Stability of Mathieu equation: $x''(t)+cos t ,x(t)=0$
The equation
$$
x''(t)+cos t ,x(t)=0 quad (1)
$$
can be transformed to the system:
$$vec{x}'=
begin{pmatrix}
0 & 1\
-cos t & 0
end{pmatrix} vec{x}=A(t) cdot x(t)
$$
with minimum period $T=2pi$. Let $mu_1,mu_2$ be its characteristic values. A theorem gives:
$$mu_1mu_2=expBigg{int_0^{2pi} tr(A(t))dtBigg}=1 quad (2)
$$
Therefore, the Wronskian of any two linearly independent solutions satisfies:
$$
W(t+2pi)=W(t) quad (3)
$$
Does $(3)$ imply that all solutions are bounded and thus we have asymptotic stability? If not, in what way could we use $(2)$ to determine $(1)$'s stability?
differential-equations dynamical-systems periodic-functions stability-in-odes
add a comment |
The equation
$$
x''(t)+cos t ,x(t)=0 quad (1)
$$
can be transformed to the system:
$$vec{x}'=
begin{pmatrix}
0 & 1\
-cos t & 0
end{pmatrix} vec{x}=A(t) cdot x(t)
$$
with minimum period $T=2pi$. Let $mu_1,mu_2$ be its characteristic values. A theorem gives:
$$mu_1mu_2=expBigg{int_0^{2pi} tr(A(t))dtBigg}=1 quad (2)
$$
Therefore, the Wronskian of any two linearly independent solutions satisfies:
$$
W(t+2pi)=W(t) quad (3)
$$
Does $(3)$ imply that all solutions are bounded and thus we have asymptotic stability? If not, in what way could we use $(2)$ to determine $(1)$'s stability?
differential-equations dynamical-systems periodic-functions stability-in-odes
Determining the numerical solution of $Phi'(t)=A(t)Phi(t)$, $Phi(0)=I_2$ gives $$Phi(2pi)=pmatrix{-8.06518375& 14.50923829\ 4.41423509& -8.06518374}$$ with eigenvalues $-16.06813251$ and $-0.06223499$, so that you have one contracting and one expanding eigenspace.
– LutzL
Dec 1 at 11:25
add a comment |
The equation
$$
x''(t)+cos t ,x(t)=0 quad (1)
$$
can be transformed to the system:
$$vec{x}'=
begin{pmatrix}
0 & 1\
-cos t & 0
end{pmatrix} vec{x}=A(t) cdot x(t)
$$
with minimum period $T=2pi$. Let $mu_1,mu_2$ be its characteristic values. A theorem gives:
$$mu_1mu_2=expBigg{int_0^{2pi} tr(A(t))dtBigg}=1 quad (2)
$$
Therefore, the Wronskian of any two linearly independent solutions satisfies:
$$
W(t+2pi)=W(t) quad (3)
$$
Does $(3)$ imply that all solutions are bounded and thus we have asymptotic stability? If not, in what way could we use $(2)$ to determine $(1)$'s stability?
differential-equations dynamical-systems periodic-functions stability-in-odes
The equation
$$
x''(t)+cos t ,x(t)=0 quad (1)
$$
can be transformed to the system:
$$vec{x}'=
begin{pmatrix}
0 & 1\
-cos t & 0
end{pmatrix} vec{x}=A(t) cdot x(t)
$$
with minimum period $T=2pi$. Let $mu_1,mu_2$ be its characteristic values. A theorem gives:
$$mu_1mu_2=expBigg{int_0^{2pi} tr(A(t))dtBigg}=1 quad (2)
$$
Therefore, the Wronskian of any two linearly independent solutions satisfies:
$$
W(t+2pi)=W(t) quad (3)
$$
Does $(3)$ imply that all solutions are bounded and thus we have asymptotic stability? If not, in what way could we use $(2)$ to determine $(1)$'s stability?
differential-equations dynamical-systems periodic-functions stability-in-odes
differential-equations dynamical-systems periodic-functions stability-in-odes
asked Nov 30 at 20:03
Jevaut
64010
64010
Determining the numerical solution of $Phi'(t)=A(t)Phi(t)$, $Phi(0)=I_2$ gives $$Phi(2pi)=pmatrix{-8.06518375& 14.50923829\ 4.41423509& -8.06518374}$$ with eigenvalues $-16.06813251$ and $-0.06223499$, so that you have one contracting and one expanding eigenspace.
– LutzL
Dec 1 at 11:25
add a comment |
Determining the numerical solution of $Phi'(t)=A(t)Phi(t)$, $Phi(0)=I_2$ gives $$Phi(2pi)=pmatrix{-8.06518375& 14.50923829\ 4.41423509& -8.06518374}$$ with eigenvalues $-16.06813251$ and $-0.06223499$, so that you have one contracting and one expanding eigenspace.
