Damped oscillator |
We consider a damped oscillator (a pendulum in the linear approximation), ruled by the differential equation
We naively discretized this equation (using a sampling time of one second) with
Choosing omega=1/8 and various values for k, and choosing initial condition thetap=8 and thetav=0, we have the following system oscillator_i0.lts.
l | #e | k=3/4 | k=1/4 | k=1/8 | k=1/16 | k=1/64 | k=0 | running time | file | ||||||
thetap | thetav | thetap | thetav | thetap | thetav | thetap | thetav | thetap | thetav | thetap | thetav | ||||
1 | 4 | [0,8.0] | [-0.125,0] | [0,8.264] | [-0.248,0] | [0,10.217] | [-0.402,0] | [-1.818,8.262] | [-0.625,0.128] | [-6.580,8] | [-0.956,0.785] | [-infty,infty] | [-infty,infty] | oscillator_i0_l1.ps | |
2 | 8 | [0,8.0] | [-0.125,0] | [0,8.184] | [-0.233,0] | [0,9.286] | [-0.394,0] | [-1.680,8.090] | [-0.600,0.123] | [-6.580,8] | [-0.924,0.760] | [-infty,infty] | [-infty,infty] | oscillator_i0_l2.ps | |
4 | 32 | [0,8.0] | [-0.125,0] | [0,8.0] | [-0.231,0] | [0,8.08] | [-0.393,0] | [-1.648,8.0] | [-0.592,0.122] | [-6.580,8] | [-0.915,0.751] | [-infty,infty] | [-infty,infty] | oscillator_i0_l4.ps | |
l | : | corresponds to "-log l" option |
#e | : | number of template expressions on the coefficients of Jordan normal form |
(related to the number "l" and the number of different coefficient of the Jordan normal form) | ||
k | : | damping factor |
thetap | : | minimum and maximum angular position in discrete trajectories |
thetav | : | minimum and maximum angular speed in discrete trajectories |
l | #e | k=3/4 | k=1/4 | k=1/8 | k=1/16 | k=1/64 | k=0 | running time | file | ||||||
thetap | thetav | thetap | thetav | thetap | thetav | thetap | thetav | thetap | thetav | thetap | thetav | ||||
4 | 32 | [0,16.0] | [-4.125,8] | [0,16.099] | [-0.25,8] | [0,31.416] | [-1.560,8] | [-8.742,42.555] | [-3.144,8] | [-49.598,60.421] | [-6.901,8] | [-infty,infty] | [-infty,infty] | oscillator_i1_l4.ps | |
Some comments:
Damped oscillator |