Answers to Exercises for Chapter 4

Second-Order Linear Systems

  1. As two first-order differential equations, \( \ddot x + 4\dot x + 5 x=0 \) is $$ \dot x= y, \ \dot y = -4y -5x $$

  2. As a second-order differential equation for \(x\), $$\ddot x =2\dot x -3(6x-y)=\dot x-16x. $$ Similarly for \( y\), $$\ddot y = 6(2x-3y)-\dot y= \dot y -16y,$$ so we get the same second-order equation.

  3. For the system $$\dot x = x + 3 y, \ \dot y = 3x -7y,$$ the matrix form is $$M = \begin{pmatrix} 1 & 3\\ 3 & -7 \end{pmatrix}$$ with eigenvalues 2 and -8, eigenvectors \( (3, 1),\ (1,-3)\). These are orthogonal as expected because the matrix is symmetric. The general solution is $$x=3a e^{2t}+ be^{-8t},\ y=a e^{2t}-3be^{-8t}.$$ The specific solution for the initial conditions \(x(0)=10, \ y(0)=0\) is $$x=9 e^{2t} + e^{-8t},\ y=3 e^{2t}-3e^{-8t}.$$

    1. $$M=\begin{pmatrix} 1 & 2 \\ 3 & 4 \end{pmatrix}$$ \( T = 5, \ D=-2\), saddle.
    2. $$M=\begin{pmatrix} 2 & 1 \\ 3 & 4 \end{pmatrix}$$ \(T=6,\ D=5\), unstable node.
    3. $$M=\begin{pmatrix} 2 & 2 \\ -3 & -2 \end{pmatrix}$$ \(T=0,\ D= 2\), centre.
    4. $$M=\begin{pmatrix} 2 & 2 \\ -2 & -1 \end{pmatrix}$$ \(T=1, \ D=2\), unstable spiral.
    1. $$ M = \begin{pmatrix} 2 & -3 \\ 4 & -4\end{pmatrix} $$ Eigenvalues are \(-1\pm i \sqrt 3 \), no need for eigenvectors, stable spiral, solutions oscillate and approach the origin.
    2. $$ M = \begin{pmatrix} -1 & 1 \\ 6 & -2\end{pmatrix} $$ Eigenvalues 1, -4, so it's a saddle. Eigenvectors \( (1,2), \ (1,-3) \). Solutions tend to infinity in the direction of the vector (1,2).
    3. $$ M = \begin{pmatrix} -1 & 2\\ 2 & -4\end{pmatrix} $$ Eigenvalues are 0, with vector \( (2,1) \), and \( -5\) with vector \( (1,-2) \). There are fixed points all along the line \( y=x/2 \), and solutions tend to a point on this line, depending on the initial condition.
  4. For the third-order system $$\dot x = x + y - 4z, \ \dot y = - y, \ \dot z = 2x+3y -3z , $$ the \( y\) variable is uncoupled and decays to zero. That leaves a 2D system for \( x, \ z\) which is a stable spiral, so solutions spiral in to the origin in that plane.

  5. If \(M\) is idempotent, \(M^2=M\). Hence the exponential of the matrix is $$\exp(M)=I +M +M/2! + M/3! + \dots$$ which can be written (after adding and subtracting \( M\)) as $$\exp(M)= e M +I-M . $$ So for the matrix given in the question, first check that it is idempotent, then $$\exp(M)=\begin{pmatrix} e & 3e-3\\0 & 1 \end{pmatrix}.$$

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