Complex Eigenvalues & Real Solutions - Linear Algebra

  1. A 3×33 \times 3 real matrix AA must have at least one real eigenvalue. Which of the following sets could NOT be the complete set of eigenvalues for such a matrix AA?
    Answer: {5,1+2i,−1−2i}\{5, 1+2i, -1-2i\} The characteristic polynomial of a real n×nn \times n matrix has real coefficients. As a result, any complex roots (eigenvalues) must occur in conjugate pairs. That is, if a+bia+bi is an eigenvalue, then a−bia-bi must also be an eigenvalue. In choice D, the set contains the eigenvalue 1+2i1+2i. Its conjugate is 1−2i1-2i, which is not in the set. The value −1−2i-1-2i is the negative of 1+2i1+2i, not its conjugate. Therefore, this set cannot be the complete set of eigenvalues for a real matrix. The other sets are all valid: A has one real root and a conjugate pair, B has three real roots, and C has one real root (0) and a pure imaginary conjugate pair.
  2. Let AA be a real n×nn \times n matrix. If λ=5−2i\lambda = 5 - 2i is an eigenvalue of AA with a corresponding eigenvector v\mathbf{v}, which of the following statements is necessarily true?
    Answer: The matrix AA has an eigenvector vˉ\bar{\mathbf{v}} corresponding to the eigenvalue 5+2i5 + 2i. A fundamental theorem of linear algebra states that if a real matrix AA has a complex eigenvalue λ=a+bi\lambda = a+bi, then its complex conjugate λˉ=a−bi\bar{\lambda} = a-bi is also an eigenvalue. Furthermore, if v\mathbf{v} is an eigenvector for λ\lambda, then its complex conjugate vˉ\bar{\mathbf{v}} is an eigenvector for λˉ\bar{\lambda}. Given λ=5−2i\lambda = 5 - 2i, its conjugate is λˉ=5+2i\bar{\lambda} = 5 + 2i. Therefore, vˉ\bar{\mathbf{v}} must be an eigenvector corresponding to 5+2i5 + 2i. Choice A is incorrect; neither the real nor imaginary part of a complex eigenvector is generally an eigenvector itself. Choice C is incorrect; the real part of the eigenvalue is +5+5, which leads to solutions growing, not decaying. Choice D is incorrect; we only know of one eigenvector, so the geometric multiplicity is at least 1.
  3. Consider the linear system x′=Ax\mathbf{x}' = A\mathbf{x} where AA has eigenvalues λ1=1+2i\lambda_1 = 1 + 2i and λ2=1−2i\lambda_2 = 1 - 2i with corresponding eigenvector v1=(1i)\mathbf{v}_1 = \begin{pmatrix} 1 \\ i \end{pmatrix}. What is the general real solution to this system?
    Answer: x(t)=c1et(cos⁡(2t)−sin⁡(2t))+c2et(sin⁡(2t)cos⁡(2t))\mathbf{x}(t) = c_1 e^t \begin{pmatrix} \cos(2t) \\ -\sin(2t) \end{pmatrix} + c_2 e^t \begin{pmatrix} \sin(2t) \\ \cos(2t) \end{pmatrix} For complex eigenvalue λ=1+2i\lambda = 1 + 2i with eigenvector (1i)\begin{pmatrix} 1 \\ i \end{pmatrix}, we have eλtv1=e(1+2i)t(1i)=et(cos⁡(2t)+isin⁡(2t))(1i)=et(cos⁡(2t)+isin⁡(2t)icos⁡(2t)−sin⁡(2t))e^{\lambda t}\mathbf{v}_1 = e^{(1+2i)t}\begin{pmatrix} 1 \\ i \end{pmatrix} = e^t(\cos(2t) + i\sin(2t))\begin{pmatrix} 1 \\ i \end{pmatrix} = e^t\begin{pmatrix} \cos(2t) + i\sin(2t) \\ i\cos(2t) - \sin(2t) \end{pmatrix}. The real and imaginary parts give us the fundamental solutions: et(cos⁡(2t)−sin⁡(2t))e^t\begin{pmatrix} \cos(2t) \\ -\sin(2t) \end{pmatrix} and et(sin⁡(2t)cos⁡(2t))e^t\begin{pmatrix} \sin(2t) \\ \cos(2t) \end{pmatrix}. Choice B has wrong signs. Choice C has wrong exponential sign. Choice D misapplies the trigonometric decomposition.
