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What transparent parametrizations of 2x2 matrices are there?



Announcing the arrival of Valued Associate #679: Cesar Manara
Planned maintenance scheduled April 23, 2019 at 00:00UTC (8:00pm US/Eastern)Solution to system of difference equations with repeated unit rootsEigenvectors of a $2 times 2$ matrix when the eigenvalues are not integersB and C matrices for real modal representation of a 2x2 linear system with complex eigenvaluesInverse spectrum problem - showing the existence of a 2x2 doubly stochastic matrix,Prove that $lambda_1^2$, $lambda_1lambda_2$ and $lambda_2^2$ are eigenvalues of matrix $A$Find “REAL” cannonical form of 4x4 matrixConjugate classes for 2x2 matriceseigenvalues of a 6x6 matrix with many zerosDetermining the maximum number of linearly independent rows and columns for a given matrixEquilibria of 2x2 linear system












1












$begingroup$


I want to contruct a time series by a recurrence relation $y_t = Ay_{t-1}$, where A is a 2x2 real matrix. Assume $y_0$ is some known initial condition. Also, I assume $y_i in mathbb R^2$.



To understand the system without having to solve the equation, it would be nice to have a parametrization of the matrix that is transparent with the behavior of the solution.



The most simple parametrization would be by the real entries in the matrix. Use $(a,b,c,d)$. Unfortunately, it is not easy to understand the dynamics of the system easily by this set of parameters.



$$ A_{a,b,c,d} = begin{bmatrix}
a& b\
c & d
end{bmatrix}$$



Option two is if the matrix is (real) diagonalizable. Taking the eigenvalues $(lambda_1,lambda_2)$. On the downside, this will only give system dynamics that are exponential growth of decline.



$$ B_{lambda_1,lambda_2} = begin{bmatrix}
lambda_1& 0\
0 & lambda_2
end{bmatrix}$$



Option three is to think of the solutions as damped pendulum solutions. Then the paramterization is $(zeta, omega)$, giving below matrix. The notation is inspired by https://en.wikipedia.org/wiki/Harmonic_oscillator, but it is not perfectly equivalent. In this notation, I can easily read off the dampening of the solutions, since $zeta$ is the real part of the eigenvalues, and the frequency, since $omega$ gives the imaginary part of the eigenvalues.



$$ C_{zeta,omega} = begin{bmatrix}
zeta& -omega\
omega & zeta
end{bmatrix}
$$



The three examples are not satisfactory to me, since they produce either (A) solutions that are not easily coupled to the parameters, (B) noninteresting dynamics, or (C) only spans a 2-dimensional subspace of all 2x2-matrices.



My question: What other parametrizations of real 2x2 matrices is there, that give instant intuition for the corresponding dynamical system?










share|cite|improve this question











$endgroup$












  • $begingroup$
    I don't know what you mean by parametrization of a matrix, but, if the matrix is diagonalizable, then the recurrence can be rewritten in terms of the diagonal matrix (and the eigenvectors).
    $endgroup$
    – Gerry Myerson
    Mar 25 at 9:53










  • $begingroup$
    I have updated the question now. Is it clearer in this phrasing?
    $endgroup$
    – LudvigH
    Mar 25 at 10:20










  • $begingroup$
    Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},pmatrix{a&1cr0&acr},pmatrix{a&-bcr b&a}$$ Each of those gives about as much insight as there is into the behavior of the dynamical system.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 10:40












  • $begingroup$
    That is just about the type of answer I hoped for. Write it as an answer and I'll accept it. :)
    $endgroup$
    – LudvigH
    Mar 25 at 11:14
















1












$begingroup$


I want to contruct a time series by a recurrence relation $y_t = Ay_{t-1}$, where A is a 2x2 real matrix. Assume $y_0$ is some known initial condition. Also, I assume $y_i in mathbb R^2$.



To understand the system without having to solve the equation, it would be nice to have a parametrization of the matrix that is transparent with the behavior of the solution.



