lecture 2 linear differential systems€¦ · lecture 2 linear differential systems harry...
TRANSCRIPT
![Page 1: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/1.jpg)
Lecture2
LINEAR DIFFERENTIAL
SYSTEMS
Harry TrentelmanUniver sity of Groning en, The Netherlands
Minicour se ECC 2003 Cambridg e, UK, September 2, 2003
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.1/22
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Part 1: Generalities
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.2/22
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Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,meaning
;
2. time-invariant, meaning
,
where denotes the shift,
3. differential, meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 4: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/4.jpg)
Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,
meaning;
2. time-invariant, meaning
,
where denotes the shift,
3. differential, meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 5: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/5.jpg)
Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,meaning
;
2. time-invariant, meaning
,
where denotes the shift,
3. differential, meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 6: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/6.jpg)
Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,meaning
;
2. time-invariant,
meaning
,
where denotes the shift,
3. differential, meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 7: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/7.jpg)
Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,meaning
;
2. time-invariant, meaning
,
where denotes the shift,
3. differential, meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 8: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/8.jpg)
Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,meaning
;
2. time-invariant, meaning
,
where denotes the shift,
3. differential,
meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 9: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/9.jpg)
Linear differ ential systems
We discuss the theor y of dynamical systems
�
that are
1. linear,meaning
;
2. time-invariant, meaning
,
where denotes the shift,
3. differential, meaning
consists of the solutions of a system of diff erentialequations.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.3/22
![Page 10: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/10.jpg)
Linear constantcoefficientdiffer ential equations
Variab les: �, up to � times diff erentiated, �equations.
��� � � ��� � � ���
��
�� �
��� � � ��� � � ���
��
�� �
......
...
��� � � � ��� � � � ���
�� �
�� �
Coefficients
� : 3 indices!
for the -th diff erential equation,for the variab le involved,
for the order of diff erentiation.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.4/22
![Page 11: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/11.jpg)
Linear constantcoefficientdiffer ential equations
Variab les: �, up to � times diff erentiated, �equations.
��� � � ��� � � ���
��
�� �
��� � � ��� � � ���
��
�� �
......
...
��� � � � ��� � � � ���
�� �
�� �
Coefficients
� : 3 indices!
� � for the�
-th diff erential equation,
for the variab le involved,
for the order of diff erentiation.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.4/22
![Page 12: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/12.jpg)
Linear constantcoefficientdiffer ential equations
Variab les: �, up to � times diff erentiated, �equations.
��� � � ��� � � ���
��
�� �
��� � � ��� � � ���
��
�� �
......
...
��� � � � ��� � � � ���
�� �
�� �
Coefficients
� : 3 indices!
� � for the�
-th diff erential equation,
� for the variab le involved,
for the order of diff erentiation.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.4/22
![Page 13: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/13.jpg)
Linear constantcoefficientdiffer ential equations
Variab les: �, up to � times diff erentiated, �equations.
��� � � ��� � � ���
��
�� �
��� � � ��� � � ���
��
�� �
......
...
��� � � � ��� � � � ���
�� �
�� �
Coefficients
� : 3 indices!
� � for the�
-th diff erential equation,
� for the variab le involved,
� � for the order
�� of diff erentiation.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.4/22
![Page 14: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/14.jpg)
In vector/matrix notation:
...
�
�
� � ��
� � ��
......
...
��
��
�� �
Yields
with
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.5/22
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In vector/matrix notation:
...
�
�
� � ��
� � ��
......
...
��
��
�� �
Yields
���
with �
� �
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.5/22
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Combined with the pol ynomial matrix (in the indeterminate )
��
we obtain for this the shor t notation
Including latent variab les
with .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.6/22
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Combined with the pol ynomial matrix (in the indeterminate )
��
we obtain for this the shor t notation
Including latent variab les
with .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.6/22
![Page 18: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/18.jpg)
Polynomial matrices
A pol ynomial matrix is a pol ynomial with matrix coefficients:
��
with �
�� ��
.
