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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.

Question 1 / 4

0 of 4 answered

A system x′=Ax\mathbf{x}' = A\mathbf{x}x′=Ax has eigenvalues λ=σ±iω\lambda = \sigma \pm i\omegaλ=σ±iω where σ<0\sigma < 0σ<0 and ω>0\omega > 0ω>0. If the distance from any trajectory to the origin decreases by a factor of eee while the trajectory rotates through angle θ\thetaθ, what is the relationship between σ\sigmaσ, ω\omegaω, and θ\thetaθ?

Select an answer to continue

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.

All questions

Question 1

A system x′=Ax\mathbf{x}' = A\mathbf{x}x′=Ax has eigenvalues λ=σ±iω\lambda = \sigma \pm i\omegaλ=σ±iω where σ<0\sigma < 0σ<0 and ω>0\omega > 0ω>0. If the distance from any trajectory to the origin decreases by a factor of eee while the trajectory rotates through angle θ\thetaθ, what is the relationship between σ\sigmaσ, ω\omegaω, and θ\thetaθ?

  1. σ=−ωθ\sigma = -\frac{\omega}{\theta}σ=−θω​ (correct answer)
  2. σ=−ωθ2π\sigma = -\frac{\omega \theta}{2\pi}σ=−2πωθ​
  3. σ=−ω2πθ\sigma = -\frac{\omega}{2\pi} \thetaσ=−2πω​θ
  4. σθ=−ω\sigma \theta = -\omegaσθ=−ω

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))x(t)=eσt(ucos(ωt)+vsin(ωt)). The distance from origin is proportional to eσte^{\sigma t}eσt, and the angular displacement is ωt\omega tωt. If the trajectory rotates through angle θ\thetaθ, then ωt=θ\omega t = \thetaωt=θ, so t=θωt = \frac{\theta}{\omega}t=ωθ​. During this time, the distance changes by factor eσt=eσθ/ωe^{\sigma t} = e^{\sigma \theta/\omega}eσt=eσθ/ω. For the distance to decrease by factor eee (i.e., become 1e\frac{1}{e}e1​ times the original), we need eσθ/ω=1e=e−1e^{\sigma \theta/\omega} = \frac{1}{e} = e^{-1}eσθ/ω=e1​=e−1. Therefore σθω=−1\frac{\sigma \theta}{\omega} = -1ωσθ​=−1, which gives σ=−ωθ\sigma = -\frac{\omega}{\theta}σ=−θω​.

Question 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}(x′y′​)=(ac​bd​)(xy​) where a+d=0a + d = 0a+d=0 and ad−bc=25ad - bc = 25ad−bc=25. If the solution satisfying x(0)=3,y(0)=4x(0) = 3, y(0) = 4x(0)=3,y(0)=4 has the property that x2(t)+y2(t)x^2(t) + y^2(t)x2(t)+y2(t) is constant for all ttt, which of the following must be true about the coefficient matrix?

  1. a=0,d=0a = 0, d = 0a=0,d=0, and bc=−25bc = -25bc=−25 with bbb and ccc having the same sign
  2. a=0,d=0a = 0, d = 0a=0,d=0, and bc=−25bc = -25bc=−25 with bbb and ccc having opposite signs (correct answer)
  3. a=−d≠0a = -d \neq 0a=−d=0, and the eigenvalues are ±5i\pm 5i±5i
  4. a=−d≠0a = -d \neq 0a=−d=0, and the eigenvalues are a±5ia \pm 5ia±5i

