Hi all!

I've created a new model for the spinning gyro (Instrumentation/gyro.*xx). 

/**
 * Complex model of a spinning gyro.
 *
 * The gyro is driven by a torque. It is slowed down by bearing
 * friction and air friction.
 * The gyro disk is defined by radius [m], width [m], and 
 * material density [kg/m�]. The disk is a solid cylinder.
 */

In the model I consider bearing friction torque to be constant. Air friction 
is only modeled  for the outer rim of the cylinder, _not_ for the two flat 
sides. Modeling air friction for the sides is more complex as the velocity 
increases with the radius-- a point close to the rim has a higher velocity 
than a point close to the center. I suspect that the friction contribution 
from the two sides would be higher than from the outer rim surface, so I 
definetely should model this too. Any suggestions on how to model air 
friction on a spinning flat surface?

The output for this model is angular velocity, angular momentum and a 
normalized spin. Angular momentum can be used to model gyroscopic precession. 
I only added normalized spin in order to be able to interface with the 
existing heading indicator and attitude indicator models.

Now, I know that the existing gyro model and heading indicator and attitude 
indicator work great and that some might think that I am trying to fix 
something that is already working. I would argue that I am trying to improve 
on something that is already working ;-). But if nobody else share my point 
of view, I might abandon the idea.

Comments are welcome!

-- 
Roy Vegard Ovesen


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