We may view also as a matrix of pol ynomials:
......
...
with the ’s pol ynomials with real coefficients.
Notation : , , , .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.7/22
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Polynomial matrices
A pol ynomial matrix is a pol ynomial with matrix coefficients:
��
with �
�� ��
.We may view also as a matrix of pol ynomials:
����
......
...
�� �� �� ��
with the ’s pol ynomials with real coefficients.
Notation : , , , .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.7/22
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Polynomial matrices
A pol ynomial matrix is a pol ynomial with matrix coefficients:
��
with �
�� ��
.We may view also as a matrix of pol ynomials:
����
......
...
�� �� �� ��
with the ’s pol ynomials with real coefficients.
Notation :
�� ��,
�
,
�
, .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.7/22
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What do we mean by the behavior of this system of diff erential equations?
When shall we define to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 22: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/22.jpg)
What do we mean by the behavior of this system of diff erential equations?
When shall we define
�
to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 23: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/23.jpg)
What do we mean by the behavior of this system of diff erential equations?
When shall we define
�
to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 24: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/24.jpg)
What do we mean by the behavior of this system of diff erential equations?
When shall we define
�
to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 25: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/25.jpg)
What do we mean by the behavior of this system of diff erential equations?
When shall we define
�
to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 26: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/26.jpg)
What do we mean by the behavior of this system of diff erential equations?
When shall we define
�
to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
�
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 27: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/27.jpg)
What do we mean by the behavior of this system of diff erential equations?
When shall we define
�
to be a solution of?
Possibilities:
Strong solutions?
Weak solutions?
�
(infinitel y diff erentiab le) solutions?
Distrib utional solutions?
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.8/22
![Page 28: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/28.jpg)
We will be ‘pra gmatic’, and take the easy way out:
solutions!
-solution: is a -solution of if
1. is infinitel y diff erentiab le ( := ), and
2. .
Transmits main ideas, easier to handle , easy theor y, sometimes(too) restrictive .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.9/22
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We will be ‘pra gmatic’, and take the easy way out:
solutions!
-solution:
�
is a -solution of if
1. is infinitel y diff erentiab le ( :=
�
), and
2. .
Transmits main ideas, easier to handle , easy theor y, sometimes(too) restrictive .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.9/22
![Page 30: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/30.jpg)
We will be ‘pra gmatic’, and take the easy way out:
solutions!
-solution:
�
is a -solution of if
1. is infinitel y diff erentiab le ( :=
�
), and
2. .
Transmits main ideas, easier to handle , easy theor y, sometimes(too) restrictive .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.9/22
![Page 31: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/31.jpg)
Whence , defines the system�
with
�
Proposition : This system is linear and time-in variant.
Note that is equal to the kernel of the operator . We will
theref ore call a kernel representation of this system,or the behavior .
determines uniquel y, the converse is not true!
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.10/22
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Whence , defines the system�
with
�
Proposition : This system is linear and time-in variant.
Note that is equal to the kernel of the operator . We will
theref ore call a kernel representation of this system,or the behavior .
determines uniquel y, the converse is not true!
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.10/22
![Page 33: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/33.jpg)
Whence , defines the system�
with
�
Proposition : This system is linear and time-in variant.
Note that is equal to the kernel of the operator . We will
theref ore call a kernel representation of this system,or the behavior .
determines uniquel y, the converse is not true!
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.10/22
![Page 34: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/34.jpg)
Whence , defines the system�
with
�
Proposition : This system is linear and time-in variant.
Note that is equal to the kernel of the operator . We will
theref ore call a kernel representation of this system,or the behavior .
determines uniquel y, the converse is not true!
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.10/22
![Page 35: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/35.jpg)
Notation and nomenclature
all suc h systems (with any - finite - number of variab les)
�
with variab les
�
(no ambiguity regar ding )
Elements of linear differential systems
‘has’ behavior
or : the system induced by
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.11/22
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Notation and nomenclature
all suc h systems (with any - finite - number of variab les)
�
with variab les
�
(no ambiguity regar ding )
Elements of linear differential systems
‘has’ behavior
or : the system induced by
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.11/22
![Page 37: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/37.jpg)
Part 2: Inputs and outputs
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.12/22
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Linear diff erential system:
�
.
induced by a pol ynomial matrix :
variab le .
