SlideShare a Scribd company logo
1 of 10
Ch 7.4: Basic Theory of Systems of First
Order Linear Equations
The general theory of a system of n first order linear equations
parallels that of a single nth order linear equation.
This system can be written as x' = P(t)x + g(t), where
)()()()(
)()()()(
)()()()(
2211
222221212
112121111
tgxtpxtpxtpx
tgxtpxtpxtpx
tgxtpxtpxtpx
nnnnnnn
nn
nn
++++=′
++++=′
++++=′


















=














=














=
)()()(
)()()(
)()()(
)(,
)(
)(
)(
)(,
)(
)(
)(
)(
21
22221
11211
2
1
2
1
tptptp
tptptp
tptptp
t
tg
tg
tg
t
tx
tx
tx
t
nnnn
n
n
nn 




Pgx
Vector Solutions of an ODE System
A vector x = φ(t) is a solution of x' = P(t)x + g(t) if the
components of x,
satisfy the system of equations on I: α < t < β.
For comparison, recall that x' = P(t)x + g(t) represents our
system of equations
Assuming P and g continuous on I, such a solution exists by
Theorem 7.1.2.
),(,),(),( 2211 txtxtx nn φφφ === 
)()()()(
)()()()(
)()()()(
2211
222221212
112121111
tgxtpxtpxtpx
tgxtpxtpxtpx
tgxtpxtpxtpx
nnnnnnn
nn
nn
++++=′
++++=′
++++=′




Example 1
Consider the homogeneous equation x' = P(t)x below, with
the solutions x as indicated.
To see that x is a solution, substitute x into the equation and
perform the indicated operations:
t
t
t
e
e
e
t 3
3
3
2
1
2
)(;
14
11






=







=





=′ xxx
xx ′=







=







=













=





t
t
t
t
t
t
e
e
e
e
e
e
3
3
3
3
3
3
2
3
6
3
214
11
14
11
Homogeneous Case; Vector Function Notation
As in Chapters 3 and 4, we first examine the general
homogeneous equation x' = P(t)x.
Also, the following notation for the vector functions
x(1)
, x(2)
,…, x(k)
,… will be used:




,
)(
)(
)(
)(,,
)(
)(
)(
)(,
)(
)(
)(
)( 2
1
)(
2
22
12
)2(
1
21
11
)1(














=














=














=
tx
tx
tx
t
tx
tx
tx
t
tx
tx
tx
t
nn
n
n
k
nn
xxx
Theorem 7.4.1
If the vector functions x(1)
and x(2)
are solutions of the system
x' = P(t)x, then the linear combination c1x(1)
+ c2x(2)
is also a
solution for any constants c1 and c2.
Note: By repeatedly applying the result of this theorem, it
can be seen that every finite linear combination
of solutions x(1)
, x(2)
,…, x(k)
is itself a solution to x' = P(t)x.
)()()( )()2(
2
)1(
1 tctctc k
k xxxx +++= 
Example 2
Consider the homogeneous equation x' = P(t)x below, with
the two solutions x(1)
and x(2)
as indicated.
Then x = c1x(1)
+ c2x(2)
is also a solution:








