Classification of parameters | Stability of the zero solution |
$ b>0 $ | upper unstable and lower stable |
$ b=0, a>0 $ | upper stable and lower stable |
$ a=b=0, c>0 $ | upper unstable and lower stable |
$ a=b=0, c<0 $ | upper stable and lower unstable |
In this paper, the existence and number of non-contractible limit cycles of the Josephson equation $ \beta \frac{d^{2}\Phi}{dt^{2}}+(1+\gamma \cos \Phi)\frac{d\Phi}{dt}+\sin \Phi = \alpha $ are studied, where $ \phi\in \mathbb S^{1} $ and $ (\alpha,\beta,\gamma)\in \mathbb R^{3} $. Concretely, by using some appropriate transformations, we prove that such type of limit cycles are changed to limit cycles of some Abel equation. By developing the methods on limit cycles of Abel equation, we prove that there are at most two non-contractible limit cycles, and the upper bound is sharp. At last, combining with the results of the paper (Chen and Tang, J. Differential Equations, 2020), we show that the sum of the number of contractible and non-contractible limit cycles of the Josephson equation is also at most two, and give the possible configurations of limit cycles when two limit cycles appear.
Citation: |
Table 1. Stability of the zero solution of equation (4)
Classification of parameters | Stability of the zero solution |
$ b>0 $ | upper unstable and lower stable |
$ b=0, a>0 $ | upper stable and lower stable |
$ a=b=0, c>0 $ | upper unstable and lower stable |
$ a=b=0, c<0 $ | upper stable and lower unstable |
Table 2. Stability of system (4) at infinity
Region | Classification of parameters | Stability of $ y=+\infty $ | Stability of $ y=-\infty $ |
$ S_{1} $ | $ 0<b<\psi_{2}(a,c),0<a<a_{*},c<0 $ | unstable | stable |
$ S_{2} $ | $\begin{gathered}\psi_{2}(a,c)<b<\varphi(a,c),0<a<a_{*},c<0 \\ 0<b<\varphi(a,c),a_{*}\leq a<1,c<0\end{gathered}$ | unstable | unstable |
$ S_{3} $ | $\begin{gathered}\varphi(a,c)<b<\psi_{1}(a,c),0<a<a^{*},c<0 \\ \varphi(a,c)<b<-c\sqrt{1-a^{2}},a^{*}\leq a<1,c<0\end{gathered}$ | unstable | unstable |
$ S_{4} $ | $ \psi_{1}(a,c)<b<-c\sqrt{1-a^{2}},0<a<a^{*},c<0 $ | stable | unstable |
$ S_{5} $ | $\begin{gathered}b\geq-c\sqrt{1-a^{2}},0<a<a^{*},c<0 \\ b>\psi_{1}(a,c),a^{*}\leq a<1,c<0 \\ b> \max \{\psi_{1}(a,c),0\},0<a<1,c\geq0\end{gathered}$ | stable | unstable |
$ S_{6} $ | $\begin{gathered}-c\sqrt{1-a^{2}}\leq b<\psi_{1}(a,c),a^{*}<a<1,c<0 \\ 0<b<\psi_{1}(a,c),0<a<1,c\geq0\end{gathered}$ | unstable | unstable |
$ S_{7} $ | $ a>1 $ | unstable | unstable |
$ HL $ | $ b=\varphi(a,c),0<a<1,c<0 $ | unstable | unstable |
$ SC_{11} $ | $\begin{gathered}b=\psi_{1}(a,c),a^{*}\leq a<1,c<0 \\ b=\psi_{1}(a,c),0<a<1,c\geq0\end{gathered}$ | - | unstable |
$ SC_{12} $ | $ b=\psi_{1}(a,c),0<a<a^{*},c<0 $ | - | unstable |
$ SC_{2} $ | $ b=\psi_{2}(a,c),0<a<a_{*}<1,c<0 $ | unstable | - |
$ P_{1} $ | $ a=1,b=\psi_{1}(1,c),c<0 $ | - | unstable |
$ SN_{1} $ | $ a=1,b>\psi_{1}(1,c) $ | stable | unstable |
$ SN_{2} $ | $ a=1,0<b<\psi_{1}(1,c) $ | unstable | unstable |
$ BT $ | $ a=1,b=0,c<0 $ | unstable | unstable |
$ HLC $ | $ 0<a<1,b=c=0 $ | unstable | unstable |
$ HE $ | $ a=0,b=\varphi(0,c),c<0 $ | - | - |
Table 3.
Sign of
Ⅰ | Ⅱ | Ⅲ | Ⅳ | Ⅴ | |
$ \sin x-a $ | + | + | - | - | + |
$ y+\frac{f(x)}{g(x)} $ | + | - | + | - | + |
$ \frac{dy}{dx} $ | + | - | - | + | + |
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Cross-sections of the bifurcation diagram of system (3)
Phase portrait of
Stability at infinity for
Stability at infinity for
Relationship between the functions
Solution curve of equation (4) when
Solution curve of equation (4) when
Solution curve of equation (26) when
Numerical limit cycle of equation (1)