Pulling a yoyo over a surface with tension

In summary: Was a rhetorical question). So you find a certain angular acceleration. What is the connection with the no-slipping condition?I dont know the connection between angular acceleration and non slipping. I know that when non slipping the relationsship between the speed of the cm and the angular speed: v(cm) = R *omegaAnd ##a## as a function of ##\alpha## ?And ##a## as a function of ##\alpha## ?Ah yes sorry ##a## = ##\alpha## * ##R##Okay now it gets confusing again. So i have an acceleration ##a## due to a force ##F##. This force leads to a rotation with an acceleraton depending on R.
  • #36
I have (from your posts):$$\begin{align*} R\mu(mg-F\sin\theta)-bF &=I\alpha \\ \ &\ \\
I\alpha&={1\over 2} m R^2 \alpha = {R\over 2} ma = {R\over 2} \Bigl ( F\cos\theta - \mu\left ( mg -F\sin\theta\right)\Bigr ) \\ \ &\ \\
2\mu(mg-F\sin\theta)-2b{F/R} &=F\cos\theta - \mu\left ( mg -F\sin\theta\right )\\ \ &\ \\
3\mu mg &= F\Bigl( \cos\theta + 3\mu\sin\theta +2b/R \Bigr ) \\ \ &\ \\
F &= {3\mu mg \over \cos\theta + 3\mu\sin\theta +2b/R }
\end{align*} $$which fits for ##\mu=0## and ##\theta = 0## -- and cw.

Must have been an overlooked minus sign.Not finished for ccw though...

##\ ##
 
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  • #37
BvU said:
I have (from your posts):$$\begin{align*} R\mu(mg-F\sin\theta)-bF &=I\alpha \\ \ &\ \\
I\alpha&={1\over 2} m R^2 \alpha = {R\over 2} ma = {R\over 2} \Bigl ( F\cos\theta - \mu\left ( mg -F\sin\theta\right)\Bigr ) \\ \ &\ \\
2\mu(mg-F\sin\theta)-2b{F/R} &=F\cos\theta - \mu\left ( mg -F\sin\theta\right )\\ \ &\ \\
3\mu mg &= F\Bigl( \cos\theta + 3\mu\sin\theta +2b/R \Bigr ) \\ \ &\ \\
F &= {3\mu mg \over \cos\theta + 3\mu\sin\theta +2b/R }
\end{align*} $$which fits for ##\mu=0## and ##\theta = 0## -- and cw.

Must have been an overlooked minus sign.Not finished for ccw though...

##\ ##
Yes that is correct. Okay i will do it for ccw and then forget about it :D
 

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