  4. A real 2×22 \times 2 matrix AA has trace tr(A)=−4\text{tr}(A) = -4. For what range of values of the determinant, det⁡(A)\det(A), will solutions to the system x′=Ax\mathbf{x}'=A\mathbf{x} spiral into the origin (a spiral sink)?
    Answer: det⁡(A)>4\det(A) > 4 For a system to be a spiral sink, two conditions must be met. First, the eigenvalues must be complex conjugates, which means the discriminant of the characteristic equation must be negative: (tr(A))2−4det⁡(A)<0(\text{tr}(A))^2 - 4\det(A) < 0. Second, the real part of the eigenvalues must be negative. The real part of the eigenvalues is given by Re(λ)=tr(A)2\text{Re}(\lambda) = \frac{\text{tr}(A)}{2}. Given tr(A)=−4\text{tr}(A) = -4, the real part is −4/2=−2-4/2 = -2, which is negative. So the second condition is automatically satisfied. We only need to satisfy the first condition: (−4)2−4det⁡(A)<0(-4)^2 - 4\det(A) < 0, which simplifies to 16−4det⁡(A)<016 - 4\det(A) < 0. Adding 4det⁡(A)4\det(A) to both sides gives 16<4det⁡(A)16 < 4\det(A). Dividing by 4 yields det⁡(A)>4\det(A) > 4.
  5. Given that (1+2i3−i)\begin{pmatrix} 1 + 2i \\ 3 - i \end{pmatrix} is an eigenvector of real matrix CC corresponding to eigenvalue μ=2−i\mu = 2 - i, what is the trace of CC?
    Answer: 44 Since CC is real and has complex eigenvalue μ1=2−i\mu_1 = 2 - i, its complex conjugate μ2=2+i\mu_2 = 2 + i must also be an eigenvalue. For a 2×22 \times 2 real matrix with complex eigenvalues, the trace equals the sum of the eigenvalues: tr(C)=μ1+μ2=(2−i)+(2+i)=4\text{tr}(C) = \mu_1 + \mu_2 = (2 - i) + (2 + i) = 4. This follows from the fact that complex eigenvalues of real matrices come in conjugate pairs, and the trace is always real (sum of diagonal entries). Choices B, C, and D represent common errors in computing eigenvalue sums or incorrectly handling the complex parts.
  6. A real 2×22 \times 2 system x′=Ax\mathbf{x}'=A\mathbf{x} has a complex eigenvalue λ=4i\lambda=4i with eigenvector v=(12i)\mathbf{v}=\begin{pmatrix} 1 \\ 2i \end{pmatrix}. One real solution is x1(t)=(cos⁡(4t)−2sin⁡(4t))\mathbf{x}_1(t) = \begin{pmatrix} \cos(4t) \\ -2\sin(4t) \end{pmatrix}. Which of the following is a second, linearly independent real solution x2(t)\mathbf{x}_2(t)?