The most simple parametrization would be by the real entries in the matrix. Use $(a,b,c,d)$. Unfortunately, it is not easy to understand the dynamics of the system easily by this set of parameters.



$$ A_{a,b,c,d} = begin{bmatrix}
a& b\
c & d
end{bmatrix}$$



Option two is if the matrix is (real) diagonalizable. Taking the eigenvalues $(lambda_1,lambda_2)$. On the downside, this will only give system dynamics that are exponential growth of decline.



$$ B_{lambda_1,lambda_2} = begin{bmatrix}
lambda_1& 0\
0 & lambda_2
end{bmatrix}$$



Option three is to think of the solutions as damped pendulum solutions. Then the paramterization is $(zeta, omega)$, giving below matrix. The notation is inspired by https://en.wikipedia.org/wiki/Harmonic_oscillator, but it is not perfectly equivalent. In this notation, I can easily read off the dampening of the solutions, since $zeta$ is the real part of the eigenvalues, and the frequency, since $omega$ gives the imaginary part of the eigenvalues.



$$ C_{zeta,omega} = begin{bmatrix}
zeta& -omega\
omega & zeta
end{bmatrix}
$$



The three examples are not satisfactory to me, since they produce either (A) solutions that are not easily coupled to the parameters, (B) noninteresting dynamics, or (C) only spans a 2-dimensional subspace of all 2x2-matrices.



My question: What other parametrizations of real 2x2 matrices is there, that give instant intuition for the corresponding dynamical system?










share|cite|improve this question











$endgroup$












  • $begingroup$
    I don't know what you mean by parametrization of a matrix, but, if the matrix is diagonalizable, then the recurrence can be rewritten in terms of the diagonal matrix (and the eigenvectors).
    $endgroup$
    – Gerry Myerson
    Mar 25 at 9:53










  • $begingroup$
    I have updated the question now. Is it clearer in this phrasing?
    $endgroup$
    – LudvigH
    Mar 25 at 10:20










  • $begingroup$
    Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},pmatrix{a&1cr0&acr},pmatrix{a&-bcr b&a}$$ Each of those gives about as much insight as there is into the behavior of the dynamical system.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 10:40












  • $begingroup$
    That is just about the type of answer I hoped for. Write it as an answer and I'll accept it. :)
    $endgroup$
    – LudvigH
    Mar 25 at 11:14














1












1








1


1



$begingroup$


I want to contruct a time series by a recurrence relation $y_t = Ay_{t-1}$, where A is a 2x2 real matrix. Assume $y_0$ is some known initial condition. Also, I assume $y_i in mathbb R^2$.



To understand the system without having to solve the equation, it would be nice to have a parametrization of the matrix that is transparent with the behavior of the solution.



The most simple parametrization would be by the real entries in the matrix. Use $(a,b,c,d)$. Unfortunately, it is not easy to understand the dynamics of the system easily by this set of parameters.



$$ A_{a,b,c,d} = begin{bmatrix}
a& b\
c & d
end{bmatrix}$$



Option two is if the matrix is (real) diagonalizable. Taking the eigenvalues $(lambda_1,lambda_2)$. On the downside, this will only give system dynamics that are exponential growth of decline.



$$ B_{lambda_1,lambda_2} = begin{bmatrix}
lambda_1& 0\
0 & lambda_2
end{bmatrix}$$



Option three is to think of the solutions as damped pendulum solutions. Then the paramterization is $(zeta, omega)$, giving below matrix. The notation is inspired by https://en.wikipedia.org/wiki/Harmonic_oscillator, but it is not perfectly equivalent. In this notation, I can easily read off the dampening of the solutions, since $zeta$ is the real part of the eigenvalues, and the frequency, since $omega$ gives the imaginary part of the eigenvalues.



$$ C_{zeta,omega} = begin{bmatrix}
zeta& -omega\
omega & zeta
end{bmatrix}
$$



The three examples are not satisfactory to me, since they produce either (A) solutions that are not easily coupled to the parameters, (B) noninteresting dynamics, or (C) only spans a 2-dimensional subspace of all 2x2-matrices.



My question: What other parametrizations of real 2x2 matrices is there, that give instant intuition for the corresponding dynamical system?










share|cite|improve this question











$endgroup$




I want to contruct a time series by a recurrence relation $y_t = Ay_{t-1}$, where A is a 2x2 real matrix. Assume $y_0$ is some known initial condition. Also, I assume $y_i in mathbb R^2$.



