looking to the doppler effect: frequency equals (the speed of sound in what ever temperature air you are in: $c$)+(Velocity of you relative to the measured object: so if you are stationary this value is zero: $V(r)$)/(speed of sound in what ever temperature air you are in: $c$)+(Velocity of object relative to you $V(s)$: essentially the speed of the object you are measuring)=frequency: $f$
$f=(c+V(r))/(c+V(s))$; this rewrites to: $V(s)=(V(r)+c(1-f))/f$; if $V(r)=0$, then $V(s)=(c/f)-1$; resolving for f: $f=c/(V(s)+1)$
your $V(s)$ should equal: $(2πL_{rope})/(t_{2π})=V(s): (2πr)/t=V(s)$
Next comes the experimental set up. Your observer should be placed so that it forms a square with side lengths equaling the radius of your rope. This is so that when the object is coming directly towards the observer, and after π/2 interval of it's rotation is going directly away from you. With these two points of data we can extrapolate: $f=c/(c-V(s))$ when it is coming at you, and $f=c/(c-V(s))$ when going away from you. If this does not give the same V(s) after input of the observed frequency, then your object probably can't be solved for.
if you observe all the frequency over all time it should be semetric. Spendinding equal times in red/blue shift. Solve for the time when your object is at both points so you can know where to look in your data.
c in this: $c=331.4+.6(T°C)$