Research Article

Motion Switching and Chaos of a Particle in a Generalized Fermi-Acceleration Oscillator

Table 2

Initial conditions for periodic motions ( 𝑚 1 = 0 . 0 1 , 𝑚 2 = 1 , 𝑘 = 1 0 , 𝑐 = 6 , 𝑒 1 = 0 . 9 , = 1 , 𝑄 = 0 . 5 ).

Mapping ( Ω , 𝑒 2 ) Initial time 𝑡 0 ( 𝑥 ( 1 ) 0 , ̇ 𝑥 ( 1 ) 0 ) ( 𝑥 ( 2 ) 0 , ̇ 𝑥 ( 2 ) 0 )

𝑃 3 2 0 ( 6 . 5 , 0 . 0 1 ) 0 . 7 0 4 9 0 6 1 4 ( 0 . 3 8 7 5 5 0 4 3 , 1 . 9 7 6 8 2 1 4 0 ) ( 0 . 3 8 7 5 5 0 4 3 , 1 . 9 7 6 8 2 1 4 0 )
𝑃 3 2 ( 1 1 . 8 , 0 . 0 1 ) 0 . 5 1 0 3 5 8 9 0 ( 0 . 0 1 4 2 2 2 3 5 , 0 . 8 7 7 1 9 8 9 7 ) ( 0 . 0 1 4 2 2 2 3 5 , 2 . 8 3 3 0 4 4 6 4 )
𝑃 ( 2 1 3 ) ( 6 . 7 , 0 . 7 ) 0 . 0 7 4 1 6 3 3 1 ( 1 . 0 , 5 . 4 1 0 4 8 8 8 4 ) ( 0 . 3 2 8 0 3 5 0 6 , 1 . 1 5 0 4 4 5 9 4 )
𝑃 ( 2 1 3 ) 2 ( 6 . 5 , 0 . 7 ) 0 . 0 8 3 4 7 1 5 3 ( 1 . 0 , 5 . 5 4 8 7 8 7 1 0 ) ( 0 . 3 4 7 3 0 0 3 6 , 0 . 9 8 8 0 1 5 0 3 )
𝑃 1 2 ( 2 2 . 7 , 0 . 7 ) 0 . 0 8 6 9 9 3 2 8 ( 1 . 0 , 8 . 1 1 2 9 8 1 9 6 ) ( 0 . 0 4 0 5 9 7 2 7 , 1 . 6 4 9 2 9 0 8 9 )
𝑃 ( 1 2 ) 2 ( 2 0 . 4 , 0 . 7 ) 0 . 3 9 9 7 5 7 7 6 ( 1 . 0 , 8 . 1 7 5 7 1 9 6 3 ) ( 0 . 0 7 1 0 2 0 9 8 , 1 . 4 4 7 9 0 3 2 8 )