Diff equation by diagonalization

  • Thread starter Thread starter EvLer
  • Start date Start date
  • Tags Tags
    Diagonalization
Join the discussion
Ask a follow-up here, or get your own question answered by working scientists, mathematicians and engineers — people, not an autocomplete.
Real named experts · corrections over time · the nuance an AI answer skips
6 replies · 3K views
EvLer
Messages
454
Reaction score
0

Homework Statement


solve initial value problem for the equation dx/dt = Ax where A =
[1 -1]
[0 1]
x(0) = [1, 1]T

x(t) = S*elambda*t*S -1*x(0)
where S is diagonal matrix, lambda is eigenvalue;

The Attempt at a Solution


I tried to diagonalize it, but I get one eigenvalue =1 mult 2 and I don't have enough eigenvectors to get S!
Am I missing something? and how do i solve it?

Thanks
 
on Phys.org
ok, so you are saying that A does not have to be diagonalizable for a solution to exist?

I am trying to see relations to the diagonalization
 
?? Every linear equation has solutions! Where did you get the idea that the matrix had to be diagonalizable?

Diagonalizable makes it easier but when a matrix is not diagonalizable you can still get the "Jordan Normal form".

The simplest way to solve this equation is two treat it as two equations:
dx/dt= x- y, dy/dt= y, since they are "partially disconnected": you can solve for y immediately: from dy/dt= y, y= Cet. Then the second equation becomes dx/dt= x- Cet or dx/dt- x= -Cet. That has integrating factor e-t: multiplying the equation by e-t give e-tdx/dt- e-tx= d(e-tx)/dt= e-t(Cet)= C. Integrating, e-tx= Ct+ D so x= Ctet+ Det. With x(0)= D= 1 and y(0)= C= 1, we have x(t)= tet+ et, y(t)= et.

Putting that back into matrix form that is x(t)= [tet+ et, et].
 
This is a linear equation of the form [itex]d\vec x/dt = \mathbf A \vec x[/itex]. If A and x were scalars, the solution would obviously be [itex]x=\exp(At)x(0)[/itex]. This is true for matrices as well:

[tex]\vec x \exp(\mathbf At) \vec x(0)[/tex]

where [itex]\exp(At)[/itex] is the matrix exponential

[tex]\exp(At) = \sum_{n=0}^\infty \frac{A^n t^n}{n!}[/tex]

Writing

[tex]\mathbf A = \mathbf 1_{2x2} - \mathbf B[/itex]<br /> <br /> where<br /> <br /> [tex]\mathbf 1_{2x2}[/tex] is the [itex]2x2[/itex] identity matrix and<br /> <br /> [tex]\mathbf B \equiv \bmatrix 0 & 1 \\ 0 & 0 \endbmatrix[/tex]<br /> <br /> Then<br /> <br /> [tex]\mathbf A^2 = \mathbf 1_{2x2} - 2\mathbf B[/tex]<br /> <br /> and in general<br /> <br /> [tex]\mathbf A^n = \mathbf 1_{2x2} - n\mathbf B[/tex]<br /> <br /> Thus<br /> <br /> [tex]\exp(At) =\mathbf 1_{2x2}\sum_{n=0}^\infty \frac{t^n}{n!} - \mathbf B \sum_{n=1}^\infty \frac{t^n}{(n-1)!}[/tex]<br /> <br /> Simplifying,<br /> <br /> [tex]\exp(At) =\mathbf 1_{2x2}\exp t - \mathbf B t\exp t[/tex]<br /> <br /> The desired solution is<br /> <br /> [tex]\vec x(t) =(\mathbf 1_{2x2}\exp t - \mathbf B t\exp t)\bmatrix 1 \\ 1\endbmatrix = \bmatrix 1-t\\1\endbmatrix \exp t[/tex][/tex]
 
HallsofIvy said:
The simplest way to solve this equation is two treat it as two equations:
dx/dt= x- y, dy/dt= y, since they are "partially disconnected": you can solve for y immediately: from dy/dt= y, y= Cet. Then the second equation becomes dx/dt= x- Cet or dx/dt- x= -Cet. That has integrating factor e-t: multiplying the equation by e-t give e-tdx/dt- e-tx= d(e-tx)/dt= e-t(Cet)= C.

There is a sign error here. That should be d(e-tx)/dt = -C

Integrating, e-tx= Ct+ D so x= Ctet+ Det. With x(0)= D= 1 and y(0)= C= 1, we have x(t)= tet+ et, y(t)= et.

Putting that back into matrix form that is x(t)= [tet+ et, et].

With the correct sign, integrating yields e-tx= D-Ct, so x= (D-Ct)et. With x(0)=y(0)=1, C=D=1, so x(t)= et-tet, y(t)= et. In matrix form,
[tex]\vec x(t) = \bmatrix e^t-te^t \\ e^t\endbmatrix[/tex]