Research Article

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

Figure 19

Phase planes. Solid and dashed curves represent motions of particle and piston, respectively, ( 𝑚 1 = 0 . 0 1 , 𝑚 2 = 1 , 𝑘 = 1 0 , 𝑐 = 6 , 𝑒 1 = 0 . 9 , 𝑄 = 0 . 5 ): (a) 𝑃 0 3 2 ( Ω = 6 . 5 , 𝑒 2 = 0 . 0 1 ) ( 𝑡 0 = 0 . 7 0 4 4 2 2 8 2 , 𝑥 ( 1 ) 0 = 𝑥 ( 2 ) 0 = 0 . 3 8 7 5 5 0 4 3 , ̇ 𝑥 ( 1 ) 0 = 1 . 9 0 5 2 7 8 1 2 , ̇ 𝑥 ( 2 ) 0 = 1 . 9 6 8 9 5 9 7 0 ), (b) 𝑃 3 2 ( Ω = 1 1 . 8 , 𝑒 2 = 0 . 0 1 ) ( 𝑡 0 = 0 . 5 1 0 3 5 8 9 0 , 𝑥 ( 1 ) 0 = 𝑥 ( 2 ) 0 = 0 . 0 1 4 2 2 2 3 5 , ̇ 𝑥 ( 1 ) 0 = 0 . 8 7 7 1 9 8 9 7 , ̇ 𝑥 ( 2 ) 0 = 2 . 8 3 3 0 4 4 6 4 ), (c) 𝑃 ( 2 1 3 ) ( Ω = 6 . 7 , 𝑒 2 = 0 . 7 ) ( 𝑡 0 = 0 . 0 7 4 1 6 3 3 1 , 𝑥 ( 1 ) 0 = 1 . 0 , ̇ 𝑥 ( 1 ) 0 = 5 . 4 1 0 4 8 8 8 4 , 𝑥 ( 2 ) 0 = 0 . 3 2 8 0 3 5 0 6 , ̇ 𝑥 ( 2 ) 0 = 1 . 1 5 0 4 4 5 9 4 ), (d) 𝑃 ( 2 1 3 ) 2 ( Ω = 6 . 5 , 𝑒 2 = 0 . 7 ) ( 𝑡 0 = 0 . 0 8 3 4 7 1 5 3 , 𝑥 ( 1 ) 0 = 1 . 0 , ̇ 𝑥 ( 1 ) 0 = 5 . 5 4 8 7 8 7 1 0 , 𝑥 ( 2 ) 0 = 0 . 3 4 7 3 0 0 3 6 , ̇ 𝑥 ( 2 ) 0 = 0 . 9 8 8 0 1 5 0 3 ), (e) 𝑃 1 2 ( Ω = 2 2 . 7 , 𝑒 2 = 0 . 7 ) ( 𝑡 0 = 0 . 0 8 6 9 9 3 2 8 , 𝑥 ( 1 ) 0 = 1 . 0 , ̇ 𝑥 ( 1 ) 0 = 8 . 1 1 2 9 8 1 9 6 , 𝑥 ( 2 ) 0 = 0 . 0 4 0 5 9 7 2 7 , ̇ 𝑥 ( 2 ) 0 = 1 . 6 4 9 2 9 0 8 9 ), and (f) 𝑃 ( 1 2 ) 2 ( Ω = 2 0 . 4 , 𝑒 2 = 0 . 7 ) ( 𝑡 0 = 0 . 3 9 9 7 5 7 7 6 , 𝑥 ( 1 ) 0 = 1 . 0 , ̇ 𝑥 ( 1 ) 0 = 8 . 1 7 5 7 1 9 6 3 , 𝑥 ( 2 ) 0 = 0 . 0 7 1 0 2 0 9 8 , ̇ 𝑥 ( 2 ) 0 = 1 . 4 4 7 9 0 3 2 8 ).
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