    Answer: (sin⁡(4t)2cos⁡(4t))\begin{pmatrix} \sin(4t) \\ 2\cos(4t) \end{pmatrix} The complex solution is z(t)=e4itv=(cos⁡(4t)+isin⁡(4t))((10)+i(02))\mathbf{z}(t) = e^{4it}\mathbf{v} = (\cos(4t)+i\sin(4t))(\begin{pmatrix} 1 \\ 0 \end{pmatrix} + i\begin{pmatrix} 0 \\ 2 \end{pmatrix}). Expanding this gives z(t)=[cos⁡(4t)(10)−sin⁡(4t)(02)]+i[sin⁡(4t)(10)+cos⁡(4t)(02)]\mathbf{z}(t) = [\cos(4t)\begin{pmatrix} 1 \\ 0 \end{pmatrix} - \sin(4t)\begin{pmatrix} 0 \\ 2 \end{pmatrix}] + i[\sin(4t)\begin{pmatrix} 1 \\ 0 \end{pmatrix} + \cos(4t)\begin{pmatrix} 0 \\ 2 \end{pmatrix}]. The real part is Re(z(t))=(cos⁡(4t)−2sin⁡(4t))\text{Re}(\mathbf{z}(t)) = \begin{pmatrix} \cos(4t) \\ -2\sin(4t) \end{pmatrix}, which is the given solution x1(t)\mathbf{x}_1(t). The imaginary part is Im(z(t))=(sin⁡(4t)2cos⁡(4t))\text{Im}(\mathbf{z}(t)) = \begin{pmatrix} \sin(4t) \\ 2\cos(4t) \end{pmatrix}, which is a second, linearly independent real solution x2(t)\mathbf{x}_2(t). Choice A is just −x1(t)-\mathbf{x}_1(t) and is not linearly independent. Choices C and D have sign errors.
  7. A real 2×22 \times 2 matrix AA has eigenvalues λ1=eiπ/3\lambda_1 = e^{i\pi/3} and λ2=e−iπ/3\lambda_2 = e^{-i\pi/3}. Which matrix is equal to A6A^6?
    Answer: The identity matrix, II. If a matrix AA has eigenvalues λ1,…,λn\lambda_1, \dots, \lambda_n, then the matrix AkA^k has eigenvalues λ1k,…,λnk\lambda_1^k, \dots, \lambda_n^k. The eigenvalues of A6A^6 are (λ1)6(\lambda_1)^6 and (λ2)6(\lambda_2)^6. Using de Moivre's formula, (λ1)6=(eiπ/3)6=ei(6π/3)=ei2π=cos⁡(2π)+isin⁡(2π)=1(\lambda_1)^6 = (e^{i\pi/3})^6 = e^{i(6\pi/3)} = e^{i2\pi} = \cos(2\pi) + i\sin(2\pi) = 1. Similarly, (λ2)6=(e−iπ/3)6=e−i2π=cos⁡(−2π)+isin⁡(−2π)=1(\lambda_2)^6 = (e^{-i\pi/3})^6 = e^{-i2\pi} = \cos(-2\pi) + i\sin(-2\pi) = 1. So, both eigenvalues of A6A^6 are 1. If AA is diagonalizable, A=PDP−1A = PDP^{-1}, then A6=PD6P−1A^6 = PD^6P^{-1}. Since D6=(1001)=ID^6 = \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix} = I, it follows that A6=PIP−1=IA^6 = PIP^{-1} = I. This holds even if AA is not diagonalizable. The only matrix with all eigenvalues equal to 1 that could result from this process is the identity matrix.
  8. The characteristic polynomial of a real 2×22 \times 2 matrix AA is p(λ)=λ2−2λ+10p(\lambda) = \lambda^2 - 2\lambda + 10. What is the long-term behavior of trajectories of the system x′=Ax\mathbf{x}' = A\mathbf{x} near the origin?
    Answer: Trajectories move away from the origin in a spiral pattern (spiral source). The eigenvalues of matrix AA are the roots of its characteristic polynomial. Using the quadratic formula, λ=−(−2)±(−2)2−4(1)(10)2(1)=2±4−402=2±−362=2±6i2=1±3i\lambda = \frac{-(-2) \pm \sqrt{(-2)^2 - 4(1)(10)}}{2(1)} = \frac{2 \pm \sqrt{4 - 40}}{2} = \frac{2 \pm \sqrt{-36}}{2} = \frac{2 \pm 6i}{2} = 1 \pm 3i. The eigenvalues are a complex conjugate pair λ=a±bi\lambda = a \pm bi with a=1a=1 and b=3b=3. Since b≠0b \neq 0, the trajectories involve rotation. Since the real part a=1a=1 is positive, the trajectories spiral away from the origin. This behavior is known as a spiral source.
