Abstract
Abstract This article discusses the rotations (windings) of solutions to the basic system of equations y ′ = F 1 ( x , y ) {y^{\prime}=F_{1}(x,y)} and x ′ = F 2 ( x , y ) {x^{\prime}=F_{2}(x,y)} . This allows us to return to the topic of known limit cycles from a much broader point of view, in particular, it makes it possible to describe the conditions for the existence of limit cycles.
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