kaapipo
Joined 5 years ago
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Apr 10
Joined 5 years ago
Any design that doesn't actually force you to handle the error case cannot be called good in my opinion.
`T = 2π√(L/g)`
substitute T = 2 s and L = 1 m:
`2 s = 2π√(1 m / g)`
solve for g:
`g = π² m/s²`.
This holds up in any strength of gravity, but the length of a meter would be different depending on it.
[1]. This actually was proposed by Talleyrand in 1790. Imagine the world if this were true!
I hope him all the best.