Differential Equations Quiz: Systems Complex Eigenvalues
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Systems Complex EigenvaluesQuestion 1 of 4

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?

σ=ωθ\sigma = -\frac{\omega}{\theta}
σ=ωθ2π\sigma = -\frac{\omega \theta}{2\pi}
σ=ω2πθ\sigma = -\frac{\omega}{2\pi} \theta
σθ=ω\sigma \theta = -\omega
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Differential Equations Quiz

Differential Equations Quiz: Systems Complex Eigenvalues

Practice Systems Complex Eigenvalues in Differential Equations with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

What this quiz covers

This quiz focuses on Systems Complex Eigenvalues, giving you a quick way to practice the rules, question types, and explanations that matter most for Differential Equations.

How to use this quiz

Try each quiz question before looking at the correct answer. Use the explanations to review missed ideas, then come back to similar questions until the pattern feels familiar.

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Question 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?

  1. σ=ωθ\sigma = -\frac{\omega}{\theta} (correct answer)
  2. σ=ωθ2π\sigma = -\frac{\omega \theta}{2\pi}
  3. σ=ω2πθ\sigma = -\frac{\omega}{2\pi} \theta
  4. σθ=ω\sigma \theta = -\omega
Explanation: 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=e1e^{\sigma \theta/\omega} = \frac{1}{e} = e^{-1}. Therefore σθω=1\frac{\sigma \theta}{\omega} = -1, which gives σ=ωθ\sigma = -\frac{\omega}{\theta}.

Question 2

Consider the system (xy)=(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 adbc=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?

  1. a=0,d=0a = 0, d = 0, and bc=25bc = -25 with bb and cc having the same sign
  2. a=0,d=0a = 0, d = 0, and bc=25bc = -25 with bb and cc having opposite signs (correct answer)
  3. a=d0a = -d \neq 0, and the eigenvalues are ±5i\pm 5i
  4. a=d0a = -d \neq 0, and the eigenvalues are a±5ia \pm 5i
Explanation: 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)xy2ay2=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 adbc=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.

Question 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 tt^*. What is the xx-coordinate of this return point?

  1. e3π/2e^{3\pi/2}
  2. 2e3π/2\sqrt{2} e^{3\pi/2} (correct answer)
  3. e3π/4e^{3\pi/4}
  4. 2e3π/4\sqrt{2} e^{3\pi/4}
Explanation: 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 e3te^{3t^*}. The initial distance is 12+12=2\sqrt{1^2 + 1^2} = \sqrt{2}. Therefore, the xx-coordinate at return is 2e3π/2\sqrt{2} \cdot e^{3\pi/2}.

Question 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)=et(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 $$\Phi_2(t) = e^{-t}\begin{pmatrix} \cos(3t) & -\sin(3t) \ 2\cos(3t) + \sin(3t) & 2\sin(3t) + \cos(3t) \end{pmatrix}

  1. Both matrices are valid fundamental solutions since det(Φ1(0))=det(Φ2(0))=10\det(\Phi_1(0)) = \det(\Phi_2(0)) = -1 \neq 0
  2. Only Φ1(t)\Phi_1(t) can be valid since fundamental matrices must have det(Φ(0))>0\det(\Phi(0)) > 0
  3. Neither can be determined valid without verifying Φ(t)=AΦ(t)\Phi'(t) = A\Phi(t) and checking linear independence (correct answer)
  4. Only Φ2(t)\Phi_2(t) can be valid since the off-diagonal terms must have opposite signs for complex eigenvalues
Explanation: 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))=10\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.