2019
DOI: 10.1142/s0218127419300428
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Hopf Bifurcations, Periodic Windows and Intermittency in the Generalized Lorenz Model

Abstract: In the present study, we analyze the dynamics of a four-dimensional generalized Lorenz system with one variable describing the profile of the magnetic field induced in a convected magnetized fluid. In particular, we identify the subcritical Hopf bifurcation, at which the dimension of the unstable manifold is increased or reduced by two. Moreover, the new four-dimensional system behavior depending on the control parameters is considered and bidirectional bifurcation structures are revealed. The results show the… Show more

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Cited by 7 publications
(5 citation statements)
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“…which occurs with w ∈ R in the Lorenz-Stenflo model from Stenflo (1996), its magnetic variant (Wawrzaszek and Krasinska 2019), and with w ∈ R 2 in the models from Molteni et al (1993); for the latter we choose α = O(ε) and shift the auxiliary variables (which gives b = 0) to obtain the form ( 47). An extension of Lorenz-Stenflo with nonlinear additional equations is considered in Moon et al (2021), but still fits into the present framework when, e.g., scaling the variables in addition to Lorenz-Stenflo with j = 3 and choosing Lewis number of order ε −2 .…”
Section: Other Lorenz-like Systemsmentioning
confidence: 99%
“…which occurs with w ∈ R in the Lorenz-Stenflo model from Stenflo (1996), its magnetic variant (Wawrzaszek and Krasinska 2019), and with w ∈ R 2 in the models from Molteni et al (1993); for the latter we choose α = O(ε) and shift the auxiliary variables (which gives b = 0) to obtain the form ( 47). An extension of Lorenz-Stenflo with nonlinear additional equations is considered in Moon et al (2021), but still fits into the present framework when, e.g., scaling the variables in addition to Lorenz-Stenflo with j = 3 and choosing Lewis number of order ε −2 .…”
Section: Other Lorenz-like Systemsmentioning
confidence: 99%
“…which occurs with w ∈ R in the Lorenz-Stenflo model from [24], its magnetic variant [26], and with w ∈ R 2 in the models from [12]; for the latter we choose α = O(ε) and shift the auxiliary variables (which gives b = 0) to obtain the form (47). An extension of Lorenz-Stenflo with nonlinear additional equations is considered in [13], but still fits into the present framework when, e.g., scaling the variables in addition to Lorenz-Stenflo with j = 3 and choosing Lewis number of order ε −2 .…”
Section: Other Lorenz-like Systemsmentioning
confidence: 99%
“…This range corresponds to the values λ > 2/3 on the left-hand side of (27). Also, every k 1 ∈ (k * , 1) gives a unique positive value for B via formula (26).…”
mentioning
confidence: 99%
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“…As the theory of bifurcation is a tool to help to understand equilibrium loss and its consequences for complex behavior. There are many types of periodic orbit local bifurcation such as period-doubling bifurcation, and Hopf bifurcation [20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%