Dzhanibekov effect: Parametrizable numerical simulation
This post is a follow-up to part one.
The Dzhanibekov Effect aka. Tennis Racket Theorem here in space:
Here in slow motion on earth:
And here in parametrizable numerical simulation:
Angular momentum
Body
Inputs
L =| +10.000 |
| +0.001 |
| +0.000 |
| +0.00 | +0.00 | +0.00 |
| +0.00 | +0.00 | +0.00 |
| +0.00 | +0.00 | +0.00 |
| +0.00 | +0.00 | +0.00 |
| +0.00 | +0.00 | +0.00 |
| +0.00 | +0.00 | +0.00 |
Outputs
ω =| +0.000 |
| +0.000 |
| +0.000 |
E = 0.000 J
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