Explanation: For x2(t)+y2(t)x^2(t) + y^2(t)x2(t)+y2(t) to be constant, we need ddt(x2+y2)=2xx′+2yy′=0\frac{d}{dt}(x^2 + y^2) = 2x x' + 2y y' = 0dtd​(x2+y2)=2xx′+2yy′=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 = 02x(ax+by)+2y(cx+dy)=2ax2+2(b+c)xy+2dy2=0. Since a+d=0a + d = 0a+d=0, we have d=−ad = -ad=−a, so 2ax2+2(b+c)xy−2ay2=02ax^2 + 2(b+c)xy - 2ay^2 = 02ax2+2(b+c)xy−2ay2=0. For this to hold for all x,yx, yx,y, we need a=0a = 0a=0 (so d=0d = 0d=0) and b+c=0b + c = 0b+c=0. With a=d=0a = d = 0a=d=0 and ad−bc=25ad - bc = 25ad−bc=25, we get −bc=25-bc = 25−bc=25, so bc=−25bc = -25bc=−25. Since b+c=0b + c = 0b+c=0, we have c=−bc = -bc=−b, so b(−b)=−b2=−25b(-b) = -b^2 = -25b(−b)=−b2=−25, giving b2=25b^2 = 25b2=25. Thus b=±5b = \pm 5b=±5 and c=∓5c = \mp 5c=∓5, meaning bbb and ccc have opposite signs.

Question 3

A system x′=Ax\mathbf{x}' = A\mathbf{x}x′=Ax has complex eigenvalues 3±4i3 \pm 4i3±4i. The trajectory starting at (1,1)(1, 1)(1,1) first returns to the positive xxx-axis (where y=0y = 0y=0 and x>0x > 0x>0) at time t∗t^*t∗. What is the xxx-coordinate of this return point?

  1. e3π/2e^{3\pi/2}e3π/2
  2. 2e3π/2\sqrt{2} e^{3\pi/2}2​e3π/2 (correct answer)
  3. e3π/4e^{3\pi/4}e3π/4
  4. 2e3π/4\sqrt{2} e^{3\pi/4}2​e3π/4

Explanation: The eigenvalues 3±4i3 \pm 4i3±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))x(t)=e3t(c1​ucos(4t)+c2​vsin(4t)) where u\mathbf{u}u and v\mathbf{v}v are the real and imaginary parts of an eigenvector. Starting at (1,1)(1,1)(1,1), the trajectory spirals outward. The trajectory returns to the positive xxx-axis when it has completed one revolution, which occurs when 4t=2π4t = 2\pi4t=2π, so t∗=π2t^* = \frac{\pi}{2}t∗=2π​. At this time, y=0y = 0y=0 and the xxx-coordinate is the initial distance from origin times e3t∗e^{3t^*}e3t∗. The initial distance is 12+12=2\sqrt{1^2 + 1^2} = \sqrt{2}12+12​=2​. Therefore, the xxx-coordinate at return is 2⋅e3π/2\sqrt{2} \cdot e^{3\pi/2}2​⋅e3π/2.

Question 4

For the system x′=Ax\mathbf{x}' = A\mathbf{x}x′=Ax where AAA has complex eigenvalues λ=−1±3i\lambda = -1 \pm 3iλ=−1±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}Φ1​(t)=e−t(cos(3t)2cos(3t)+sin(3t)​sin(3t)2sin(3t)−cos(3t)​). 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}Φ2​(t)=e−t(cos(3t)2cos(3t)+sin(3t)​−sin(3t)2sin(3t)+cos(3t)​). Which statement is most accurate?

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

Explanation: A fundamental matrix Φ(t)\Phi(t)Φ(t) must satisfy two conditions: (1) Φ′(t)=AΦ(t)\Phi'(t) = A\Phi(t)Φ′(t)=AΦ(t) and (2) det⁡(Φ(t))≠0\det(\Phi(t)) \neq 0det(Φ(t))=0 for all ttt. While both proposed matrices have det⁡(Φ(0))=−1≠0\det(\Phi(0)) = -1 \neq 0det(Φ(0))=−1=0, this alone doesn't guarantee they satisfy the differential equation. The specific form of the matrix AAA determines which solution is correct. We cannot conclude validity without explicitly checking that the derivative equals AAA 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.