Chaos in Essentially Singular 3D Dynamical Systems with Two Quadratic Nonlinearities

<div>The phase portrait of a quasi-periodic behavior (a) and the graph of the function <svg height="12.7178pt" id="M290" style="vertical-align:-3.42947pt" version="1.1" viewbox="-0.0498162 -9.28833 20.6122 12.7178" width="20.6122pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M516 277C516 378 460 448 376 448C335 448 288 434 240 401C158 345 127 277 107 159C53 -161 38 -221 23 -247L28 -261C43 -260 95 -250 114 -226C122 -216 129 -199 146 -75C152 -29 157 0 164 31C182 9 206 -12 237 -12C267 -12 325 8 376 46C451 102 516 179 516 277ZM432 259C432 134 366 40 259 40C236 40 204 48 171 76L195 203C219 327 253 400 326 400C398 400 432 336 432 259Z" id="g113-239"></path><glyph.data ascent="3473" descent="-2876" horiz-adv-x="539" vert-adv-y="539"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,7.01,0)"><path d="M300 -147C201 -63 143 98 143 270S200 602 300 686L282 710C136 610 70 450 70 271V270C70 89 136 -72 282 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Journal of Nonlinear Dynamics

fig1

Figure 1

Figure 1: Chaos in Essentially Singular 3D Dynamical Systems with Two Quadratic Nonlinearities 