Physical realization of a system

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Discussion Overview

The discussion centers around the concept of realizability in control systems, specifically regarding the conditions under which a transfer function can be considered physically realizable. Participants explore the implications of transfer functions, such as G(s) = Cs, and question the definitions and criteria for realizability in both theoretical and practical contexts.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants express confusion about the definition of a realizable system, particularly in relation to the degrees of the numerator and denominator of a transfer function.
  • One participant suggests that a capacitor can realize the transfer function G(s) = Cs, questioning why it is deemed not realizable.
  • Another participant proposes that the ability to produce an infinite output from an infinite frequency input is a key factor in determining realizability, implying that physical systems cannot achieve this.
  • There is a discussion about the historical context of the terms "realizable" and "unrealizable," with some suggesting that these terms may not align with common usage.
  • Participants debate whether the conditions for realizability are self-evident or require further explanation, with some expressing the need for clarity on how to physically realize certain models.
  • One participant corrects a misunderstanding regarding the Laplace transform of a capacitor, stating that it is 1/(C*s), which aligns with the condition that the denominator's degree must be at least that of the numerator.
  • There is a discussion about the stability of systems and how it relates to the conditions for realizability, with some questioning the significance of the degrees of the numerator and denominator in this context.

Areas of Agreement / Disagreement

Participants express differing views on the definition of realizability and whether certain transfer functions can be physically realized. There is no consensus on the implications of the conditions for realizability, and the discussion remains unresolved regarding the interpretation of these concepts.

Contextual Notes

Participants note that the definition of realizability may depend on the frequency range considered, and there are unresolved questions about the applicability of certain transfer functions in practical scenarios.

Tusike
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Hi!

I have a simple question regarding the realization of systems. In my university course books, it's mentioned multiple times that a system with a transfer function G(s) is realizable, if the denominator's degree is at least that of the numerator's degree. I found the same statement on the internet as well: http://en.wikibooks.org/wiki/Control_Systems/Realizations

I don't understand what exactly this means, and it's always without explanation.

For example, suppose I have a transfer function G(s) = Y(s)/U(s) = Cs, which so shouldn't be realizable physically.
Doesn't a simple capacitor "realize" this transfer functions? If I consider the voltage of the capacitor my input, and the current through it the output? Then i = C*du/dt.
What do we mean by a system being realizable?

Thanks for any help!

-Tusike
 
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I'm sorry, I don't understand how that helps... That's the same link I posted, and it doesn't provide an explanation as to why the statements it makes are true. What am I missing? Why wouldn't my capacitor example be considered a realization?
 
Tusike said:
Why wouldn't my capacitor example be considered a realization?

I'm not an expert on control systems, but I'll make a guess based on the "Implications" section of
http://en.wikipedia.org/wiki/Proper_transfer_function
[Edit: I edited the post to give the correct link.]

If a transfer function reduces to a form like k_0 + k_1 s + k_2 s^2 the terms in powers of s have the effect of differentiating the input function. So if you set the the input to be a high frequency wave or rapidly wigglling curve you would get a high amplitude output. Apparently the ability to get an arbitrarily high amplitude output by picking a suitable high frequency input is considered not physically realizable.
 
Last edited:
It is not clear where you are having difficulty.

There are three "realization conditions" listed ... go through the one at a time and consider the converse.
Explain, in your own words, how the converse situation could be realized (or cannot be).

For your specific example - describe, in your own words, how you would physically realize the model.
 
OK, so I understand how the idea is that you shouldn't get an infinite response from an infinite frequency input, because a physical system wouldn't have enough energy to produce that.

1) However, why is an infinite frequency input considered physically realizable? Is it possible to generate such a thing? If not, then it shouldn't be used as a definition for why something isn't physically realizable...

2) Just because my capacitor wouldn't work at infinite frequency, it would still work in an operating range of e.g. 1kHz-1MHz. So, for such an application, I would describe it as I(s)/U(s)=G(s)=Cs, and I would use that transfer function for all my calculations, and it would work in practice just as I have calculated. Still, it's not considered physically realizable because it wouldn't work outside my planned operating range? Isn't this the same as saying a resistor isn't physically realizable, because it will break down at a very high U and won't follow it's supposed characteristic?

-Tusike
 
Tusike said:
1) However, why is an infinite frequency input considered physically realizable? Is it possible to generate such a thing? If not, then it shouldn't be used as a definition for why something isn't physically realizable...

Giving the Wikipedia article it's due, it defined a "proper" transfer functions. Even if we call them "realizable" transfer functions, there is no law of culture that says the use of words as technical terms must match their use in common speech. Why the terms "realizable" and "unrealizable" came into use mght have a historical explanation - perhaps it makes sense for people trying to design particular types of devices.

As I said, I'm not an expert in control theory. ( I once read a SAMS book about it.) Refresh my mind on how one evaluates if a given control system is "stable". Does that have anything to do with proper transfer functions?
 
"realizable" is commonly said to mean that the model can be turned into a physical device - but that is not a definition in the strict mathematical sense. The definition is the list of conditions.
The question then goes to how that list got to be chosen.
The reason nobody derives the conditions is because they are usually considered self-evident when thought about.
So it is not possible to help you without you telling us more about how you are thinking re post #5.
 
  • #10
Tusike said:
For example, suppose I have a transfer function G(s) = Y(s)/U(s) = Cs, which so shouldn't be realizable physically.
Doesn't a simple capacitor "realize" this transfer functions?
I think that your problem is that you have the wrong Laplace transform for a capacitor. It is 1/(C*s). So the original statement that the order of the denominator must be at least the order of the numerator would say this is realizable..
 
  • #11
@stephen: I guess that's the same conclusion I'm arriving at, that the naming is for historical reasons, or is very strict to avoid any confusion. Perhaps a better way of saying would be that the system is realizable "in a given frequency domain", and the formal definition requires it to be realizable at all domains. The requirement for a certain stability, say the output approaches zero after a dirac impulse, is that lim(sG(s)) be zero as 's' approaches zero. Whether or not the numerator has a higher polynomial in s than the denominator doesn't really effect this.

@simon: I'm not really sure how my first post isn't enough of an explanation for how to physically realize the example system. I can create a G(s)=Cs transfer function by connecting a capacitor to a signal generator. I consider the e.g. sinusoidal signal my input, and the current through the capacitor my output. Then I(s)=G(s)*U(s).

@FactChecker: the transfer function depends on what I consider my input and output, so Cs is okay.
 
  • #12
Tusike said:
@stephen: The requirement for a certain stability, say the output approaches zero after a dirac impulse, is that lim(sG(s)) be zero as 's' approaches zero. Whether or not the numerator has a higher polynomial in s than the denominator doesn't really effect this.

Just from a mathematical point of view, doesn't the degree of the numerator and denominator of G(s) have an important bearing on lim_{s \rightarrow 0} s G(s) ?
 
  • #13
Tusike said:
the transfer function depends on what I consider my input and output, so Cs is okay.
Sorry. I guess between capacitors and inductors, there is a problem either way. In the math definition, I don't see why there would not be a state-space representation of either one.
PS. For a second, I thought that the quick explanation is that it was not an "if and only if" condition. But the link you gave states it as if and only if
 

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