  9. The phase portrait for a 2×22 \times 2 system x′=Ax\mathbf{x}' = A\mathbf{x} shows trajectories that are concentric ellipses centered at the origin. Which of the following conditions on the trace and determinant of AA must be true?
    Answer: tr(A)=0\text{tr}(A) = 0 and det⁡(A)>0\det(A) > 0 Trajectories that are concentric ellipses correspond to a center. This behavior occurs when the eigenvalues of the matrix AA are purely imaginary, i.e., λ=±bi\lambda = \pm bi for some real b≠0b \neq 0. The sum of the eigenvalues is the trace, so tr(A)=bi+(−bi)=0\text{tr}(A) = bi + (-bi) = 0. The product of the eigenvalues is the determinant, so det⁡(A)=(bi)(−bi)=−b2i2=b2\det(A) = (bi)(-bi) = -b^2i^2 = b^2. Since b≠0b \neq 0, the determinant must be positive. Thus, the conditions are tr(A)=0\text{tr}(A) = 0 and det⁡(A)>0\det(A) > 0.
  10. The general real solution to a 2×22 \times 2 linear system x′=Ax\mathbf{x}' = A\mathbf{x} is given by x(t)=c1e3t(cos⁡(4t)−2sin⁡(4t))+c2e3t(sin⁡(4t)2cos⁡(4t))\mathbf{x}(t) = c_1 e^{3t} \begin{pmatrix} \cos(4t) \\ -2\sin(4t) \end{pmatrix} + c_2 e^{3t} \begin{pmatrix} \sin(4t) \\ 2\cos(4t) \end{pmatrix}. What are the eigenvalues of the matrix AA?
    Answer: 3±4i3 \pm 4i The form of the real solutions to a system with complex eigenvalues λ=a±bi\lambda = a \pm bi is x(t)=eat(c1(…cos⁡(bt)… )+c2(…sin⁡(bt)… ))\mathbf{x}(t) = e^{at} (c_1 (\dots \cos(bt) \dots) + c_2 (\dots \sin(bt) \dots)). By inspecting the given solution, we can identify the exponential term e3te^{3t}, which implies the real part of the eigenvalue is a=3a=3. The trigonometric terms cos⁡(4t)\cos(4t) and sin⁡(4t)\sin(4t) imply the imaginary part of the eigenvalue is b=4b=4. Therefore, the eigenvalues of matrix AA are 3±4i3 \pm 4i.
  11. For a real 2×22 \times 2 matrix A=(abcd)A = \begin{pmatrix} a & b \\ c & d \end{pmatrix}, the system x′=Ax\mathbf{x}' = A\mathbf{x} has solutions that exhibit rotational behavior (either as a center or a spiral). This occurs if and only if the eigenvalues of AA are complex. Which of the following inequalities ensures this?
    Answer: (a+d)2−4(ad−bc)<0(a+d)^2 - 4(ad-bc) < 0 The eigenvalues of AA are the roots of the characteristic equation λ2−tr(A)λ+det⁡(A)=0\lambda^2 - \text{tr}(A)\lambda + \det(A) = 0. For a 2×22 \times 2 matrix, tr(A)=a+d\text{tr}(A) = a+d and det⁡(A)=ad−bc\det(A) = ad-bc. The eigenvalues are complex if and only if the discriminant of this quadratic equation is negative. The discriminant is B2−4AC=(−tr(A))2−4(1)(det⁡(A))=(a+d)2−4(ad−bc)B^2 - 4AC = (-\text{tr}(A))^2 - 4(1)(\det(A)) = (a+d)^2 - 4(ad-bc). Therefore, the condition for complex eigenvalues is (a+d)2−4(ad−bc)<0(a+d)^2 - 4(ad-bc) < 0.
