Chaotic signal source with adjustable dynamic amplitude linearity
A chaotic signal and amplitude technology, which is applied in the field of chaotic signal sources, can solve the problems of linear change in the dynamic range of the output chaotic signal and the inability to realize linear adjustment of the dynamic amplitude, and achieve good consistency
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[0032] See Figure 1-8 , the mathematical model of a dynamic amplitude linearly adjustable chaotic signal source in this embodiment can be described as:
[0033] (2)
[0034] where a, b and c are all real numbers. make , formula (2) can be rewritten as follows:
[0035] (3)
[0036] make , there are two equilibrium points in formula (3): S1:(-c / b,0,0), S2:(c / b,0,0). At the equilibrium point S*=(x*, y*, z*), the equation (3) is linearized, and the Jacobian matrix is obtained as:
[0037] (4)
[0038] From formula (4), the characteristic root equation of system (3) can be obtained as:
[0039] (5)
[0040] For the equilibrium point S 1 :(c / b,0,0), its characteristic root equation can be simplified as , according to the Routh-Horwitz criterion, when a, b>0, and a1 is unstable. When a=0.4, b=0.81, c=4, find S 1 : The characteristic root of (-4.9383,0,0) is
[0041]
[0042]...
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