Elliptic, Parabolic, and Hyperbolic PDEs

In summary, the conversation discusses the use of symbols in second-order partial differential equations (PDEs) and how they can be manipulated to characterize the behavior of solutions. The given equation, ##\sigma(\xi) = \xi^t A \xi##, is modified by replacing ##\xi_i\xi_j## with ##\partial_i\partial_ju##, giving ##a_{11}\partial_x^2+2a_{12}\partial_x\partial_yu+a_{22}\partial_y^2##. The trace and determinant of the matrix A do not provide enough information about the eigenvalues, but matrix diagonalization can be used to express A as a diagonal matrix with the eigenvalues
  • #1
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Homework Statement
Discover the classification of linear second order PDE yourself.
Relevant Equations
Please see below
Screen Shot 2021-01-16 at 2.06.58 AM.png


(1) ok.

(2) We start with ##\sigma(ξ) = a_{11} ξ_1^2 +2a_{12}ξ_1ξ_2 +a_{22}ξ_2^2ξ##
and we replace every ##ξ_iξ_j## with ##\partial_i\partial_ju##,
giving ##a_{11}\partial_x^2+2a_{12}\partial_x\partial_yu+1_{22}\partial_2^2##

(3) The given equation is the following.
##\sigma(ξ) = ξ^t A ξ ##
we take the product.
##\sigma(ξ) = \begin{pmatrix} ξ_1^t & ξ_2^t \end{pmatrix} \begin{pmatrix} a_{11} & 1_{12} \\ a_{21} & a_{22} \end{pmatrix} \begin{pmatrix} ξ_1 \\ ξ_2 \end{pmatrix} ##
giving
##\sigma(ξ) = a_{11}ξ_1^{t+1} +2a_{12}ξ_1ξ_2+a_{22}ξ_2^{t+1}##
which is different from the symbol given in part (2)
##\sigma(ξ) = a_{11} ξ_1^2 +2a_{12}ξ_1ξ_2 +a_{22}ξ_2^2ξ##
what is the ##t## used for, is this not a typo?

(4) The trace is the sum of the eigenvalues ##a_{11}+a_{22}##. knowing the the trace does not tell us anything about the eigenvalues. the determinant is given by ##det(A) = a_{11}a_{22}-(a_{12})^2 ##, which does not tell us ##a_{11}, a_{22}##. we have two equations and three unknowns, so we cannot use the trace and determinant for characterization.

(5) we could use matrix diagonalization (change of coordinates) to express ##A## as some matrix whose diagonal entries are ##a_{11}, a_{22}##. Doing this would cancel out the crossterm ##2a_{12}ξ_1ξ_2##. so
(a) ##\sigma(η) = \sigma(ξ) - 2a_{12}ξ_1ξ_2##
(b) ##\sigma(η) = \sigma(ξ) - a_{11} ξ_1^2-2a_{12}ξ_1ξ_2##
(c) ##\sigma(η) = \sigma(ξ) - 2a_{11} ξ_1^2-2a_{12}ξ_1ξ_2##
I definitely need to think more about this problem, but I value any suggestions.

(6) The highest order terms of the symbol controls the qualitative behavior of the solutions of PDEs, so we could use the symbols of every second order PDE by ignoring the lower order terms for a close approximation. And manipulate the symbols to fit the three cases by a change of coordinates.

(7) If we have non-constant coefficients, could we use the same procedure as before, but instead the eigenvalues will be functions, and not numbers?

(8) For higher dimensions, could we define elliptic, parabolic, and hyperbolic PDEs in just two variables and keep the other variables undisturbed?
 
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3) I am not sure but I think the symbol t is not an exponent but it denotes the transpose of the vector ##\xi##. So if ##\xi=\begin{pmatrix}\xi_1 & \xi_2\end{pmatrix}## is the vector (single raw) its transpose ##\xi^T=\begin{pmatrix}\xi_1\\ \xi_2\end{pmatrix}## or the other way around if we have a single column its transpose is a single raw.
8) I think the problem setter means that we have to incorporate all the derivatives ##\partial_i\partial_j## where ##i,j## now range from ##1## to ##n##. I think the matrix A will be ##n\times n## instead of ##2\times 2## and ##\xi=\begin{pmatrix}\xi_1&\xi_2&...&\xi_n\end{pmatrix}##.
 
