A Sinusoidally Driven Lorenz System and Circuit Implementation

<div><svg height="9.50777pt" id="M61" style="vertical-align:-0.70224pt" version="1.1" viewbox="-0.0498162 -8.80553 30.3117 9.50777" width="30.3117pt" 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="M610 0V27L347 666L316 657L46 26V0H610ZM504 54H116L310 537L504 54Z" id="g50-133"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="654" vert-adv-y="654"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,12.171,0)"><path d="M530 -6V57L144 261V263L530 468V530L81 290V234L530 -6Z" id="g54-91"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="611" vert-adv-y="611"></glyph.data></g><g transform="matrix(.013,0,0,-0.013,23.79,0)"><path d="M245 635C92 635 37 457 37 312C37 148 92 -12 244 -12C395 -12 449 165 449 312C449 469 394 635 245 635ZM243 598C332 598 358 454 358 312C358 172 334 26 245 26C158 26 128 174 128 313S151 598 243 598Z" id="g58-46"></path><glyph.data ascent="1007" descent="-369" horiz-adv-x="487" vert-adv-y="487"></glyph.data></g></svg> with time evolution for two-wing hyperchaotic attractor.</div>

Mathematical Problems in Engineering

A Sinusoidally Driven Lorenz System and Circuit Implementation

Figure 4