What is the solution for a system of ODEs with a matrix coefficient?

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SUMMARY

The solution to the system of ordinary differential equations (ODEs) represented by \(\frac{d^2\vec{u}}{dt^2} = A\vec{u}\) can be approached using the characteristic equation \((A - \lambda^2 I)\vec{u}=\vec{0}\). This method parallels the solution of simpler ODEs, where the characteristic equation yields exponential solutions. The exponential of a matrix, denoted as \(e^{At}\), plays a crucial role in solving these systems, as it allows for the representation of the solution in terms of initial conditions. Understanding matrix exponentiation is essential for applying these concepts effectively.

PREREQUISITES
  • Matrix exponentiation, specifically \(e^{At}\)
  • Characteristic equations in differential equations
  • Basic concepts of linear algebra and eigenvalues
  • Understanding of systems of ordinary differential equations (ODEs)
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  • Study matrix exponentiation techniques and their applications in ODEs
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  • Explore the method of undetermined coefficients for solving linear ODEs
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Mathematicians, engineers, and students studying systems of ordinary differential equations, particularly those interested in advanced techniques for solving linear ODEs with matrix coefficients.

kostoglotov
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I know how to solve \frac{d\vec{u}}{dt} = A\vec{u}, I was just watching a lecture, and the lecturer related that solving that equation is pretty much a direct analogy to \vec{u} = e^{At}\vec{u}(0), in so far as all we need to do after that is understand exactly what it means to take the exponential of a matrix, which is fine...

My question is this, do I solve \frac{d^2\vec{u}}{dt^2} = A\vec{u} with \vec{u}=A^{-1}e^{At}\frac{d\vec{u}}{dt}(0)?

edit:

OR do I need to go along the lines

\frac{d^2\vec{u}}{dt^2} = \lambda^2\vec{u} = A\vec{u}

and solve

(A - \lambda^2 I)\vec{u}=\vec{0}

?
 
Last edited:
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One way to look at it: Introduce a new function v: \frac{d\vec{u}}{dt}= \vec{v}, \frac{d\vec{v}}{dt}=A\vec{u}.
 
kostoglotov said:
I know how to solve \frac{d\vec{u}}{dt} = A\vec{u}, I was just watching a lecture, and the lecturer related that solving that equation is pretty much a direct analogy to \vec{u} = e^{At}\vec{u}(0), in so far as all we need to do after that is understand exactly what it means to take the exponential of a matrix, which is fine...

My question is this, do I solve \frac{d^2\vec{u}}{dt^2} = A\vec{u} with \vec{u}=A^{-1}e^{At}\frac{d\vec{u}}{dt}(0)?

edit:

OR do I need to go along the lines

\frac{d^2\vec{u}}{dt^2} = \lambda^2\vec{u} = A\vec{u}

and solve

(A - \lambda^2 I)\vec{u}=\vec{0}

?
I haven't thought about this in quite a while.
If you had a regular ODE of the form u' = au, or u' - au = 0, the characteristic equation would be r - a = 0, so the solution would be u = Ceat, similar to your first order example above.

If you had u'' = λ2u, or u'' - λ2u = 0, the characteristic equation would be r2 - λ2 = 0, or r = ±λ. The solution would be u = C1eλt + C2e-λt.

Your example, with a system of ODEs, will have a solution that is analogous to the above, with exponentials involving the matrix.
 

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