  12. A 3×33 \times 3 real matrix has eigenvalues λ1=2\lambda_1 = 2, λ2=−1+3i\lambda_2 = -1 + 3i, and λ3=−1−3i\lambda_3 = -1 - 3i. If the matrix represents a dynamical system x′=Ax\mathbf{x}' = A\mathbf{x}, which statement best describes the long-term behavior of solutions?
    Answer: Solutions grow exponentially and oscillate due to the positive real eigenvalue dominating the complex eigenvalues The real eigenvalue λ1=2>0\lambda_1 = 2 > 0 dominates the complex eigenvalues λ2,3=−1±3i\lambda_{2,3} = -1 \pm 3i which have negative real part −1-1. Since 2>∣−1∣2 > |-1|, the positive real eigenvalue determines the long-term behavior. Solutions will grow exponentially in the direction of the eigenvector corresponding to λ1=2\lambda_1 = 2, while also exhibiting oscillatory behavior from the complex eigenvalues. Choice A incorrectly focuses on complex eigenvalues. Choice C is wrong because real parts are not zero. Choice D describes saddle points which occur when eigenvalues have mixed signs in purely real cases.
  13. The solution to a system x′=Ax\mathbf{x}' = A\mathbf{x} can be written as x(t)=eAtx(0)\mathbf{x}(t) = e^{At}\mathbf{x}(0). If one of the entries in the matrix eAte^{At} contains the term e5tsin⁡(2t)e^{5t}\sin(2t), what can be concluded about the eigenvalues of the real matrix AA?
    Answer: The eigenvalues of AA are a complex conjugate pair 5±2i5 \pm 2i. When you encounter a differential equation system x′=Ax\mathbf{x}' = A\mathbf{x} with solution x(t)=eAtx(0)\mathbf{x}(t) = e^{At}\mathbf{x}(0), the key insight is that the entries of the matrix exponential eAte^{At} directly reflect the eigenvalues of matrix AA. The term e5tsin⁡(2t)e^{5t}\sin(2t) tells us everything we need to know about the eigenvalues. This expression has the characteristic form that arises from complex eigenvalues: eαtsin⁡(βt)e^{\alpha t}\sin(\beta t), where α\alpha is the real part and β\beta is the imaginary part of the eigenvalue. Since we see e5tsin⁡(2t)e^{5t}\sin(2t), we can identify α=5\alpha = 5 and β=2\beta = 2, meaning the eigenvalues are 5±2i5 \pm 2i. Since AA is real, complex eigenvalues must occur in conjugate pairs. Looking at the wrong answers: Choice A incorrectly assumes the eigenvalues are real—but real eigenvalues produce exponential terms like e5te^{5t} and e2te^{2t}, never trigonometric functions. Choice B reverses the roles of the real and imaginary parts; 2±5i2 \pm 5i would generate e2tsin⁡(5t)e^{2t}\sin(5t) or e2tcos⁡(5t)e^{2t}\cos(5t) terms instead. Choice C suggests purely imaginary eigenvalues ±2i\pm 2i, which would produce terms like sin⁡(2t)\sin(2t) and cos⁡(2t)\cos(2t) without the exponential growth factor e5te^{5t}. The answer is D: the eigenvalues are 5±2i5 \pm 2i. Remember this pattern: in eAte^{At}, terms like eαtsin⁡(βt)e^{\alpha t}\sin(\beta t) always signal complex eigenvalues α±βi\alpha \pm \beta i.
  14. A real 2×22 \times 2 matrix AA has an eigenvalue λ=1−3i\lambda = 1 - 3i with eigenvector v=(2+i5)\mathbf{v} = \begin{pmatrix} 2+i \\ 5 \end{pmatrix}. Let u=Re(v)\mathbf{u} = \text{Re}(\mathbf{v}) and w=Im(v)\mathbf{w} = \text{Im}(\mathbf{v}). The set S=span{u,w}S = \text{span}\{\mathbf{u}, \mathbf{w}\} forms a plane in R2\mathbb{R}^2. What is the primary significance of this plane with respect to the matrix AA?
