Systems: Complex Eigenvalues - Differential Equations

  1. A system x′=Ax\mathbf{x}' = A\mathbf{x} has eigenvalues λ=σ±iω\lambda = \sigma \pm i\omega where σ<0\sigma < 0 and ω>0\omega > 0. If the distance from any trajectory to the origin decreases by a factor of ee while the trajectory rotates through angle θ\theta, what is the relationship between σ\sigma, ω\omega, and θ\theta?
    Answer: σ=−ωθ\sigma = -\frac{\omega}{\theta} The solution has form x(t)=eσt(ucos⁡(ωt)+vsin⁡(ωt))\mathbf{x}(t) = e^{\sigma t}(\mathbf{u}\cos(\omega t) + \mathbf{v}\sin(\omega t)). The distance from origin is proportional to eσte^{\sigma t}, and the angular displacement is ωt\omega t. If the trajectory rotates through angle θ\theta, then ωt=θ\omega t = \theta, so t=θωt = \frac{\theta}{\omega}. During this time, the distance changes by factor eσt=eσθ/ωe^{\sigma t} = e^{\sigma \theta/\omega}. For the distance to decrease by factor ee (i.e., become 1e\frac{1}{e} times the original), we need eσθ/ω=1e=e−1e^{\sigma \theta/\omega} = \frac{1}{e} = e^{-1}. Therefore σθω=−1\frac{\sigma \theta}{\omega} = -1, which gives σ=−ωθ\sigma = -\frac{\omega}{\theta}.
  2. Consider the system (x′y′)=(abcd)(xy)\begin{pmatrix} x' \\ y' \end{pmatrix} = \begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} where a+d=0a + d = 0 and ad−bc=25ad - bc = 25. If the solution satisfying x(0)=3,y(0)=4x(0) = 3, y(0) = 4 has the property that x2(t)+y2(t)x^2(t) + y^2(t) is constant for all tt, which of the following must be true about the coefficient matrix?
    Answer: a=0,d=0a = 0, d = 0, and bc=−25bc = -25 with bb and cc having opposite signs For x2(t)+y2(t)x^2(t) + y^2(t) to be constant, we need ddt(x2+y2)=2xx′+2yy′=0\frac{d}{dt}(x^2 + y^2) = 2x x' + 2y y' = 0 for all solutions. Substituting the system: 2x(ax+by)+2y(cx+dy)=2ax2+2(b+c)xy+2dy2=02x(ax + by) + 2y(cx + dy) = 2ax^2 + 2(b+c)xy + 2dy^2 = 0. Since a+d=0a + d = 0, we have d=−ad = -a, so 2ax2+2(b+c)xy−2ay2=02ax^2 + 2(b+c)xy - 2ay^2 = 0. For this to hold for all x,yx, y, we need a=0a = 0 (so d=0d = 0) and b+c=0b + c = 0. With a=d=0a = d = 0 and ad−bc=25ad - bc = 25, we get −bc=25-bc = 25, so bc=−25bc = -25. Since b+c=0b + c = 0, we have c=−bc = -b, so b(−b)=−b2=−25b(-b) = -b^2 = -25, giving b2=25b^2 = 25. Thus b=±5b = \pm 5 and c=∓5c = \mp 5, meaning bb and cc have opposite signs.
  3. A system x′=Ax\mathbf{x}' = A\mathbf{x} has complex eigenvalues 3±4i3 \pm 4i. The trajectory starting at (1,1)(1, 1) first returns to the positive xx-axis (where y=0y = 0 and x>0x > 0) at time t∗t^*. What is the xx-coordinate of this return point?
    Answer: 2e3π/2\sqrt{2} e^{3\pi/2} The eigenvalues 3±4i3 \pm 4i give solutions of the form x(t)=e3t(c1ucos⁡(4t)+c2vsin⁡(4t))\mathbf{x}(t) = e^{3t}(c_1\mathbf{u}\cos(4t) + c_2\mathbf{v}\sin(4t)) where u\mathbf{u} and v\mathbf{v} are the real and imaginary parts of an eigenvector. Starting at (1,1)(1,1), the trajectory spirals outward. The trajectory returns to the positive xx-axis when it has completed one revolution, which occurs when 4t=2π4t = 2\pi, so t∗=π2t^* = \frac{\pi}{2}. At this time, y=0y = 0 and the xx-coordinate is the initial distance from origin times e3t∗e^{3t^*}. The initial distance is 12+12=2\sqrt{1^2 + 1^2} = \sqrt{2}. Therefore, the xx-coordinate at return is 2⋅e3π/2\sqrt{2} \cdot e^{3\pi/2}.
  4. For the system x′=Ax\mathbf{x}' = A\mathbf{x} where AA has complex eigenvalues λ=−1±3i\lambda = -1 \pm 3i, two students propose different fundamental matrix solutions. Student 1 claims Φ1(t)=e−t(cos⁡(3t)sin⁡(3t)2cos⁡(3t)+sin⁡(3t)2sin⁡(3t)−cos⁡(3t))\Phi_1(t) = e^{-t}\begin{pmatrix} \cos(3t) & \sin(3t) \\ 2\cos(3t) + \sin(3t) & 2\sin(3t) - \cos(3t) \end{pmatrix}. Student 2 claims Φ2(t)=e−t(cos⁡(3t)−sin⁡(3t)2cos⁡(3t)+sin⁡(3t)2sin⁡(3t)+cos⁡(3t))\Phi_2(t) = e^{-t}\begin{pmatrix} \cos(3t) & -\sin(3t) \\ 2\cos(3t) + \sin(3t) & 2\sin(3t) + \cos(3t) \end{pmatrix}. Which statement is most accurate?
    Answer: Neither can be determined valid without verifying Φ′(t)=AΦ(t)\Phi'(t) = A\Phi(t) and checking linear independence A fundamental matrix Φ(t)\Phi(t) must satisfy two conditions: (1) Φ′(t)=AΦ(t)\Phi'(t) = A\Phi(t) and (2) det⁡(Φ(t))≠0\det(\Phi(t)) \neq 0 for all tt. While both proposed matrices have det⁡(Φ(0))=−1≠0\det(\Phi(0)) = -1 \neq 0, this alone doesn't guarantee they satisfy the differential equation. The specific form of the matrix AA determines which solution is correct. We cannot conclude validity without explicitly checking that the derivative equals AA times the matrix. The sign of the determinant and patterns in off-diagonal terms don't determine validity by themselves - only the fundamental differential equation relationship matters.

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