Talk:Coriolis field

Whole article unclear
This article does not clearly state the point at all. It mentions not a single word about a nonrotating frame of reference behaving like a rotating one in the presence of a Gravitomagnetic field with a coriolis force existing as a real force. Blackbombchu (talk) 01:41, 13 October 2013 (UTC)

What is the kinematics under a constant Coriolis field?
I mean, what is the solution to the vector first-order ODE (or in which book or site can I find it?):

$$ \vec \omega \times \frac {d}{dt} \vec r = \vec g $$

ω, g are constant coefficient, not dependent on the variable t. I call it Coriolis equation, sinice the first member is half of a Coriolis field. I know that if k is the unit vector of ω, j the u.v. of g, i is defined jxk:

$$ \frac {d}{dt} \vec r (t) = \frac {|\vec g|}{|\vec \omega|} \hat i(t) + v_b(t) \hat k(t) $$

But then how to integrate it?

$$ \vec r (t) = ? $$

Can I pivot on the Poisson relations even if the problem is not apparently the standard rotation one? Can I assume as a choice on frame of reference:

$$ \frac {d}{dt} \vec r (t) =? \, \vec \omega \times \vec r$$

Thank you in advance, --95.238.61.51 (talk) 08:23, 23 October 2014 (UTC)