TY - JOUR
T1 - Forcing an entire bifurcation diagram
T2 - Case studies in chemical oscillators
AU - Kevrekidis, I. G.
AU - Aris, R.
AU - Schmidt, L. D.
N1 - Funding Information:
This work was partiallys upportebdy NSF grant no. CPE 83-13497a nd the U.S. Departmenot f Energy.
PY - 1986/12
Y1 - 1986/12
N2 - We study the finite amplitude periodic forcing of chemical oscillators. In particular, we examine systems that, when autonomous, (i.e. for zero forcing amplitude) exhibit a single stable oscillation. Using one of the system parameters as a forcing variable by varying it periodically, we show through extensive numerical work how the bifurcation diagram of the autonomous system with respect to this parameter affects the qualitative response of the full forced system. As the forcing variable oscillates around its midpoint, its instantaneous values may cross points (such as Hopf bifurcation poiints) of the autonomous bifurcation diagram so that the characterization of the system as a simple forced oscillator is no longer valid. Such a neighboring Hopf bifurcation of the unforced system is found to set the scene for the interaction of resonance horns and the loss of tori in the full forced system as the amplitude of the forcing grows. Our test case presented here is the Continuous Stirred Tank Reactor (CSTR) with periodically forced coolant temperature.
AB - We study the finite amplitude periodic forcing of chemical oscillators. In particular, we examine systems that, when autonomous, (i.e. for zero forcing amplitude) exhibit a single stable oscillation. Using one of the system parameters as a forcing variable by varying it periodically, we show through extensive numerical work how the bifurcation diagram of the autonomous system with respect to this parameter affects the qualitative response of the full forced system. As the forcing variable oscillates around its midpoint, its instantaneous values may cross points (such as Hopf bifurcation poiints) of the autonomous bifurcation diagram so that the characterization of the system as a simple forced oscillator is no longer valid. Such a neighboring Hopf bifurcation of the unforced system is found to set the scene for the interaction of resonance horns and the loss of tori in the full forced system as the amplitude of the forcing grows. Our test case presented here is the Continuous Stirred Tank Reactor (CSTR) with periodically forced coolant temperature.
UR - http://www.scopus.com/inward/record.url?scp=0000573221&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0000573221&partnerID=8YFLogxK
U2 - 10.1016/0167-2789(86)90145-4
DO - 10.1016/0167-2789(86)90145-4
M3 - Article
AN - SCOPUS:0000573221
SN - 0167-2789
VL - 23
SP - 391
EP - 395
JO - Physica D: Nonlinear Phenomena
JF - Physica D: Nonlinear Phenomena
IS - 1-3
ER -