To understand the system without having to solve the equation, it would be nice to have a parametrization of the matrix that is transparent with the behavior of the solution.



The most simple parametrization would be by the real entries in the matrix. Use $(a,b,c,d)$. Unfortunately, it is not easy to understand the dynamics of the system easily by this set of parameters.



$$ A_{a,b,c,d} = begin{bmatrix}
a& b\
c & d
end{bmatrix}$$



Option two is if the matrix is (real) diagonalizable. Taking the eigenvalues $(lambda_1,lambda_2)$. On the downside, this will only give system dynamics that are exponential growth of decline.



$$ B_{lambda_1,lambda_2} = begin{bmatrix}
lambda_1& 0\
0 & lambda_2
end{bmatrix}$$



Option three is to think of the solutions as damped pendulum solutions. Then the paramterization is $(zeta, omega)$, giving below matrix. The notation is inspired by https://en.wikipedia.org/wiki/Harmonic_oscillator, but it is not perfectly equivalent. In this notation, I can easily read off the dampening of the solutions, since $zeta$ is the real part of the eigenvalues, and the frequency, since $omega$ gives the imaginary part of the eigenvalues.



$$ C_{zeta,omega} = begin{bmatrix}
zeta& -omega\
omega & zeta
end{bmatrix}
$$



The three examples are not satisfactory to me, since they produce either (A) solutions that are not easily coupled to the parameters, (B) noninteresting dynamics, or (C) only spans a 2-dimensional subspace of all 2x2-matrices.



My question: What other parametrizations of real 2x2 matrices is there, that give instant intuition for the corresponding dynamical system?







matrices dynamical-systems






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Mar 25 at 10:19







LudvigH

















asked Mar 25 at 8:59









LudvigHLudvigH

1186




1186












  • $begingroup$
    I don't know what you mean by parametrization of a matrix, but, if the matrix is diagonalizable, then the recurrence can be rewritten in terms of the diagonal matrix (and the eigenvectors).
    $endgroup$
    – Gerry Myerson
    Mar 25 at 9:53










  • $begingroup$
    I have updated the question now. Is it clearer in this phrasing?
    $endgroup$
    – LudvigH
    Mar 25 at 10:20










  • $begingroup$
    Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},pmatrix{a&1cr0&acr},pmatrix{a&-bcr b&a}$$ Each of those gives about as much insight as there is into the behavior of the dynamical system.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 10:40












  • $begingroup$
    That is just about the type of answer I hoped for. Write it as an answer and I'll accept it. :)
    $endgroup$
    – LudvigH
    Mar 25 at 11:14


















  • $begingroup$
    I don't know what you mean by parametrization of a matrix, but, if the matrix is diagonalizable, then the recurrence can be rewritten in terms of the diagonal matrix (and the eigenvectors).
    $endgroup$
    – Gerry Myerson
    Mar 25 at 9:53










  • $begingroup$
    I have updated the question now. Is it clearer in this phrasing?
    $endgroup$
    – LudvigH
    Mar 25 at 10:20










  • $begingroup$
    Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},pmatrix{a&1cr0&acr},pmatrix{a&-bcr b&a}$$ Each of those gives about as much insight as there is into the behavior of the dynamical system.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 10:40












  • $begingroup$
    That is just about the type of answer I hoped for. Write it as an answer and I'll accept it. :)
    $endgroup$
    – LudvigH
    Mar 25 at 11:14
















$begingroup$
I don't know what you mean by parametrization of a matrix, but, if the matrix is diagonalizable, then the recurrence can be rewritten in terms of the diagonal matrix (and the eigenvectors).
$endgroup$
– Gerry Myerson
Mar 25 at 9:53




$begingroup$
I don't know what you mean by parametrization of a matrix, but, if the matrix is diagonalizable, then the recurrence can be rewritten in terms of the diagonal matrix (and the eigenvectors).
$endgroup$
– Gerry Myerson
Mar 25 at 9:53