−
=







=





=′ −
−
t
t
t
t
e
e
t
e
e
t
2
)(,
2
)(;
14
11 )2(
3
3
)1(
xxxx
x
x
′=






−
+







=







−
+







=








−





+













=





−
−
−
−
−
−
t
t
t
t
t
t
t
t
t
t
t
t
e
e
c
e
e
c
ec
ec
ec
ec
ec
ec
ec
ec
26
3
26
3
214
11
214
11
14
11
23
3
1
2
2
3
1
3
1
2
2
3
1
3
1
Theorem 7.4.2
If x(1)
, x(2)
,…, x(n)
are linearly independent solutions of the
system x' = P(t)x for each point in I: α < t < β, then each
solution x = φ(t) can be expressed uniquely in the form
If solutions x(1)
,…, x(n)
are linearly independent for each point
in I: α < t < β, then they are fundamental solutions on I,
and the general solution is given by
)()()( )()2(
2
)1(
1 tctctc n
nxxxx +++= 
)()()( )()2(
2
)1(
1 tctctc n
nxxxx +++= 
The Wronskian and Linear Independence
The proof of Thm 7.4.2 uses the fact that if x(1)
, x(2)
,…, x(n)
are
linearly independent on I, then detX(t) ≠ 0 on I, where
The Wronskian of x(1)
,…, x(n)
is defined as
W[x(1)
,…, x(n)
](t) = detX(t).
It follows that W[x(1)
,…, x(n)
](t) ≠ 0 on I iff x(1)
,…, x(n)
are
linearly independent for each point in I.
,
)()(
)()(
)(
1
111










=
txtx
txtx
t
nnn
n



X
Theorem 7.4.3
If x(1)
, x(2)
,…, x(n)
are solutions of the system x' = P(t)x on I: α
< t < β, then the Wronskian W[x(1)
,…, x(n)
](t) is either
identically zero on I or else is never zero on I.
This result enables us to determine whether a given set of
solutions x(1)
, x(2)
,…, x(n)
are fundamental solutions by
evaluating W[x(1)
,…, x(n)
](t) at any point t in α < t < β.
Theorem 7.4.4
Let
Let x(1)
, x(2)
,…, x(n)
be solutions of the system x' = P(t)x,
α < t < β, that satisfy the initial conditions
respectively, where t0 is any point in α < t < β. Then
x(1)
, x(2)
,…, x(n)
are fundamental solutions of x' = P(t)x.
















=
















=
















=
1
0
0
0
,,
0
0
1
0
,
0
0
0
1
)()2()1(


n
eee
,)(,,)( )(
0
)()1(
0
)1( nn
tt exex == 

More Related Content

What's hot

Differential Equations Lecture: Non-Homogeneous Linear Differential Equations
Differential Equations Lecture: Non-Homogeneous Linear Differential EquationsDifferential Equations Lecture: Non-Homogeneous Linear Differential Equations
Differential Equations Lecture: Non-Homogeneous Linear Differential Equationsbullardcr
 
Digital text book
Digital text bookDigital text book
Digital text bookshareenapr5
 
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...IOSR Journals
 
E041046051
E041046051E041046051
E041046051inventy
 
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...ieijjournal
 
Finite difference method
Finite difference methodFinite difference method
Finite difference methodDivyansh Verma
 
Numerical Methods
Numerical MethodsNumerical Methods
Numerical MethodsTeja Ande
 
Partial Differential Equation - Notes
Partial Differential Equation - NotesPartial Differential Equation - Notes
Partial Differential Equation - NotesDr. Nirav Vyas
 

What's hot (18)

Differential Equations Lecture: Non-Homogeneous Linear Differential Equations
Differential Equations Lecture: Non-Homogeneous Linear Differential EquationsDifferential Equations Lecture: Non-Homogeneous Linear Differential Equations
Differential Equations Lecture: Non-Homogeneous Linear Differential Equations
 
Shareena p r
Shareena p r Shareena p r
Shareena p r
 
Digital text book
Digital text bookDigital text book
Digital text book
 
Ch08 1
Ch08 1Ch08 1
Ch08 1
 
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...
 
E041046051
E041046051E041046051
E041046051
 
Deconvolution
DeconvolutionDeconvolution
Deconvolution
 
Unit1 vrs
Unit1 vrsUnit1 vrs
Unit1 vrs
 
Section3 stochastic
Section3 stochasticSection3 stochastic
Section3 stochastic
 
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...
 