Idea: there are degrees of freedom in the diff erential equation
. In other words: the requirement leavessome of the components unconstrained. Thesecomponents are arbitrar y functions . inputs.
After choosing these free components, the remaining componentsare determined up to initial conditions. outputs.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.13/22
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Linear diff erential system:
�
.
induced by a pol ynomial matrix
�
:
�
variab le � .
Idea: there are degrees of freedom in the diff erential equation
. In other words: the requirement leavessome of the components � unconstrained. Thesecomponents are arbitrar y functions .
inputs.
After choosing these free components, the remaining componentsare determined up to initial conditions. outputs.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.13/22
![Page 40: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/40.jpg)
Linear diff erential system:
�
.
induced by a pol ynomial matrix
�
:
�
variab le � .
Idea: there are degrees of freedom in the diff erential equation
. In other words: the requirement leavessome of the components � unconstrained. Thesecomponents are arbitrar y functions . inputs.
After choosing these free components, the remaining componentsare determined up to initial conditions. outputs.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.13/22
![Page 41: Lecture 2 LINEAR DIFFERENTIAL SYSTEMS€¦ · Lecture 2 LINEAR DIFFERENTIAL SYSTEMS Harry Trentelman University of Groningen, The Netherlands Minicourse ECC 2003 Cambridge, UK, September](https://reader036.vdocument.in/reader036/viewer/2022081522/5fbf126bb8431c1ade298f9f/html5/thumbnails/41.jpg)
Linear diff erential system:
�
.
induced by a pol ynomial matrix
�
:
�
variab le � .
Idea: there are degrees of freedom in the diff erential equation
. In other words: the requirement leavessome of the components � unconstrained. Thesecomponents are arbitrar y functions . inputs.
After choosing these free components, the remaining componentsare determined up to initial conditions.
outputs.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.13/22
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Linear diff erential system:
�
.
induced by a pol ynomial matrix
�
:
�
variab le � .
Idea: there are degrees of freedom in the diff erential equation
. In other words: the requirement leavessome of the components � unconstrained. Thesecomponents are arbitrar y functions . inputs.
After choosing these free components, the remaining componentsare determined up to initial conditions. outputs.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.13/22
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Linear diff erential system:
�
.
induced by a pol ynomial matrix
�
:
�
variab le � .
Idea: there are degrees of freedom in the diff erential equation
. In other words: the requirement leavessome of the components � unconstrained. Thesecomponents are arbitrar y functions . inputs.
After choosing these free components, the remaining componentsare determined up to initial conditions. outputs.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.13/22
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Example
Position of point mass subject to a force
:
Three (diff erential) equations, six variab les. does notput constraints on : is allo wed to be any function. After
choosing , is determined up to and .
Also: does not put constraints on : is allo wed tobe any function. After choosing , is determined uniquel y.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.14/22
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Example
Position of point mass subject to a force
:
Three (diff erential) equations, six variab les. does notput constraints on : is allo wed to be any function. After
choosing , is determined up to and .
Also: does not put constraints on : is allo wed tobe any function. After choosing , is determined uniquel y.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.14/22
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Example
Position of point mass subject to a force
:
Three (diff erential) equations, six variab les. does notput constraints on : is allo wed to be any function. After
choosing , is determined up to and .
Also: does not put constraints on : is allo wed tobe any function. After choosing , is determined uniquel y.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.14/22
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Freevariables
Let
�
, � .
Let ,
The functions � � � obtained by selectingfrom � onl y the components in theinde x set , form again a linear diff erential system (the eliminationtheorem, see lecture 3).
Denote it by .
The set of variab les is called free in if
where , the cardinality of the set .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.15/22
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Freevariables
Let
�
, � .
