Lorenz attractor system is a system of ordinary differential equations first studied by mathematician and meteorologist Edward Lorenz attractor.
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Lorenz attractor system is a system of ordinary differential equations first studied by mathematician and meteorologist Edward Lorenz attractor.
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In particular, the Lorenz attractor is a set of chaotic solutions of the Lorenz system.
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Lorenz attractor equations arise in simplified models for lasers, dynamos, thermosyphons, brushless DC motors, electric circuits, chemical reactions and forward osmosis.
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The Lorenz attractor equations are the governing equations in Fourier space for the Malkus waterwheel.
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From a technical standpoint, the Lorenz attractor system is nonlinear, aperiodic, three-dimensional and deterministic.
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The Lorenz attractor equations have been the subject of hundreds of research articles, and at least one book-length study.
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Lorenz attractor is difficult to analyze, but the action of the differential equation on the attractor is described by a fairly simple geometric model.
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In Figure 4 of his paper, Lorenz attractor plotted the relative maximum value in the z direction achieved by the system against the previous relative maximum in the direction.
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Lorenz attractor found that when the maximum value is above a certain cut-off, the system will switch to the next lobe.
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The Lorenz attractor equations are derived from the Oberbeck–Boussinesq approximation to the equations describing fluid circulation in a shallow layer of fluid, heated uniformly from below and cooled uniformly from above.
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Solution in the Lorenz attractor rendered as a metal wire to show direction and 3D structure.
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