|
-
Sep 20th, 2002, 10:44 AM
#1
Thread Starter
Addicted Member
-
Oct 1st, 2002, 09:22 AM
#2
What you have to do is switch to the coordinate system that rotates along with the wheel and express the marker trajectory in that system.
The trajectory equations in the stationary coordinate system are simply:
x(t) = rMax - v0*t (v0 being the constant velocity toward the origin)
y(t) = 0
Let omega be the angular velocity of the wheel (and therefore of the rotating coordinate system) and assume it is rotating CCW.
If you call x' and y' the axes of the rotating coordinate system, then the transformation equations are the well known:
x' = x*cos(omega*t) + y*sin(omega*t)
y' = -x*sin(omega*t) + y*cos(omega*t)
Susbtituting the above x(t) & y(t) in the latter pair of equations, we end up with:
x'(t) = (rMax - v0*t)*cos(omega*t)
y'(t) = -(rMax - v0*t)*sin(omega*t)
so these are the equtions describing the marker trajectory as seen from the wheel or, conversely, the
resulting curve drawn on the wheel.
-
Oct 14th, 2002, 05:09 PM
#3
Thread Starter
Addicted Member
Thanks
Thanks krtxmrtz.
That definitely looks like the way I should have approached it. I ended up generating a table of points for discrete rotational steps. I haven't verified if we actually have the same equations, but I wanted to thank you.
-
Oct 16th, 2002, 09:48 AM
#4
Re: Thanks
Originally posted by Phenix
I haven't verified if we actually have the same equations, but I wanted to thank you.
You're very welcome!
Posting Permissions
- You may not post new threads
- You may not post replies
- You may not post attachments
- You may not edit your posts
-
Forum Rules
|
Click Here to Expand Forum to Full Width
|