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Matrices & Determinants
Matrices and Determinants
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Question

Let A=[cosθ0sinθ010sinθ0cosθ]A=\left[\begin{array}{ccc}\cos \theta & 0 & -\sin \theta \\ 0 & 1 & 0 \\ \sin \theta & 0 & \cos \theta\end{array}\right]. If for some θ(0,π),A2=AT\theta \in(0, \pi), A^2=A^T, then the sum of the diagonal elements of the matrix (A+I)3+(AI)36 A(\mathrm{A}+\mathrm{I})^3+(\mathrm{A}-\mathrm{I})^3-6 \mathrm{~A} is equal to _________ .

Answer: 1

Solution

This problem combines concepts of special matrices, matrix algebra, and the trace of a matrix. Our goal is to simplify a complex matrix expression and then find the sum of its diagonal elements (trace), given a specific condition relating the matrix AA to its transpose.

1. Analyzing the Given Matrix AA and Identifying its Properties

The problem starts with a 3×33 \times 3 matrix AA: A=[cosθ0sinθ010sinθ0cosθ]A=\left[\begin{array}{ccc}\cos \theta & 0 & -\sin \theta \\ 0 & 1 & 0 \\ \sin \theta & 0 & \cos \theta\end{array}\right] This matrix is a well-known form of a rotation matrix around the y-axis by an angle θ\theta. Such matrices often possess special properties. Let's find its transpose, ATA^T: AT=[cosθ0sinθ010sinθ0cosθ]A^T=\left[\begin{array}{ccc}\cos \theta & 0 & \sin \theta \\ 0 & 1 & 0 \\ -\sin \theta & 0 & \cos \theta\end{array}\right] Now, let's compute the product AATAA^T. This is a crucial step to check for orthogonality: AAT=[cosθ0sinθ010sinθ0cosθ][cosθ0sinθ010sinθ0cosθ]AA^T = \left[\begin{array}{ccc}\cos \theta & 0 & -\sin \theta \\ 0 & 1 & 0 \\ \sin \theta & 0 & \cos \theta\end{array}\right] \left[\begin{array}{ccc}\cos \theta & 0 & \sin \theta \\ 0 & 1 & 0 \\ -\sin \theta & 0 & \cos \theta\end{array}\right] Multiplying these matrices: AAT=[(cos2θ+sin2θ)0(cosθsinθsinθcosθ)010(sinθcosθcosθsinθ)0(sin2θ+cos2θ)]AA^T = \left[\begin{array}{ccc} (\cos^2\theta + \sin^2\theta) & 0 & (\cos\theta\sin\theta - \sin\theta\cos\theta) \\ 0 & 1 & 0 \\ (\sin\theta\cos\theta - \cos\theta\sin\theta) & 0 & (\sin^2\theta + \cos^2\theta) \end{array}\right] Using the identity cos2θ+sin2θ=1\cos^2\theta + \sin^2\theta = 1: AAT=[100010001]=IAA^T = \left[\begin{array}{ccc} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end{array}\right] = I Where II is the 3×33 \times 3 identity matrix.

Explanation: A matrix AA is defined as an orthogonal matrix if AAT=ATA=IAA^T = A^T A = I. A key property of orthogonal matrices is that their transpose is equal to their inverse, i.e., AT=A1A^T = A^{-1}. Recognizing this property is fundamental as it allows us to relate ATA^T to A1A^{-1}, simplifying subsequent steps.

2. Utilizing the Given Condition A2=ATA^2 = A^T

We are given the condition A2=ATA^2 = A^T. From our analysis in Section 1, we established that AT=A1A^T = A^{-1} because AA is an orthogonal matrix. Substituting A1A^{-1} for ATA^T into the given condition: A2=A1A^2 = A^{-1} To eliminate the inverse and simplify this relationship, we can multiply both sides of the equation by AA. Since AA is invertible (as shown by AAT=IAA^T=I), we can multiply from either the left or the right. Let's multiply by AA from the right: A2A=A1AA^2 \cdot A = A^{-1} \cdot A A3=IA^3 = I

Explanation: The result A3=IA^3=I is a very powerful simplification. It means that the matrix AA is periodic with a period of 3. Any higher power of AA can be reduced based on this (e.g., A4=A,A5=A2A^4=A, A^5=A^2, etc.). This condition also tells us about the angle θ\theta. Since AA is a rotation matrix, An=[cosnθ0sinnθ010sinnθ0cosnθ]A^n = \left[\begin{array}{ccc}\cos n\theta & 0 & -\sin n\theta \\ 0 & 1 & 0 \\ \sin n\theta & 0 & \cos n\theta\end{array}\right]. So, A3=IA^3=I implies cos3θ=1\cos 3\theta = 1 and sin3θ=0\sin 3\theta = 0. For θ(0,π)\theta \in (0, \pi), this means 3θ=2π3\theta = 2\pi, so θ=2π/3\theta = 2\pi/3. This specific value of θ\theta ensures the condition A3=IA^3=I holds.

