Root Locus Sketching: Re-arrange & Sketch for Parameter "a

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Discussion Overview

The discussion revolves around the process of re-arranging an open-loop transfer function and sketching the root locus for a system as the parameter 'a' varies from 0 to infinity. The focus is on understanding the implications of this variation on the system's behavior, with participants exploring both theoretical and practical aspects of root locus analysis.

Discussion Character

  • Homework-related
  • Technical explanation
  • Exploratory
  • Debate/contested

Main Points Raised

  • One participant expresses uncertainty about how to re-arrange the transfer function into the familiar form of KF(s).
  • Another participant questions the necessary angle and magnitude conditions for poles of the closed-loop transfer function.
  • Clarifications are made regarding the angle condition for root locus, with some participants agreeing on the angle being -180 degrees and magnitude 1.
  • There is a discussion about the differences between traditional root locus problems and this specific case where the parameter under variation is the position of a zero, suggesting it may be more complex.
  • Participants discuss whether the problem should be solved numerically or graphically, with a leaning towards graphical methods based on angle and magnitude conditions.
  • A later reply provides a method for re-arranging the transfer function to find where G(s)H(s) = -1, suggesting a specific approach to achieve the traditional root locus form.
  • One participant expresses gratitude for the assistance received, indicating a resolution to their confusion regarding the re-arrangement process.

Areas of Agreement / Disagreement

Participants generally agree on the need to re-arrange the transfer function and the importance of angle and magnitude conditions for root locus. However, there is no consensus on the best approach to solve the problem, with differing opinions on whether numerical or graphical methods should be employed.

Contextual Notes

Participants note that the problem may be more challenging than traditional root locus questions due to the variation of a parameter that is not the loop gain. This introduces additional complexity in satisfying both angle and magnitude conditions.

wh88
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Homework Statement



Re-arrange the open-loop transfer function and sketch the root locus for the system for variation of the parameter 'a' from 0 to infinity.

Homework Equations



G(s)H(s) = 10(s+a) / [s(s+1)(s+8)]

The Attempt at a Solution



my problem is that i don't know how to re-arrange the transfer function into the familiar form of KF(s). any help would be appreciated. Thanks!
 
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Hi wh88. Can you tell me what must be the angle (and magnitude) of G(s)H(s) for the point "s" to be a pole of the closed loop TF?
 
sorry i made a mistake in the opening post. it should be 'variation of the parameter a'. i missed out the 'a'.

to uart, i believe its -180 degs and magnitude 1
 
wh88 said:
sorry i made a mistake in the opening post. it should be 'variation of the parameter a'. i missed out the 'a'.
That's ok, I guessed that :smile:

i believe its -180 degs and magnitude 1
Yep that's correct (180 degrees + any multiple of 360). The key to the root locus method is to find points in the complex plane where the sum of the angles on the numerator differs by 180 degrees (+360n) from the sum of angles on the denominator.

Start by plotting all the poles and zeros (of GH) on the complex plane and recognize that the angle that each pole (or zero) contributes to GH is equal to the angle of the vector drawn from the pole (or zero) to the test point "s". It's definitely a process that requires some practice before you become proficient.
 
uart said:
That's ok, I guessed that :smile:


Yep that's correct (180 degrees + any multiple of 360). The key to the root locus method is to find points in the complex plane where the sum of the angles on the numerator differs by 180 degrees (+360n) from the sum of angles on the denominator.

Start by plotting all the poles and zeros (of GH) on the complex plane and recognize that the angle that each pole (or zero) contributes to GH is equal to the angle of the vector drawn from the pole (or zero) to the test point "s". It's definitely a process that requires some practice before you become proficient.

Thanks for your help, uart. My understanding is that before plotting the poles and zeros on the complex plane, we have to get the open loop TF arranged in the form KF(s) if we want to find out how variation of K from 0 to infinity affects the system.
So in this case, won't we have to re-arrange the TF to the form aF(s)?
 
Hi wh88,

while uart has very kindly answered your question if you are doing a course in linear control you MUST (along with anyone else interested in this topic) look at the series of lectures by prof Madan Gopal on utube. I think root locus starts around lec 33.

Likely you will find these vids of more use than any text or lecture you might otherwise sit in on. Definitely worth you time. extremely well presented!
 
wh88 said:
Thanks for your help, uart. My understanding is that before plotting the poles and zeros on the complex plane, we have to get the open loop TF arranged in the form KF(s) if we want to find out how variation of K from 0 to infinity affects the system.
So in this case, won't we have to re-arrange the TF to the form aF(s)?

Ok you're right, this case is quite different to a traditional root locus question where the parameter under variation is the loop gain. It's been a long while since I've had to do root locus so I'm pretty rusty, but I think that in the traditional case that every point in the complex plane that satisfies the angle condition automatically satisfies magnitude condition for some value of of loop gain. In this case however, where the parameter under variation is the position of a zero, then it's definitely not true that magnitude condition is automatically satisfied, so this seems like a much harder problem (compared to the standard type root locus problem).
 
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wh88, is there any further context to this problem. Do you know if you're meant to try and solve it numerically or are you pretty sure that you're meant to be solving it graphically using the angle and magnitude conditions of root locus?
 
uart said:
wh88, is there any further context to this problem. Do you know if you're meant to try and solve it numerically or are you pretty sure that you're meant to be solving it graphically using the angle and magnitude conditions of root locus?

uart, the question asks us to re-arrange the open loop transfer function and sketch the root locus for the system as a varies from 0 to infinty. I doubt numerical methods are required. Its the re-arrangement that's troubling me.
 
  • #10
wh88 said:
uart, the question asks us to re-arrange the open loop transfer function and sketch the root locus for the system as a varies from 0 to infinty. I doubt numerical methods are required. Its the re-arrangement that's troubling me.

Ok I can see what they want you to do now.

You have to find where G(s) H(s) = -1. So split it across the numerator as :

\frac{10s +10a}{s (s+1) (s+8) } = \frac{10s}{s (s+1) (s+8) } + \frac{10a}{s (s+1) (s+8) }

Using the above you can rearrange GH=-1 to :

\frac{10a}{s (s+1) (s+8) } =- \left(1 + \frac{10s}{s (s+1) (s+8) } \right)

Now put the RHS to a common denominator and factorize the resulting numerator (it factorizes pretty easily). Finally mult/divide both sides in the obvious way so as to re-establish "-1" on the RHS.

You end up with an equation in the traditional root locus form, where the variable is proportional to the loop gain.
 
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  • #11
uart said:
Ok I can see what they want you to do now.

You have to find where G(s) H(s) = -1. So split it across the numerator as :

\frac{10s +10a}{s (s+1) (s+8) } = \frac{10s}{s (s+1) (s+8) } + \frac{10a}{s (s+1) (s+8) }

Using the above you can rearrange GH=-1 to :

\frac{10a}{s (s+1) (s+8) } =- \left(1 + \frac{10s}{s (s+1) (s+8) } \right)

Now put the RHS to a common denominator and factorize the resulting numerator (it factorizes pretty easily). Finally mult/divide both sides in the obvious way so as to re-establish "-1" on the RHS.

You end up with an equation in the traditional root locus form, where the variable is proportional to the loop gain.

i finally got it. Thank you very much uart!
 

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