Sect4 4
Sect4 4Sect4 4
Sect4 4
 
Unit2 vrs
Unit2 vrsUnit2 vrs
Unit2 vrs
 
Finite difference method
Finite difference methodFinite difference method
Finite difference method
 
Ma2002 1.19 rm
Ma2002 1.19 rmMa2002 1.19 rm
Ma2002 1.19 rm
 
maths
maths maths
maths
 
Numerical Methods
Numerical MethodsNumerical Methods
Numerical Methods
 
Partial Differential Equation - Notes
Partial Differential Equation - NotesPartial Differential Equation - Notes
Partial Differential Equation - Notes
 
Bca numer
Bca numerBca numer
Bca numer
 

Viewers also liked

Wronskianと一次独立性
Wronskianと一次独立性Wronskianと一次独立性
Wronskianと一次独立性HanpenRobot
 
Soy protein copy
Soy protein   copySoy protein   copy
Soy protein copyDevang Shah
 
Term paper on new product development process
Term paper on new product development processTerm paper on new product development process
Term paper on new product development processShourav Mahmud
 
honey jose presentation
honey jose presentationhoney jose presentation
honey jose presentationHoney jose
 
Second order homogeneous linear differential equations
Second order homogeneous linear differential equations Second order homogeneous linear differential equations
Second order homogeneous linear differential equations Viraj Patel
 
Causes and effects of inflation
Causes and effects of inflationCauses and effects of inflation
Causes and effects of inflationJanayeC
 

Viewers also liked (9)

Ch03 4
Ch03 4Ch03 4
Ch03 4
 
Ch03 5
Ch03 5Ch03 5
Ch03 5
 
Ch03 3
Ch03 3Ch03 3
Ch03 3
 
Wronskianと一次独立性
Wronskianと一次独立性Wronskianと一次独立性
Wronskianと一次独立性
 
Soy protein copy
Soy protein   copySoy protein   copy
Soy protein copy
 
Term paper on new product development process
Term paper on new product development processTerm paper on new product development process
Term paper on new product development process
 
honey jose presentation
honey jose presentationhoney jose presentation
honey jose presentation
 
Second order homogeneous linear differential equations
Second order homogeneous linear differential equations Second order homogeneous linear differential equations
Second order homogeneous linear differential equations
 
Causes and effects of inflation
Causes and effects of inflationCauses and effects of inflation
Causes and effects of inflation
 

Similar to Ch07 4

Similar to Ch07 4 (20)

Continuous Time Convolution1. Solve the following for y(t.docx
Continuous Time Convolution1. Solve the following for y(t.docxContinuous Time Convolution1. Solve the following for y(t.docx
Continuous Time Convolution1. Solve the following for y(t.docx
 
Signal Processing Assignment Help
Signal Processing Assignment HelpSignal Processing Assignment Help
Signal Processing Assignment Help
 
Design of Linear Control Systems(0).ppt
Design of Linear Control Systems(0).pptDesign of Linear Control Systems(0).ppt
Design of Linear Control Systems(0).ppt
 
5_2019_02_01!09_42_56_PM.pptx
5_2019_02_01!09_42_56_PM.pptx5_2019_02_01!09_42_56_PM.pptx
5_2019_02_01!09_42_56_PM.pptx
 
On the Application of the Fixed Point Theory to the Solution of Systems of Li...
On the Application of the Fixed Point Theory to the Solution of Systems of Li...On the Application of the Fixed Point Theory to the Solution of Systems of Li...
On the Application of the Fixed Point Theory to the Solution of Systems of Li...
 
03_AJMS_170_19_RA.pdf
03_AJMS_170_19_RA.pdf03_AJMS_170_19_RA.pdf
03_AJMS_170_19_RA.pdf
 
03_AJMS_170_19_RA.pdf
03_AJMS_170_19_RA.pdf03_AJMS_170_19_RA.pdf
03_AJMS_170_19_RA.pdf
 
legendre.pptx
legendre.pptxlegendre.pptx
legendre.pptx
 
P3.4,p3.2
P3.4,p3.2P3.4,p3.2
P3.4,p3.2
 
05_AJMS_332_21.pdf
05_AJMS_332_21.pdf05_AJMS_332_21.pdf
05_AJMS_332_21.pdf
 
adspchap1.pdf
adspchap1.pdfadspchap1.pdf
adspchap1.pdf
 
K12105 sharukh...
K12105 sharukh...K12105 sharukh...
K12105 sharukh...
 