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  • #3
4) The eigenvalues [itex]\sigma[/itex] are found by solving [itex]\det (A - \sigma I) = 0[/itex], which for a 2x2 matrix is [tex](a_{11} - \sigma)(a_{22} - \sigma) - a_{12}a_{21} = 0.[/tex] Expand this. What is the coefficient of [itex]\sigma[/itex]? What is the constant term? What conditions must these coefficients satisfy for the roots to be of the same sign, or of opposite sign, or for there to be a zero root?
 
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  • #4
Delta2 said:
3) I am not sure but I think the symbol t is not an exponent but it denotes the transpose of the vector ##\xi##. So if ##\xi=\begin{pmatrix}\xi_1 & \xi_2\end{pmatrix}## is the vector (single raw) its transpose ##\xi^T=\begin{pmatrix}\xi_1\\ \xi_2\end{pmatrix}## or the other way around if we have a single column its transpose is a single raw.
8) I think the problem setter means that we have to incorporate all the derivatives ##\partial_i\partial_j## where ##i,j## now range from ##1## to ##n##. I think the matrix A will be ##n\times n## instead of ##2\times 2## and ##\xi=\begin{pmatrix}\xi_1&\xi_2&...&\xi_n\end{pmatrix}##.
of course, how silly of me to assume ##t## is an exponent. Realizing this mistake, the correct solution is
##\sigma(ξ) = \begin{pmatrix} ξ_1 & ξ_2\end{pmatrix} \begin{pmatrix} a_{11} & 1_{12} \\ a_{21} & a_{22} \end{pmatrix} \begin{pmatrix} ξ_1 \\ ξ_2 \end{pmatrix} = a_{11} ξ_1^2 +2a_{12}ξ_1ξ_2 +a_{22}ξ_2^2ξ##

For (8) I was thinking that too. it seems like I will need to learn how to characterize a ##n×n## matrix as parabolic, elliptical, or hyperbolic when ##n>2##. I am asking for more time to work this out.

pasmith said:
4) The eigenvalues [itex]\sigma[/itex] are found by solving [itex]\det (A - \sigma I) = 0[/itex], which for a 2x2 matrix is [tex](a_{11} - \sigma)(a_{22} - \sigma) - a_{12}a_{21} = 0.[/tex] Expand this. What is the coefficient of [itex]\sigma[/itex]? What is the constant term? What conditions must these coefficients satisfy for the roots to be of the same sign, or of opposite sign, or for there to be a zero root?
Of course, I mistakenly thought the eigenvalues of a symmetric matrix are its diagonal entries.
To compute the eigenvalues ##\lambda## (to avoid getting confused with the other ##\sigma##s) we solve the characteristic polynomial of ##A##.
##(a_{11} - \lambda)(a_{22} - \lambda) - (a_{12})^2 + \lambda^2= 0##
##a_{11}a_{22}-(a_{12})^2-(a_{11}+a_{22})\lambda+\lambda^2=0##
the coefficient of ##\lambda## is ##-(a_{11}+a_{22})## and the constant term is ##a_{11}a_{22}-(a_{12})^2##.

The roots are equal when the discriminant is 0
##(a_{11}+a_{22})^2 -4(a_{11}a_{22}-(a_{12})^2)=0##.
##(a_{11}+a_{22})^2-4a_{11}a_{22}+4(a_{12})^2=0##
##(a_{11})^2+2a_{11}a_{22}+(a_{22})^2-4a_{11}a_{22}+4(a_{12})^2=0##
##(a_{11})^2-2a_{11}a_{22}+(a_{22})^2+4(a_{12})^2=0##
##(a_{11}-a_{22})^2+4(a_{12})^2=0##
which is an expression that seems unrelated to the determinant of ##A## and its trace. this does not help us.

