TY - GEN
T1 - The attractors in the complex Lorenz model
AU - Gómez-Mont, Xavier
AU - Flores-Godoy, José Job
AU - Fernández-Anaya, Guillermo
PY - 2012
Y1 - 2012
N2 - We address the question of finding the attractors of the complex Lorenz model (CLM), which is obtained by extending the space from R3 to C3, and defining the model by the same equations as the classical Lorenz model (LM). We have numerical evidence of 2 strong attractors un-related to the Lorenz attractor. We calculate its Lyapunov exponents and show that 2 of them are 0, and the other 4 are double and negative. Hence the attractors are non-chaotic. We show that they have a quasi-periodic nature. To decipher the structure of these attractors, we introduce the imaginary Lorenz model (ILM), which is defined in the same space C3 by multiplying with i = √-1 the Lorenz equations. Both models locally commute, and with its help we account for the double Lyapunov exponent 0 and show that the basin of attraction of each attractor is a big open set of C3. The chaotic limit set Lℂ ∪ ℂ3 obtained from the classical Lorenz attractor L0 of (LM) by moving it with the (ILM) has 2 positive Lyapunov exponents, but only captures a set of 6D-volume 0 in its basin of attraction.
AB - We address the question of finding the attractors of the complex Lorenz model (CLM), which is obtained by extending the space from R3 to C3, and defining the model by the same equations as the classical Lorenz model (LM). We have numerical evidence of 2 strong attractors un-related to the Lorenz attractor. We calculate its Lyapunov exponents and show that 2 of them are 0, and the other 4 are double and negative. Hence the attractors are non-chaotic. We show that they have a quasi-periodic nature. To decipher the structure of these attractors, we introduce the imaginary Lorenz model (ILM), which is defined in the same space C3 by multiplying with i = √-1 the Lorenz equations. Both models locally commute, and with its help we account for the double Lyapunov exponent 0 and show that the basin of attraction of each attractor is a big open set of C3. The chaotic limit set Lℂ ∪ ℂ3 obtained from the classical Lorenz attractor L0 of (LM) by moving it with the (ILM) has 2 positive Lyapunov exponents, but only captures a set of 6D-volume 0 in its basin of attraction.
KW - Chaos
KW - Complex systems
KW - Differential equations
KW - Dynamic model
KW - Nonlinear analysis
KW - Nonlinear equations
UR - http://www.scopus.com/inward/record.url?scp=84880993913&partnerID=8YFLogxK
U2 - 10.3182/20120620-3-MX-3012.00007
DO - 10.3182/20120620-3-MX-3012.00007
M3 - Contribución a la conferencia
AN - SCOPUS:84880993913
SN - 9783902823021
T3 - IFAC Proceedings Volumes (IFAC-PapersOnline)
SP - 87
EP - 92
BT - 3rd IFAC Conference on Analysis and Control of Chaotic Systems, CHAOS 2012
PB - IFAC Secretariat
T2 - 3rd IFAC Conference on Analysis and Control of Chaotic Systems, CHAOS 2012
Y2 - 20 June 2012 through 22 June 2012
ER -