Ch07 5
Ch07 5Ch07 5
Ch07 5
 
Ch07 1
Ch07 1Ch07 1
Ch07 1
 
Unit v rpq1
Unit v rpq1Unit v rpq1
Unit v rpq1
 
Ch04 2
Ch04 2Ch04 2
Ch04 2
 
Lect3-signal-processing.pdf
Lect3-signal-processing.pdfLect3-signal-processing.pdf
Lect3-signal-processing.pdf
 
Random Matrix Theory and Machine Learning - Part 3
Random Matrix Theory and Machine Learning - Part 3Random Matrix Theory and Machine Learning - Part 3
Random Matrix Theory and Machine Learning - Part 3
 
Signals and systems: Part ii
Signals and systems:  Part iiSignals and systems:  Part ii
Signals and systems: Part ii
 
Manual solucoes ex_extras
Manual solucoes ex_extrasManual solucoes ex_extras
Manual solucoes ex_extras
 

More from Rendy Robert (20)

Ch08 3
Ch08 3Ch08 3
Ch08 3
 
Ch07 3
Ch07 3Ch07 3
Ch07 3
 
Ch07 2
Ch07 2Ch07 2
Ch07 2
 
Ch06 6
Ch06 6Ch06 6
Ch06 6
 
Ch06 5
Ch06 5Ch06 5
Ch06 5
 
Ch06 4
Ch06 4Ch06 4
Ch06 4
 
Ch06 3
Ch06 3Ch06 3
Ch06 3
 
Ch06 2
Ch06 2Ch06 2
Ch06 2
 
Ch06 1
Ch06 1Ch06 1
Ch06 1
 
Ch05 8
Ch05 8Ch05 8
Ch05 8
 
Ch05 7
Ch05 7Ch05 7
Ch05 7
 
Ch05 6
Ch05 6Ch05 6
Ch05 6
 
Ch05 5
Ch05 5Ch05 5
Ch05 5
 
Ch05 4
Ch05 4Ch05 4
Ch05 4
 
Ch05 3
Ch05 3Ch05 3
Ch05 3
 
Ch05 2
Ch05 2Ch05 2
Ch05 2
 
Ch05 1
Ch05 1Ch05 1
Ch05 1
 
Ch04 4
Ch04 4Ch04 4
Ch04 4
 
Ch04 3
Ch04 3Ch04 3
Ch04 3
 
Ch04 1
Ch04 1Ch04 1
Ch04 1
 

Ch07 4

  • 1. Ch 7.4: Basic Theory of Systems of First Order Linear Equations The general theory of a system of n first order linear equations parallels that of a single nth order linear equation. This system can be written as x' = P(t)x + g(t), where )()()()( )()()()( )()()()( 2211 222221212 112121111 tgxtpxtpxtpx tgxtpxtpxtpx tgxtpxtpxtpx nnnnnnn nn nn ++++=′ ++++=′ ++++=′                   =               =               = )()()( )()()( )()()( )(, )( )( )( )(, )( )( )( )( 21 22221 11211 2 1 2 1 tptptp tptptp tptptp t tg tg tg t tx tx tx t nnnn n n nn      Pgx
  • 2. Vector Solutions of an ODE System A vector x = φ(t) is a solution of x' = P(t)x + g(t) if the components of x, satisfy the system of equations on I: α < t < β. For comparison, recall that x' = P(t)x + g(t) represents our system of equations Assuming P and g continuous on I, such a solution exists by Theorem 7.1.2. ),(,),(),( 2211 txtxtx nn φφφ ===  )()()()( )()()()( )()()()( 2211 222221212 112121111 tgxtpxtpxtpx tgxtpxtpxtpx tgxtpxtpxtpx nnnnnnn nn nn ++++=′ ++++=′ ++++=′    
  • 3. Example 1 Consider the homogeneous equation x' = P(t)x below, with the solutions x as indicated. To see that x is a solution, substitute x into the equation and perform the indicated operations: t t t e e e t 3 3 3 2 1 2 )(; 14 11       =        =      =′ xxx xx ′=        =        =              =      t t t t t t e e e e e e 3 3 3 3 3 3 2 3 6 3 214 11 14 11
