While in a debate at UBI soft's IL-2 Forums, apparent problems concerning physics have come up, and it's got me stumped.
Read this thread first please!
The discussion is about the pitching capabilities of the Fw190A under high speeds. The case presented, is a 800km/h(492mph) near-90 degrees dive, plane probably not properly trimmed, so the pilot probably would have to push the stick to generate no pitch movement at all.
At about 500m(1500ft) the Fw190 pilot, (momentarily notwithstanding the effects of high Gs dumped onto the pilot, or the G forces that might destroy the plane) pulls full stick deflection possible. The plane recovers level flight with about 300m loss of altitude.
The primary question of interest is:
1) How high would be the G forces generated for a typical Fw190A to pull out in such a manner?
2) Would the elevator authority of a Fw190A allow such an input technically?(not withstanding effects given to a pilot, or G loads to the plane)
The point of view I stand in the afore mentioned discussion is this:
I am willing to accept the elevator authority of the Fw190As are overdone to a certain point, but I certainly don't think a pilot 490mph vertical dive would necessarily need a 'vector-thrust' technology to initiate a safe pull-out from 1500 feet. Pulling out within a 300m radius might be overdone, but I think it was possible with a close call.
I've been searching through almost every physics equation I could find about aerodynamics, but being a layman in physics in the first place, applying them to my needs are very tough!

The centripetal calcualtion of force as presented in the thread, does not seem to be right, or at least not to be applied as such in simple turms, but I could not find a method of calculating speed, G forces, sustained AoA needed per given time to be used as a correct method.
I'd appreciate some help from what you guys think about the discussion! I've been going through things like Lift Factor, ClMax, air density, cosine this, tangent that.. and my head is practically spinning wild