$begingroup$
I have updated the question now. Is it clearer in this phrasing?
$endgroup$
– LudvigH
Mar 25 at 10:20




$begingroup$
I have updated the question now. Is it clearer in this phrasing?
$endgroup$
– LudvigH
Mar 25 at 10:20












$begingroup$
Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},pmatrix{a&1cr0&acr},pmatrix{a&-bcr b&a}$$ Each of those gives about as much insight as there is into the behavior of the dynamical system.
$endgroup$
– Gerry Myerson
Mar 25 at 10:40






$begingroup$
Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},pmatrix{a&1cr0&acr},pmatrix{a&-bcr b&a}$$ Each of those gives about as much insight as there is into the behavior of the dynamical system.
$endgroup$
– Gerry Myerson
Mar 25 at 10:40














$begingroup$
That is just about the type of answer I hoped for. Write it as an answer and I'll accept it. :)
$endgroup$
– LudvigH
Mar 25 at 11:14




$begingroup$
That is just about the type of answer I hoped for. Write it as an answer and I'll accept it. :)
$endgroup$
– LudvigH
Mar 25 at 11:14










1 Answer
1






active

oldest

votes


















1












$begingroup$

Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},quadpmatrix{a&1cr0&acr},quadpmatrix{a&-bcr b&acr}$$ Each of those gives you about as much insight into the behavior of a dynamical system as you can get.






share|cite|improve this answer









$endgroup$













  • $begingroup$
    So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
    $endgroup$
    – LudvigH
    Mar 25 at 12:43






  • 1




    $begingroup$
    The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 21:58












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1 Answer
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active

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active

oldest

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active

oldest

votes









1












$begingroup$

Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},quadpmatrix{a&1cr0&acr},quadpmatrix{a&-bcr b&acr}$$ Each of those gives you about as much insight into the behavior of a dynamical system as you can get.






share|cite|improve this answer









$endgroup$













  • $begingroup$
    So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
    $endgroup$
    – LudvigH
    Mar 25 at 12:43






  • 1




    $begingroup$
    The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 21:58
















1












$begingroup$

Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},quadpmatrix{a&1cr0&acr},quadpmatrix{a&-bcr b&acr}$$ Each of those gives you about as much insight into the behavior of a dynamical system as you can get.






share|cite|improve this answer









$endgroup$













  • $begingroup$
    So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
    $endgroup$
    – LudvigH
    Mar 25 at 12:43






  • 1




    $begingroup$
    The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 21:58














1












1








1





$begingroup$

Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},quadpmatrix{a&1cr0&acr},quadpmatrix{a&-bcr b&acr}$$ Each of those gives you about as much insight into the behavior of a dynamical system as you can get.






share|cite|improve this answer









$endgroup$



Every $2times2$ real matrix is similar to a real matrix of exactly one of the following three forms: $$pmatrix{a&0cr0&bcr},quadpmatrix{a&1cr0&acr},quadpmatrix{a&-bcr b&acr}$$ Each of those gives you about as much insight into the behavior of a dynamical system as you can get.







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Mar 25 at 11:34









Gerry MyersonGerry Myerson

148k8152306




148k8152306












  • $begingroup$
    So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
    $endgroup$
    – LudvigH
    Mar 25 at 12:43






  • 1




    $begingroup$
    The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 21:58


















  • $begingroup$
    So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
    $endgroup$
    – LudvigH
    Mar 25 at 12:43






  • 1




    $begingroup$
    The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
    $endgroup$
    – Gerry Myerson
    Mar 25 at 21:58
















$begingroup$
So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
$endgroup$
– LudvigH
Mar 25 at 12:43




$begingroup$
So what do you call the three? Diagonal form, Jordan form and 'real jordan form' ?
$endgroup$
– LudvigH
Mar 25 at 12:43




1




1




$begingroup$
The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
$endgroup$
– Gerry Myerson
Mar 25 at 21:58




$begingroup$
The third one could be called real canonical form as at math.byu.edu/~grant/courses/m634/f99/lec11.pdf Diagonal form is just a special case of Jordan form.
$endgroup$
– Gerry Myerson
Mar 25 at 21:58


















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