arXiv:1511.04593 · uncategorized
Parametric resonance induced chaos in magnetic damped driven pendulum
Giorgi Khomeriki
Abstract
A damped driven pendulum with a magnetic driving force, appearing from a solenoid, where ac current flows is considered. The solenoid acts on the magnet, which is located at the free end of the pendulum. In this system, the existence and interrelation of chaos and parametric resonance is theoretically examined. Derived analytical results are supported by numerical simulations and conducted experiments.
Simulation skipped or failed
no parseable d.../dt equation found
Extracted equations
- m*ℓ*α'' = F_x*cos(α) + F_y*sin(α) - m*g*sin(α) - q*α'
- α'' = -α*(ω₀² + h*cos(2ωt)) - q*α'
- where F_x = -∂U/∂x, F_y = -∂U/∂y, and U is the dipole-dipole interaction energy
Paper claims vs. our run
- Parametric resonance condition: h ≥ 2|ω² - ω₀² + 2qω|not-testableno fidelity score recorded
- Parametric instability growth rate: s = (ω₀² + h/2 - ω² - qω)/(2ω)not-testableno fidelity score recorded
- Chaos occurs when parametric resonance conditions are satisfiednot-testableno fidelity score recorded
- Lyapunov exponent for small angles matches theoretical growth rate snot-testableno fidelity score recorded
- System exhibits large-amplitude oscillations from small initial perturbations when parametrically unstablenot-testableno fidelity score recorded
Parameters
| m | 0.05 |
| ℓ | 0.5 |
| g | 9.81 |
| q | 0.01 |
| ω | 29π |
| 2ω | 58π |
| r0 | 0.014 |
| L2 | symbolic |
| L0_1 | symbolic |
| ω₀ | sqrt(g/ℓ) |
| h | L0_1*(12*L2/(m*r0^5) + 2*L2/(m*ℓ^2*r0^3)) |
Run notes
equations tried: ["m*ℓ*α'' = F_x*cos(α) + F_y*sin(α) - m*g*sin(α) - q*α'", "α'' = -α*(ω₀² + h*cos(2ωt)) - q*α'", 'where F_x = -∂U/∂x, F_y = -∂U/∂y, and U is the dipole-dipole interaction energy']