle-node bifurcations. Our numerical simulations show that the onset of bifurcations in the problem is delayed when $Q$ increases, while solutions with fluid velocity patterns aligning with the background vertical magnetic field are privileged. Additionally, we report a branch of states that stabilizes at high magnetic coupling, suggesting that one may take advantage of the magnetic field to discriminate solutions.
翻译:我们对二维磁性Rayleigh-B\'enard问题进行两维磁性Rayleigh-B\'enard 问题进行双向分析,使用所谓的减缩后继技术。我们的目标是研究磁场对双向图的影响,因为Chandrashekhar 的金额会随着Chandrasekhar 的美元增长而增加,并且把它与标准(非磁性)Rayleigh-B\'enard 问题相比较。我们计算出一个高Chandrasekhar 的10美分的稳态。我们发现,在Rayleley 的数种数字中,10美分是10美分的10美分。这些解决方案是通过通货通货与稳定状态的恒定状态结合而获得的。我们的数字模拟显示,磁场的力量是QQQ的强度会随着低位的组合而增加,而磁性磁力变化的开始时间会推迟。