Antonio S. Torralba
Universidad Complutense  

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FUNDER - Theoretical Background


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SYSTEMS - FUNCTIONAL REPRESENTATION


FUNCTIONALS


Functionals map functions to numbers (or to other functions). They can be understood as a generalization of multivariate functions. Consider the vectors


Discrete input

(1)


and

Discrete output

(2)


where the elements of Output vector are


Multivariate function of the input

(3)


Vectors Input vector and Output vector can be viewed as a discretization in Tau time points of the input, Continuous input, and output, Continuous output, of a system, respectively.


Increasing the number of discrete-time points, for a fixed time interval Interval from a to b, vectors tend to functions. In the continuous limit, the function Function of the input becomes a functional. Introducing the notation


Functional

(4)


where


Definition of continuous time

(5)


the response, Continuous output, of a system with one input, Continuous input, can be represented as a functional relationship, Symbol of a functional. The generalization to systems with more than one input is obvious.


Note that in this approach the emphasis is on the relationship between the input and the output, and not between the mechanism of the system and the output. Extremely complex systems can be represented by eq. (4).



LINEAR SYSTEMS


A simple way to illustrate the meaning of functionals is to derive a general one for linear systems. First, we recall that any signal can be constructed as a superposition of deltas. Say that we know the response to a unit impulse at time Perturbation time,


Response to impulses

(6)


or, in functional notation,


Response to impulses as a functional

(7)


Using eq. (9) of the Dirac's delta page, the response to any excitation is


Response to any excitation

(8)


From the additivity of linear systems, the response becomes


Additivity of responses

(9)


Furthermore, applying the homogeneity property, we have that


Homogeneity of responses

(10)


Finally, substituting the impulse response, eq. (7), a general functional of the input results:


General response of a linear system

(11)


This expression further simplifies if the system is time-invariant, which requires that


Time-invariance condition

(12)


For this important class of systems, eq. (11) becomes a convolution product:


Response of time-invariant linear systems

(13)


The above derivations show that one need not know the mechanism of a linear system for being able to predict its response to any excitation. Furthermore, if the system is time-invariant, the only information required for completely characterising its response is an impulse-perturbation experiment at any time.


The following pages give an approach of this kind for nonlinear systems.



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