Let ,
The functions � � � obtained by selectingfrom � onl y the components in theinde x set , form again a linear diff erential system (the eliminationtheorem, see lecture 3).
Denote it by .
The set of variab les � � � is called free in if
where , the cardinality of the set .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.15/22
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Maximally fr ee
Let
�
, � .
Let
The set of variab les � � � is called
maximall y free in if it is free , and if for any
suc h that we have
So: if is maximall y free , then any set ofvariab les obtained by adding to this set one or more of theremaining variab les is no long er free .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.16/22
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Maximally fr ee
Let
�
, � .
Let
The set of variab les � � � is called
maximall y free in if it is free , and if for any
suc h that we have
So: if � � � is maximall y free , then any set ofvariab les obtained by adding to this set one or more of theremaining variab les is no long er free .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.16/22
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Input/output partition
Let
�
, � .
Possib ly after perm utation of its components, a par tition of into
, with � and
� � � , is called
an input/output par tition in if � is maximall y
free .
In that case , is called an input of , and is called an
output of . Usuall y, we write for , and for .
Non-uniqueness: for given , the manif est variab le in generalallo ws more than one input/output par tition.
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Input/output partition
Let
�
, � .
Possib ly after perm utation of its components, a par tition of into
, with � and
� � � , is called
an input/output par tition in if � is maximall y
free .
In that case , is called an input of , and is called an
output of . Usuall y, we write for , and for .
Non-uniqueness: for given , the manif est variab le in generalallo ws more than one input/output par tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.17/22
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Input/output partition
Let
�
, � .
Possib ly after perm utation of its components, a par tition of into
, with � and
� � � , is called
an input/output par tition in if � is maximall y
free .
In that case , is called an input of , and is called an
output of . Usuall y, we write for , and for .
Non-uniqueness: for given , the manif est variab le in generalallo ws more than one input/output par tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.17/22
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Input/output representations
Let
�
be the system with kernel representation
where , and .
Question: Under what conditions on the pol ynomial matricesand is an input/output par tition (with input andoutput )?Proposition: is an input/output par tition of with input
, output if and onl y if is square and .
The representation is then called an
input/output representation of .The rational matrix is called the transf er matrix of w.r.t.the given input/output par tition
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.18/22
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Input/output representations
Let
�
be the system with kernel representation
where , and .Question: Under what conditions on the pol ynomial matricesand is an input/output par tition (with input andoutput )?
Proposition: is an input/output par tition of with input
, output if and onl y if is square and .
The representation is then called an
input/output representation of .The rational matrix is called the transf er matrix of w.r.t.the given input/output par tition
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.18/22
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Input/output representations
Let
�
be the system with kernel representation
where , and .Question: Under what conditions on the pol ynomial matricesand is an input/output par tition (with input andoutput )?Proposition: is an input/output par tition of with input
, output if and onl y if is square and .
The representation is then called an
input/output representation of .The rational matrix is called the transf er matrix of w.r.t.the given input/output par tition
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.18/22
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Input/output representations
Let
�
be the system with kernel representation
where , and .Question: Under what conditions on the pol ynomial matricesand is an input/output par tition (with input andoutput )?Proposition: is an input/output par tition of with input
, output if and onl y if is square and .
The representation is then called an
input/output representation of .The rational matrix is called the transf er matrix of w.r.t.the given input/output par tition
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.18/22
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Does every
�
have an input/output representation?
Theorem: Let , with manif est variab le . There exists(possib ly after perm utation of the components) a componentwisepar tition of into , and pol ynomial matrices
, , , suc h that
There even exists suc h a par tition suc h that is proper .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.19/22
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Does every
�
have an input/output representation?
Theorem: Let
�
, with manif est variab le . There exists(possib ly after perm utation of the components) a componentwisepar tition of into , and pol ynomial matrices
� �
, ,
� �, suc h that
There even exists suc h a par tition suc h that is proper .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.19/22
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Does every
�
have an input/output representation?
