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Parametric instability in a rotating cylinder of gas subject to sinusoidal axial compression. Part 2. Weakly nonlinear theory

机译:正弦轴向压缩的气体旋转气缸中的参数不稳定性。第2部分。弱非线性理论

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A weakly nonlinear analysis is presented of parametric instability in a rotating cylinder subject to periodic axial compression by small sinusoidal oscillations of one of its ends (the piston'). Amplitude equations are derived for the pair of parametrically resonant (primary) inertial modes which were found to arise from linear instability in Part 1. These equations introduce an infinity of geostrophic mode amplitudes, representing a nonlinear modification of the mean flow, for which evolution equations are also derived. Consequences of the total system of equations are investigated for axisymmetric modes. Different possible outcomes are found at large times: (a) a fixed point, representing a saturated state in which the oscillatory toroidal vortices of the primary mode are phase-locked to the piston motion with half its frequency; (b) a limit cycle or chaotic attractor, corresponding to slow-time oscillations of the primary mode; or (c) exponential divergence of the amplitudes to infinity. The latter outcome, a necessary condition for which is derived in the form of a threshold piston amplitude for divergence, invalidates the theory, inducing a gross change in the character of the flow and providing a route out of the weakly nonlinear regime. Non-zero fixed-point branches arise via bifurcations from both sides of the linear neutral curve, where the basic flow changes local stability. The lower-amplitude branch is shown to be unstable, while the upper one may lose local stability, resulting in a Hopf bifurcation to a limit cycle, which can subsequently become aperiodic via a series of further bifurcations. Typically, during the resulting oscillations, whether periodic or not, the perturbation first grows from small amplitude owing to basic-flow instability, then nonlinear detuning of the parametric resonance causes decay back to small amplitude in the second half of the cycle, which then restarts.
机译:提出了一个弱非线性分析,它对旋转汽缸的参数不稳定性进行了周期性的轴向压缩,该汽缸的一端(活塞)之一发生小正弦振动。对于在第1部分中发现的线性不稳定性引起的一对参数共振(主)惯性模式,得出了振幅方程。这些方程引入了地转模式振幅的无穷大,代表了平均流的非线性修正,为此,发展方程也得出。对于轴对称模式,研究了整个方程组的结果。经常会发现不同的可能结果:(a)一个固定点,表示一个饱和状态,在该状态下,主模式的振荡环形涡旋以一半的频率锁相到活塞运动; (b)极限周期或混沌吸引子,对应于初级模式的慢速振荡; (c)振幅到无穷大的指数散度。后者的结果(以发散的阈值活塞振幅的形式得出的必要条件)使该理论无效,从而导致流动特性发生重大变化并提供了从弱非线性状态中脱颖而出的途径。非零定点分支是通过线性中性曲线两侧的分叉产生的,基本流量会改变局部稳定性。较低幅度的分支显示为不稳定,而较高幅度的分支可能会失去局部稳定性,从而导致Hopf分叉达到极限循环,随后可能会通过一系列进一步的分叉变为非周期性。通常,在产生的振荡过程中,无论是否周期性发生振荡,由于基本流的不稳定性,扰动首先从小振幅开始增大,然后参数共振的非线性失谐导致在周期的后半段衰减回到小振幅,然后重新开始。

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