By Sylvester's criterion, the eigenvalues are same sign if the matrix is positive definite or negative definite.
for positive definite, the leading principal minors must be positive.
##a_{11}>0##
##a_{11}a_{22}-(a_{12})^2>0##
And for negative definite
##a_{11}<0##
##a_{11}a_{22}-(a_{12})^2>0##

The eigenvalues are opposite signs if ##A## is indefinite. This is when an even leading principal minor is negative.
##a_{11}a_{22}-(a_{12})^2<0##

there are no real roots when the discriminant is less than 0
##(a_{11}+a_{22})^2 -4(a_{11}a_{22}-(a_{12})^2)<0##
##(a_{11}-a_{22})^2+4(a_{12})^2<0##I think for this problem we assume the determinant and trace of ##A## are known, and not its entries. So this may be unneccessary. But I could be wrong.
 
  • #5
Oh, I just caught my mistake. If the determinant of ##A## is negative, the eigenvalues are opposite signs and the PDE is hyperbolic. If the square of the trace is less than 4 times the determinant, there are no real roots. If the determinant is positive, the eigenvalues are the same signs and our PDE is elliptic. Thank you @pasmith
 
  • #6
So what about the parabolic case when one eigenvalues is 0? The professor said he would grade us on effort and give 100% credit if we try. I am looking to solve most of this problem though because it is valuable learning.
 
  • #7
For (5) i found the following information made available by UMI. It turns out a change of variables is a more involved process than I initially thought.

http://faculty.uml.edu/spennell/Teaching/PDE/classification.pdf

I cannot even begin to answer question (8) until I have figured out (5) and (6), so maybe this problem will not be finished. It seems like a lot to learn for a 1st week PDE classs assignment.
 
  • #8
For 8) I think
  • if all the eigenvalues of the ##n\times n## matrix are of the same sign (some of which might be zero) then it is elliptic
  • if all are zero (except one) then it is parabolic
  • if some are positive and some are negative (while some might be zero) then it is hyperbolic
 
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FAQ: Elliptic, Parabolic, and Hyperbolic PDEs

1. What is the difference between an elliptic, parabolic, and hyperbolic PDE?

Elliptic, parabolic, and hyperbolic PDEs are types of partial differential equations that describe different types of physical systems. The main difference between them lies in the behavior of their solutions. Elliptic PDEs have solutions that are smooth and continuous, while parabolic PDEs have solutions that change smoothly over time. Hyperbolic PDEs have solutions that exhibit wave-like behavior.

2. What are some real-world applications of elliptic, parabolic, and hyperbolic PDEs?

Elliptic PDEs are commonly used to model steady-state systems, such as heat conduction or electrostatics. Parabolic PDEs are used to model diffusion processes, such as heat transfer or chemical reactions. Hyperbolic PDEs are often used to model wave phenomena, such as sound or electromagnetic waves.

3. How do you solve an elliptic, parabolic, or hyperbolic PDE?

The method for solving a PDE depends on its type and specific form. Elliptic PDEs are typically solved using numerical methods, such as finite differences or finite elements. Parabolic PDEs can also be solved numerically, but they can also be solved using separation of variables or the method of characteristics. Hyperbolic PDEs are usually solved using the method of characteristics or finite difference methods.

4. Can elliptic, parabolic, and hyperbolic PDEs be coupled together?

Yes, it is possible for different types of PDEs to be coupled together in a single system. For example, a parabolic PDE describing heat transfer may be coupled with an elliptic PDE describing fluid flow. These coupled systems can be solved using numerical methods or by breaking them down into smaller, simpler problems that can be solved individually.

5. How do elliptic, parabolic, and hyperbolic PDEs relate to each other?

Elliptic, parabolic, and hyperbolic PDEs are all types of partial differential equations, but they have distinct characteristics and behaviors. Elliptic PDEs are often seen as the "opposite" of hyperbolic PDEs, as their solutions are smooth and continuous while hyperbolic solutions exhibit wave-like behavior. Parabolic PDEs can be seen as a bridge between the two, as their solutions change smoothly over time but do not exhibit wave behavior.

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