  • 4. Homogeneous Case; Vector Function Notation As in Chapters 3 and 4, we first examine the general homogeneous equation x' = P(t)x. Also, the following notation for the vector functions x(1) , x(2) ,…, x(k) ,… will be used:     , )( )( )( )(,, )( )( )( )(, )( )( )( )( 2 1 )( 2 22 12 )2( 1 21 11 )1(               =               =               = tx tx tx t tx tx tx t tx tx tx t nn n n k nn xxx
  • 5. Theorem 7.4.1 If the vector functions x(1) and x(2) are solutions of the system x' = P(t)x, then the linear combination c1x(1) + c2x(2) is also a solution for any constants c1 and c2. Note: By repeatedly applying the result of this theorem, it can be seen that every finite linear combination of solutions x(1) , x(2) ,…, x(k) is itself a solution to x' = P(t)x. )()()( )()2( 2 )1( 1 tctctc k k xxxx +++= 
  • 6. Example 2 Consider the homogeneous equation x' = P(t)x below, with the two solutions x(1) and x(2) as indicated. Then x = c1x(1) + c2x(2) is also a solution:         − =        =      =′ − − t t t t e e t e e t 2 )(, 2 )(; 14 11 )2( 3 3 )1( xxxx x x ′=       − +        =        − +        =         −      +              =      − − − − − − t t t t t t t t t t t t e e c e e c ec ec ec ec ec ec ec ec 26 3 26 3 214 11 214 11 14 11 23 3 1 2 2 3 1 3 1 2 2 3 1 3 1
  • 7. Theorem 7.4.2 If x(1) , x(2) ,…, x(n) are linearly independent solutions of the system x' = P(t)x for each point in I: α < t < β, then each solution x = φ(t) can be expressed uniquely in the form If solutions x(1) ,…, x(n) are linearly independent for each point in I: α < t < β, then they are fundamental solutions on I, and the general solution is given by )()()( )()2( 2 )1( 1 tctctc n nxxxx +++=  )()()( )()2( 2 )1( 1 tctctc n nxxxx +++= 
  • 8. The Wronskian and Linear Independence The proof of Thm 7.4.2 uses the fact that if x(1) , x(2) ,…, x(n) are linearly independent on I, then detX(t) ≠ 0 on I, where The Wronskian of x(1) ,…, x(n) is defined as W[x(1) ,…, x(n) ](t) = detX(t). It follows that W[x(1) ,…, x(n) ](t) ≠ 0 on I iff x(1) ,…, x(n) are linearly independent for each point in I. , )()( )()( )( 1 111           = txtx txtx t nnn n    X
  • 9. Theorem 7.4.3 If x(1) , x(2) ,…, x(n) are solutions of the system x' = P(t)x on I: α < t < β, then the Wronskian W[x(1) ,…, x(n) ](t) is either identically zero on I or else is never zero on I. This result enables us to determine whether a given set of solutions x(1) , x(2) ,…, x(n) are fundamental solutions by evaluating W[x(1) ,…, x(n) ](t) at any point t in α < t < β.
  • 10. Theorem 7.4.4 Let Let x(1) , x(2) ,…, x(n) be solutions of the system x' = P(t)x, α < t < β, that satisfy the initial conditions respectively, where t0 is any point in α < t < β. Then x(1) , x(2) ,…, x(n) are fundamental solutions of x' = P(t)x.                 =                 =                 = 1 0 0 0 ,, 0 0 1 0 , 0 0 0 1 )()2()1(   n eee ,)(,,)( )( 0 )()1( 0 )1( nn tt exex == 