3. Simplifying the Target Matrix Expression

We need to find the sum of the diagonal elements (trace) of the matrix expression (A+I)3+(AI)36 A(\mathrm{A}+\mathrm{I})^3+(\mathrm{A}-\mathrm{I})^3-6 \mathrm{~A}. Let's first simplify the sum of the cubic terms: (A+I)3+(AI)3(\mathrm{A}+\mathrm{I})^3+(\mathrm{A}-\mathrm{I})^3. We can use the algebraic identity for real numbers: (x+y)3+(xy)3=(x3+3x2y+3xy2+y3)+(x33x2y+3xy2y3)=2x3+6xy2(x+y)^3 + (x-y)^3 = (x^3 + 3x^2y + 3xy^2 + y^3) + (x^3 - 3x^2y + 3xy^2 - y^3) = 2x^3 + 6xy^2.

Explanation: This identity can be directly applied to matrices AA and II because AA and II commute. That is, AI=IA=AAI = IA = A. Commutativity is essential for binomial expansions and standard algebraic identities to hold in matrix algebra. If AA and II did not commute, we would have to expand the terms carefully, preserving the order of multiplication.

Applying the identity with x=Ax=A and y=Iy=I: (A+I)3+(AI)3=2A3+6AI2(A+I)^3 + (A-I)^3 = 2A^3 + 6AI^2 Since I2=II=II^2 = I \cdot I = I (the identity matrix multiplied by itself is itself), the expression becomes: 2A3+6AI2A^3 + 6AI Also, multiplying any matrix by the identity matrix results in the same matrix, so AI=AAI = A. Thus, the expression simplifies to: 2A3+6A2A^3 + 6A Now, substitute this back into the full target expression: (A+I)3+(AI)36 A=(2A3+6A)6A(\mathrm{A}+\mathrm{I})^3+(\mathrm{A}-\mathrm{I})^3-6 \mathrm{~A} = (2A^3 + 6A) - 6A =2A3 = 2A^3 Finally, we use our crucial result from Section 2, A3=IA^3 = I: 2A3=2I2A^3 = 2I So, the entire complex matrix expression simplifies dramatically to 2I2I.

4. Calculating the Sum of Diagonal Elements (Trace)

We need to find the sum of the diagonal elements of the simplified expression, which is 2I2I. The trace of a matrix MM, denoted as Tr(M)\operatorname{Tr}(M), is the sum of its diagonal elements. For an n×nn \times n identity matrix InI_n, its diagonal elements are all 1s. Therefore, Tr(In)=n\operatorname{Tr}(I_n) = n. In this problem, II is a 3×33 \times 3 identity matrix, so its trace is Tr(I)=1+1+1=3\operatorname{Tr}(I) = 1+1+1 = 3.

We need to find Tr(2I)\operatorname{Tr}(2I). We use the property of the trace operator that for a scalar kk and a matrix MM, Tr(kM)=kTr(M)\operatorname{Tr}(kM) = k \operatorname{Tr}(M): Tr(2I)=2Tr(I)\operatorname{Tr}(2I) = 2 \operatorname{Tr}(I) Tr(2I)=2×3\operatorname{Tr}(2I) = 2 \times 3 Tr(2I)=6\operatorname{Tr}(2I) = 6

Therefore, the sum of the diagonal elements of the matrix (A+I)3+(AI)36 A(\mathrm{A}+\mathrm{I})^3+(\mathrm{A}-\mathrm{I})^3-6 \mathrm{~A} is 6\boxed{6}.

5. Important Tips and Common Pitfalls

  • Recognize Special Matrix Types: Always check if the given matrix possesses special properties like being orthogonal, symmetric, skew-symmetric, idempotent, or nilpotent. These properties often provide shortcuts (e.g., AT=A1A^T = A^{-1} for orthogonal matrices).
  • Matrix Algebra vs. Scalar Algebra: Be mindful that matrix multiplication is generally not commutative (ABBAAB \neq BA). However, the identity matrix II commutes with all matrices (AI=IA=AAI = IA = A). This commutativity is key to applying scalar algebraic identities like (x+y)3+(xy)3(x+y)^3+(x-y)^3 to matrix expressions involving II.
  • Properties of Trace: Remember the fundamental properties of the trace operator:
    • Tr(A+B)=Tr(A)+Tr(B)\operatorname{Tr}(A+B) = \operatorname{Tr}(A) + \operatorname{Tr}(B)
    • Tr(kA)=kTr(A)\operatorname{Tr}(kA) = k \operatorname{Tr}(A)
    • Tr(In)=n\operatorname{Tr}(I_n) = n (for an n×nn \times n identity matrix).
  • Invertibility: When manipulating equations involving inverses (e.g., A2=A1A^2=A^{-1} implying A3=IA^3=I), ensure the matrix is invertible. Orthogonal matrices are always invertible, with det(A)=±1\det(A) = \pm 1.

6. Summary and Key Takeaway

This problem is an excellent illustration of how to simplify complex matrix expressions by:

  1. Identifying special matrix properties: Recognizing AA as an orthogonal matrix (AAT=IAA^T = I) leads to AT=A1A^T = A^{-1}.
  2. Using given conditions to derive simpler matrix relationships: The condition A2=ATA^2 = A^T, combined with AT=A1A^T = A^{-1}, directly yields A3=IA^3 = I.
  3. Applying algebraic identities in matrix contexts: The algebraic identity for (X+Y)3+(XY)3(X+Y)^3+(X-Y)^3 is applicable due to the commutativity of AA and II.
  4. Calculating the trace: Finally, the properties of the trace operator allow for a straightforward calculation of the sum of diagonal elements.

By following these steps, the seemingly complicated expression reduces to a simple scalar multiple of the identity matrix, making the trace calculation trivial.

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