– LutzL
Dec 1 at 11:25
Determining the numerical solution of $Phi'(t)=A(t)Phi(t)$, $Phi(0)=I_2$ gives $$Phi(2pi)=pmatrix{-8.06518375& 14.50923829\ 4.41423509& -8.06518374}$$ with eigenvalues $-16.06813251$ and $-0.06223499$, so that you have one contracting and one expanding eigenspace.
– LutzL
Dec 1 at 11:25
Determining the numerical solution of $Phi'(t)=A(t)Phi(t)$, $Phi(0)=I_2$ gives $$Phi(2pi)=pmatrix{-8.06518375& 14.50923829\ 4.41423509& -8.06518374}$$ with eigenvalues $-16.06813251$ and $-0.06223499$, so that you have one contracting and one expanding eigenspace.
– LutzL
Dec 1 at 11:25
add a comment |
1 Answer
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Hint :
If you want to make a conclusion about the stability of the given system and thus the initial equation via Floquet Theory (as your initial approach), then there is a theorem, that states that if for a multiplier $mu_j$ for your given system, it is $|mu_j| <1$, then the system is unstable. But, that's true, if you can prove that :
$$mu_1mu_2 = 1 Rightarrow |mu_1mu_2| = 1 Leftrightarrow |mu_1| = frac{1}{|mu_2|} <1, ; text{if} ; mu_1, mu_2 neq 1$$
In order to conclude that, use the case of the characteristic matrix being periodic, thus $Phi(t+T) = Phi(t) Rightarrow Phi(2 pi) = Phi(0)E Rightarrow E= Phi(0)^{-1}Phi(2pi)$.
Now, the characteristic values will be the eigenvalues of the matrix $E$. You can calculate them (or approximate them) and conclude if $mu_1,mu_2 neq 1$.
You can find more information and elaborations (proofs etc) about that theorem (which also states 2 cases about stability and asymptotic stability) and Floquet Theory in general, here.
Graphs :
(A phase portrait for a certain $t$) For a simple case of time $t$ such that $cos t = -1$, the system has the image of the phase portrait :
$qquad qquad qquad quad$
which is a saddle, thus unstable.
Now, a sample solution family by sampling some initial values for the solution of the given equation and its derivative, one can see the unstability :
$qquad qquad qquad qquad$
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
|
show 7 more comments
Your Answer
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1 Answer
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1 Answer
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active
oldest
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active
oldest
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active
oldest
votes
Hint :
If you want to make a conclusion about the stability of the given system and thus the initial equation via Floquet Theory (as your initial approach), then there is a theorem, that states that if for a multiplier $mu_j$ for your given system, it is $|mu_j| <1$, then the system is unstable. But, that's true, if you can prove that :
$$mu_1mu_2 = 1 Rightarrow |mu_1mu_2| = 1 Leftrightarrow |mu_1| = frac{1}{|mu_2|} <1, ; text{if} ; mu_1, mu_2 neq 1$$
In order to conclude that, use the case of the characteristic matrix being periodic, thus $Phi(t+T) = Phi(t) Rightarrow Phi(2 pi) = Phi(0)E Rightarrow E= Phi(0)^{-1}Phi(2pi)$.
Now, the characteristic values will be the eigenvalues of the matrix $E$. You can calculate them (or approximate them) and conclude if $mu_1,mu_2 neq 1$.
You can find more information and elaborations (proofs etc) about that theorem (which also states 2 cases about stability and asymptotic stability) and Floquet Theory in general, here.
Graphs :
(A phase portrait for a certain $t$) For a simple case of time $t$ such that $cos t = -1$, the system has the image of the phase portrait :
$qquad qquad qquad quad$
which is a saddle, thus unstable.
Now, a sample solution family by sampling some initial values for the solution of the given equation and its derivative, one can see the unstability :
$qquad qquad qquad qquad$
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
|
show 7 more comments
Hint :
If you want to make a conclusion about the stability of the given system and thus the initial equation via Floquet Theory (as your initial approach), then there is a theorem, that states that if for a multiplier $mu_j$ for your given system, it is $|mu_j| <1$, then the system is unstable. But, that's true, if you can prove that :
$$mu_1mu_2 = 1 Rightarrow |mu_1mu_2| = 1 Leftrightarrow |mu_1| = frac{1}{|mu_2|} <1, ; text{if} ; mu_1, mu_2 neq 1$$
In order to conclude that, use the case of the characteristic matrix being periodic, thus $Phi(t+T) = Phi(t) Rightarrow Phi(2 pi) = Phi(0)E Rightarrow E= Phi(0)^{-1}Phi(2pi)$.
