Viscous drag parallel to the axis of rotation: Control Systems

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kostoglotov
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Homework Statement



WPAKuf4.png


https://i.imgur.com/WPAKuf4.png

seeking [itex]G(s) = \frac{\theta_2(s)}{\tau(s)}[/itex]

Homework Equations

The Attempt at a Solution



What does it mean when the viscous drag is parallel to the axis of rotation?[/B]

It also turns out that this system needs two equations. I can sort of see why, even though it doesn't have two masses, I'm not 100% sure though, how to break this system up into two equations, where and how to make the break.

Any help at all would be very appreciated, thank you :)
 
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That is a truly awful diagram .

Nevertheless it is possible to work out what the various bits do if we assume that this is a purely rotary system .

Those damper terms and the energy accumulator term all act in a rotary sense and not in the linear sense depicted . You can infer this anyway from their dimensions - they are all quoted as being per radian .
 
kostoglotov said:

Homework Statement



View attachment 210469

https://i.imgur.com/WPAKuf4.png

seeking [itex]G(s) = \frac{\theta_2(s)}{\tau(s)}[/itex]

Homework Equations

The Attempt at a Solution



What does it mean when the viscous drag is parallel to the axis of rotation?[/B]
poor statement but just assume there is rotational drag torque in those three places.

It also turns out that this system needs two equations. I can sort of see why, even though it doesn't have two masses, I'm not 100% sure though, how to break this system up into two equations, where and how to make the break.
I would label the right-hand side of the rotor θ1, then you can have θ1/τ as the 1st equation and θ2/θ1 as the 2nd equation, then multiply the two transfer functions to get θ2/τ.
 
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