Theorem: Let
�
, with manif est variab le . There exists(possib ly after perm utation of the components) a componentwisepar tition of into , and pol ynomial matrices
� �
, ,
� �, suc h that
There even exists suc h a par tition suc h that is proper .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.19/22
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Input and output cardinality
�
has many input/output par titions . However:the number of input components in any input/output par tition ofis fix ed. This number is denoted by � and is called the
input cardinality of :
� � � � is free in
The output cardinality of , denoted by , is the number of
output components in any input/output par tition of . Obviousl y:
For : .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.20/22
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Input and output cardinality
�
has many input/output par titions . However:the number of input components in any input/output par tition ofis fix ed. This number is denoted by � and is called the
input cardinality of :
� � � � is free in
The output cardinality of , denoted by � , is the number of
output components in any input/output par tition of . Obviousl y:
� �
For : .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.20/22
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Input and output cardinality
�
has many input/output par titions . However:the number of input components in any input/output par tition ofis fix ed. This number is denoted by � and is called the
input cardinality of :
� � � � is free in
The output cardinality of , denoted by � , is the number of
output components in any input/output par tition of . Obviousl y:
� �
For : � .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.20/22
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Summarizing
Linear diff erential systems: those decribed by linear constantcoefficient diff erential equations , etc.
Behavior := the set of solutions (for convenience).
pol ynomial matrix, a kernel
representation of the system induced by .
For a given system , is an input/output par titionif the set of components of is maximall y free: thesecomponents can be chosen arbitraril y. The components ofare then determined up to initial conditions.
An input/output representation of is a special kind of kernel
representation: , , with
. Equiv alent with: is an input/outputpar tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.21/22
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Summarizing
Linear diff erential systems: those decribed by linear constantcoefficient diff erential equations , etc.
Behavior := the set of solutions (for convenience).
pol ynomial matrix, a kernel
representation of the system induced by .
For a given system , is an input/output par titionif the set of components of is maximall y free: thesecomponents can be chosen arbitraril y. The components ofare then determined up to initial conditions.
An input/output representation of is a special kind of kernel
representation: , , with
. Equiv alent with: is an input/outputpar tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.21/22
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Summarizing
Linear diff erential systems: those decribed by linear constantcoefficient diff erential equations , etc.
Behavior := the set of solutions (for convenience).
pol ynomial matrix, a kernel
representation of the system induced by .
For a given system , is an input/output par titionif the set of components of is maximall y free: thesecomponents can be chosen arbitraril y. The components ofare then determined up to initial conditions.
An input/output representation of is a special kind of kernel
representation: , , with
. Equiv alent with: is an input/outputpar tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.21/22
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Summarizing
Linear diff erential systems: those decribed by linear constantcoefficient diff erential equations , etc.
Behavior := the set of solutions (for convenience).
pol ynomial matrix, a kernel
representation of the system induced by .
For a given system , is an input/output par titionif the set of components of is maximall y free: thesecomponents can be chosen arbitraril y. The components ofare then determined up to initial conditions.
An input/output representation of is a special kind of kernel
representation: , , with
. Equiv alent with: is an input/outputpar tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.21/22
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Summarizing
Linear diff erential systems: those decribed by linear constantcoefficient diff erential equations , etc.
Behavior := the set of solutions (for convenience).
pol ynomial matrix, a kernel
representation of the system induced by .
For a given system , is an input/output par titionif the set of components of is maximall y free: thesecomponents can be chosen arbitraril y. The components ofare then determined up to initial conditions.
An input/output representation of is a special kind of kernel
representation: , , with
. Equiv alent with: is an input/outputpar tition.
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.21/22
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A system has in general many i/o representations, so also i/opar titions.
Given , the number of components of is the same in anyi/o par tition . This number is called the inputcardinality of .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.22/22
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A system has in general many i/o representations, so also i/opar titions.
Given , the number of components of is the same in anyi/o par tition . This number is called the inputcardinality � of .
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.22/22
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End of Lecture 2
Lecture 2 LINEAR DIFFERENTIAL SYSTEMS – p.23/22