Consider a class of planar autonomous differential systems with cylindric phase space which represent generalized pendulum equations. We describe a method to construct such systems with prescribed maximum number of limit cycles which are not contractible to a point (limit cycles of the second kind). The underlying idea consists in employing Dulac-Cherkas functions. We also show how this approach can be used to control the bifurcation of multiple limit cycles
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
summary:We consider limit cycles of a class of polynomial differential systems of the form $$ \begin...
summary:The two-parameter Hamiltonian system with the autonomous perturbation is considered. Via the...
Consider a class of planar autonomous differential systems with cylindric phase space which represen...
We consider a generalized pendulum equation depending on the scalar parameter $\mu$ having for $\mu...
We present a new approach to study limit cycles of planar systems of autonomous differential equatio...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
Consider the class of planar systems fracdxdt=y,quadfracdydt=−x+musumj=03hj(x,mu)yj depending on the...
We consider autonomous systems with cylindrical phase space. Lower and upper bounds for the number o...
We present a new approach for the global bifurcation analysis of limit cycles for a generalized van ...
We consider two-dimensional smooth vector fields $dx/dt = P(x,y), dy/dt = Q(x,y)$ and estimate the m...
We consider a generalized pendulum equation depending on the scalar parameter $\mu$ having for $\mu=...
We consider planar autonomous systems dx/dt =P(x,y,λ), dy/dt =Q(x,y,λ) depending on a scalar paramet...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
summary:We consider limit cycles of a class of polynomial differential systems of the form $$ \begin...
summary:The two-parameter Hamiltonian system with the autonomous perturbation is considered. Via the...
Consider a class of planar autonomous differential systems with cylindric phase space which represen...
We consider a generalized pendulum equation depending on the scalar parameter $\mu$ having for $\mu...
We present a new approach to study limit cycles of planar systems of autonomous differential equatio...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
Consider the class of planar systems fracdxdt=y,quadfracdydt=−x+musumj=03hj(x,mu)yj depending on the...
We consider autonomous systems with cylindrical phase space. Lower and upper bounds for the number o...
We present a new approach for the global bifurcation analysis of limit cycles for a generalized van ...
We consider two-dimensional smooth vector fields $dx/dt = P(x,y), dy/dt = Q(x,y)$ and estimate the m...
We consider a generalized pendulum equation depending on the scalar parameter $\mu$ having for $\mu=...
We consider planar autonomous systems dx/dt =P(x,y,λ), dy/dt =Q(x,y,λ) depending on a scalar paramet...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
Dulac-Cherkas functions can be used to derive an upper bound for the number of limit cycles of plana...
summary:We consider limit cycles of a class of polynomial differential systems of the form $$ \begin...
summary:The two-parameter Hamiltonian system with the autonomous perturbation is considered. Via the...