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)