From: The periodic rotary motions of a rigid body in a new domain of angular velocity
t | p2a | γ2a | xa = dp2a/dt | ya = dγ2a/dt |
---|---|---|---|---|
0 | 1.88117E−15 | 1 | 0 | 0 |
10 | 1.52189E−15 | 0.809017 | − 1.10572E−15 | − 0.587785 |
20 | 5.81312E−16 | 0.309017 | − 1.78909E−15 | − 0.951057 |
30 | − 5.81312E−16 | − 0.309017 | − 1.78909E−15 | − 0.951056 |
40 | − 1.5219E−15 | − 0.809017 | − 1.10572E−15 | − 0.587785 |
50 | − 1.88117E−15 | − 1 | − 2.84048E−22 | − 1.50996E−07 |
60 | − 1.52189E−15 | − 0.809017 | 1.10572E−15 | 0.587785 |
70 | − 5.81312E−16 | − 0.309017 | 1.78909E−15 | 0.951056 |
80 | 5.81312E−16 | 0.309017 | 1.78909E−15 | 0.951056 |
90 | 1.5219E−15 | 0.809017 | 1.10572E−15 | 0.587785 |
100 | 1.88117E−15 | 1 | 5.68096E−22 | 3.01992E−07 |
110 | 1.52189E−15 | 0.809017 | − 1.10572E−15 | − 0.587785 |
120 | 5.81312E−16 | 0.309017 | − 1.78909E−15 | − 0.951057 |
130 | − 5.81313E−16 | − 0.309017 | − 1.78909E−15 | − 0.951056 |
140 | − 1.52189E−15 | − 0.809017 | − 1.10572E−15 | − 0.587785 |
150 | − 1.88117E−15 | − 1 | 4.48654E−23 | 2.38498E−08 |
160 | − 1.52189E−15 | − 0.809017 | 1.10572E−15 | 0.587785 |
170 | − 5.81311E−16 | − 0.309016 | 1.78909E−15 | 0.951057 |
180 | 5.81314E−16 | 0.309018 | 1.78909E−15 | 0.951056 |
190 | 1.5219E−15 | 0.809017 | 1.10572E−15 | 0.587785 |
200 | 1.88117E−15 | 1 | 1.13619E−21 | 6.03983E−07 |
210 | 1.5219E−15 | 0.809017 | − 1.10572E−15 | − 0.587785 |
220 | 5.81312E−16 | 0.309017 | − 1.78909E−15 | − 0.951056 |
230 | − 5.81312E−16 | − 0.309017 | − 1.78909E−15 | − 0.951056 |
240 | − 1.5219E−15 | − 0.809017 | − 1.10572E−15 | − 0.587785 |
250 | − 1.88117E−15 | − 1 | 1.27079E−21 | 6.75532E−07 |
260 | − 1.52189E−15 | − 0.809016 | 1.10572E−15 | 0.587786 |
270 | − 5.81313E−16 | − 0.309018 | 1.78909E−15 | 0.951056 |
280 | 5.81311E−16 | 0.309017 | 1.78909E−15 | 0.951057 |
290 | 1.52189E−15 | 0.809017 | 1.10572E−15 | 0.587785 |
300 | 1.88117E−15 | 1 | − 8.97307E−23 | − 4.76995E−08 |