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Intermittent chaos in the Bray-Liebhafsky oscillator. Temperature dependence

机译:Bray-Liebhafsky振荡器中的间歇性混乱。温度依赖性

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Intermittent oscillations as a chaotic mixture of large amplitude relaxation oscillations, grouped in bursts and small-amplitude sinusoidal ones or even quiescent parts between them known as gaps, were found and examined in the Bray-Liebhafsky (BL) reaction performed in CSTR under controlled temperature variations. They were obtained in a narrow temperature range from 61.0 degrees C to 63.1 degrees C, where 61.0 degrees C is the critical temperature for burst emergence from the stable steady state and 63.1 degrees C is the critical temperature for gap emergence from regular oscillations. Since intermittencies appear gradually from the regular oscillatory state, and no hysteresis was obtained with decreasing/increasing temperature in the vicinity of these two bifurcations, a linear relationship between (tau(B)/tau)(2) and (tau(G)/tau)(2) (where tau(B), tau(G) and tau denotes duration of bursts, gaps, and whole experiment, respectively), as a function of the temperature as the control parameter, was expected and obtained. Although these intermittent oscillations are chaotic with respect to the lengths of individual gaps as well as bursts, their deterministic behavior related to temperature was additionally established. Thus, the number of bursts or gaps per unit of time (N-B/tau and N-G/tau) has the form of a normal distribution function over the temperature range in the region where intermittencies are obtained. Temperature dependence of the Lyapunov exponents was also described by a function of the normal distribution form. Hence, we established some regularities in the chaotic behavior of intermittent oscillations that are common in life but difficult for determinations.
机译:在可控温度下在CSTR中进行的Bray-Liebhafsky(BL)反应中发现并检查了间歇振动,该间歇振动是大振幅弛豫振荡的混沌混合物,分为脉冲串和小振幅正弦波,甚至它们之间的静止部分也称为间隙。变化。它们是在61.0摄氏度到63.1摄氏度的狭窄温度范围内获得的,其中61.0摄氏度是从稳定稳态爆发的临界温度,而63.1摄氏度是从规则振荡产生的间隙的临界温度。由于间断性是从规则的振荡状态逐渐出现的,并且在这两个分叉附近,随着温度的升高/降低,没有磁滞现象发生,因此(tau(B)/ tau)(2)和(tau(G)/ tau(2)(其中tau(B),tau(G)和tau分别表示爆发,间隙和整个实验的持续时间),它是温度作为控制参数的函数。尽管这些间歇性振荡相对于各个间隙的长度以及突发来说是混乱的,但还是建立了与温度有关的确定性行为。因此,每单位时间的突发或间隙的数量(N-B / tau和N-G / tau)在获得间歇性的区域内的温度范围内具有正态分布函数的形式。 Lyapunov指数的温度依赖性还通过正态分布形式来描述。因此,我们在生活中常见但难以确定的间歇振荡的混沌行为中建立了一些规律。

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