    Answer: The plane SS is an invariant subspace under the transformation AA. When you encounter complex eigenvalues of real matrices, you're working with a fundamental concept: real matrices with complex eigenvalues create rotational transformations, and certain real subspaces remain invariant under these transformations. Since AA is real but has complex eigenvalue λ=1−3i\lambda = 1 - 3i, its complex conjugate λˉ=1+3i\bar{\lambda} = 1 + 3i is also an eigenvalue. The key insight is that while the eigenvectors are complex, we can extract real vectors that span an invariant subspace. Given v=(2+i5)\mathbf{v} = \begin{pmatrix} 2+i \\ 5 \end{pmatrix}, we have u=Re(v)=(25)\mathbf{u} = \text{Re}(\mathbf{v}) = \begin{pmatrix} 2 \\ 5 \end{pmatrix} and w=Im(v)=(10)\mathbf{w} = \text{Im}(\mathbf{v}) = \begin{pmatrix} 1 \\ 0 \end{pmatrix}. The plane S=span{u,w}S = \text{span}\{\mathbf{u}, \mathbf{w}\} is invariant under AA, meaning AA maps any vector in SS to another vector in SS. This is answer D. Answer A is wrong because SS contains real vectors, but the actual eigenvectors are complex. Answer B is incorrect because A−IA - I would have eigenvalue −3i≠0-3i \neq 0, so its null space is trivial. Answer C misunderstands the geometry—both eigenspaces correspond to the same invariant plane when projected to real space. Study tip: For real matrices with complex eigenvalues, always remember that the real and imaginary parts of any complex eigenvector span a 2D invariant subspace. This pattern appears frequently in applications involving rotations and oscillations.
  15. Let AA be a real 2×22 \times 2 matrix. A complex eigenvalue and corresponding eigenvector for the system x′=Ax\mathbf{x}' = A\mathbf{x} are λ=−2+i\lambda = -2 + i and v=(11−i)\mathbf{v} = \begin{pmatrix} 1 \\ 1-i \end{pmatrix}. Which of the following is a valid real-valued solution x(t)\mathbf{x}(t) to the system?
    Answer: e−2t(cos⁡(t)(11)−sin⁡(t)(0−1))e^{-2t} \left( \cos(t)\begin{pmatrix} 1 \\ 1 \end{pmatrix} - \sin(t)\begin{pmatrix} 0 \\ -1 \end{pmatrix} \right) A complex solution is z(t)=eλtv\mathbf{z}(t) = e^{\lambda t}\mathbf{v}. The real and imaginary parts of z(t)\mathbf{z}(t) form two linearly independent real solutions. Let v=Re(v)+iIm(v)\mathbf{v} = \text{Re}(\mathbf{v}) + i\text{Im}(\mathbf{v}), where Re(v)=(11)\text{Re}(\mathbf{v}) = \begin{pmatrix} 1 \\ 1 \end{pmatrix} and Im(v)=(0−1)\text{Im}(\mathbf{v}) = \begin{pmatrix} 0 \\ -1 \end{pmatrix}. Using Euler's formula, e(−2+i)t=e−2t(cos⁡(t)+isin⁡(t))e^{(-2+i)t} = e^{-2t}(\cos(t) + i\sin(t)). Then z(t)=e−2t(cos⁡(t)+isin⁡(t))(Re(v)+iIm(v))\mathbf{z}(t) = e^{-2t}(\cos(t) + i\sin(t))(\text{Re}(\mathbf{v}) + i\text{Im}(\mathbf{v})). The real part of this expression is Re(z(t))=e−2t(cos⁡(t)Re(v)−sin⁡(t)Im(v))\text{Re}(\mathbf{z}(t)) = e^{-2t}(\cos(t)\text{Re}(\mathbf{v}) - \sin(t)\text{Im}(\mathbf{v})). Substituting the vectors gives the solution in choice A. Choice B has a sign error. Choice C incorrectly swaps the real and imaginary parts of λ\lambda. Choice D swaps the real and imaginary parts of v\mathbf{v}.

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