Now, the characteristic values will be the eigenvalues of the matrix $E$. You can calculate them (or approximate them) and conclude if $mu_1,mu_2 neq 1$.
You can find more information and elaborations (proofs etc) about that theorem (which also states 2 cases about stability and asymptotic stability) and Floquet Theory in general, here.
Graphs :
(A phase portrait for a certain $t$) For a simple case of time $t$ such that $cos t = -1$, the system has the image of the phase portrait :
$qquad qquad qquad quad$
which is a saddle, thus unstable.
Now, a sample solution family by sampling some initial values for the solution of the given equation and its derivative, one can see the unstability :
$qquad qquad qquad qquad$
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
|
show 7 more comments
Hint :
If you want to make a conclusion about the stability of the given system and thus the initial equation via Floquet Theory (as your initial approach), then there is a theorem, that states that if for a multiplier $mu_j$ for your given system, it is $|mu_j| <1$, then the system is unstable. But, that's true, if you can prove that :
$$mu_1mu_2 = 1 Rightarrow |mu_1mu_2| = 1 Leftrightarrow |mu_1| = frac{1}{|mu_2|} <1, ; text{if} ; mu_1, mu_2 neq 1$$
In order to conclude that, use the case of the characteristic matrix being periodic, thus $Phi(t+T) = Phi(t) Rightarrow Phi(2 pi) = Phi(0)E Rightarrow E= Phi(0)^{-1}Phi(2pi)$.
Now, the characteristic values will be the eigenvalues of the matrix $E$. You can calculate them (or approximate them) and conclude if $mu_1,mu_2 neq 1$.
You can find more information and elaborations (proofs etc) about that theorem (which also states 2 cases about stability and asymptotic stability) and Floquet Theory in general, here.
Graphs :
(A phase portrait for a certain $t$) For a simple case of time $t$ such that $cos t = -1$, the system has the image of the phase portrait :
$qquad qquad qquad quad$
which is a saddle, thus unstable.
Now, a sample solution family by sampling some initial values for the solution of the given equation and its derivative, one can see the unstability :
$qquad qquad qquad qquad$
Hint :
If you want to make a conclusion about the stability of the given system and thus the initial equation via Floquet Theory (as your initial approach), then there is a theorem, that states that if for a multiplier $mu_j$ for your given system, it is $|mu_j| <1$, then the system is unstable. But, that's true, if you can prove that :
$$mu_1mu_2 = 1 Rightarrow |mu_1mu_2| = 1 Leftrightarrow |mu_1| = frac{1}{|mu_2|} <1, ; text{if} ; mu_1, mu_2 neq 1$$
In order to conclude that, use the case of the characteristic matrix being periodic, thus $Phi(t+T) = Phi(t) Rightarrow Phi(2 pi) = Phi(0)E Rightarrow E= Phi(0)^{-1}Phi(2pi)$.
Now, the characteristic values will be the eigenvalues of the matrix $E$. You can calculate them (or approximate them) and conclude if $mu_1,mu_2 neq 1$.
You can find more information and elaborations (proofs etc) about that theorem (which also states 2 cases about stability and asymptotic stability) and Floquet Theory in general, here.
Graphs :
(A phase portrait for a certain $t$) For a simple case of time $t$ such that $cos t = -1$, the system has the image of the phase portrait :
$qquad qquad qquad quad$
which is a saddle, thus unstable.
Now, a sample solution family by sampling some initial values for the solution of the given equation and its derivative, one can see the unstability :
$qquad qquad qquad qquad$
edited Dec 1 at 11:00
answered Nov 30 at 21:16
Rebellos
14.4k31245
14.4k31245
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
|
show 7 more comments
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
You cannot use the linearization to infer the stability of a time dependent system.
– Artem
Nov 30 at 21:25
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
Once again, you cannot use eigenvalues of time dependent systems to conclude the stability. -1.
– Artem
Nov 30 at 21:28
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Fine, I altered my answer to only use the Floquet Theory approach which is the standard and theoritical way of handling time dependent systems (also given abstracts and conent for further justification and studying).
– Rebellos
Nov 30 at 21:45
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
@Artem Any issues now for that -1 ?
– Rebellos
Nov 30 at 21:54
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
1. There is no such thing as a "phase portrait" for a time dependent system. Also, your reasoning about multipliers is incorrect.
– Artem
Nov 30 at 22:19
|
show 7 more comments
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Determining the numerical solution of $Phi'(t)=A(t)Phi(t)$, $Phi(0)=I_2$ gives $$Phi(2pi)=pmatrix{-8.06518375& 14.50923829\ 4.41423509& -8.06518374}$$ with eigenvalues $-16.06813251$ and $-0.06223499$, so that you have one contracting and one expanding eigenspace.
– LutzL
Dec 1 at 11:25