The periodic $μ$-$b$-equation and Euler equations on the circle

In this paper, we study the $μ$-variant of the periodic $b$-equation and show that this equation can be realized as a metric Euler equation on the Lie group $\Diff^{\infty}(§)$ if and only if $b=2$ (for which it becomes the $μ$-Camassa-Holm equation). In this case, the inertia operator generating the metric on $\Diff^{\infty}(§)$ is given by $L=μ-\partial_x^2$. In contrast, the $μ$-Degasperis-Procesi equation (obtained for $b=3$) is not a metric Euler equation on $\Diff^{\infty}(§)$ for any regular inertia operator $A\in\mathcal L_{\text{is}}^{\text{sym}}(C^{\infty}(§))$. The paper generalizes some recent results of [J. Escher and B. Kolev, DOI 10.1007/s00209-010-0778-2], [J. Escher and J. Seiler, J. Math. Phys. 51 (2010), 053101.1-053101.6] and [B. Kolev, Wave Motion 46 (2009), 412-419].

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