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Matrices & Determinants
Matrices and Determinants
Medium

Question

If the matrix A = \left( {\matrix{ 0 & 2 \cr K & { - 1} \cr } } \right) satisfies A(A3+3I)=2IA({A^3} + 3I) = 2I, then the value of K is :

Options

Solution

Key Concept: The Cayley-Hamilton Theorem

The Cayley-Hamilton Theorem states that every square matrix satisfies its own characteristic equation. For a 2×22 \times 2 matrix AA, if its characteristic equation is λ2tr(A)λ+det(A)=0\lambda^2 - \text{tr}(A)\lambda + \det(A) = 0, then A2tr(A)A+det(A)I=0A^2 - \text{tr}(A)A + \det(A)I = 0, where tr(A)\text{tr}(A) is the trace of AA (sum of diagonal elements) and det(A)\det(A) is the determinant of AA. This theorem is crucial for simplifying matrix polynomial expressions.


Step-by-Step Solution

1. Analyze the Given Information and Simplify the Matrix Equation

We are given the matrix A = \left( {\matrix{ 0 & 2 \cr K & { - 1} \cr } } \right) and the matrix equation A(A3+3I)=2IA({A^3} + 3I) = 2I.

First, let's simplify the given matrix equation: A(A3+3I)=2IA({A^3} + 3I) = 2I Distribute AA on the left side: AA3+A(3I)=2IA \cdot A^3 + A \cdot (3I) = 2I A4+3(AI)=2IA^4 + 3(AI) = 2I Since AI=AAI = A (identity matrix multiplication property), we have: A4+3A=2IA^4 + 3A = 2I Now, isolate A4A^4: A4=2I3A()A^4 = 2I - 3A \quad (*) This equation provides a direct relationship between A4A^4 and AA, which we will use later to find KK.

2. Find the Characteristic Equation of Matrix A

To apply the Cayley-Hamilton Theorem, we first need to find the characteristic equation of matrix AA. The characteristic equation is given by det(AλI)=0\det(A - \lambda I) = 0, where λ\lambda is an eigenvalue and II is the identity matrix.

For A = \left( {\matrix{ 0 & 2 \cr K & { - 1} \cr } } \right), we have: A - \lambda I = \left( {\matrix{ 0 & 2 \cr K & { - 1} \cr } } \right) - \lambda \left( {\matrix{ 1 & 0 \cr 0 & 1 \cr } } \right) = \left( {\matrix{ {0 - \lambda} & 2 \cr K & {-1 - \lambda} \cr } } \right) Now, calculate the determinant: det(AλI)=(0λ)(1λ)(2)(K)=0\det(A - \lambda I) = (0 - \lambda)(-1 - \lambda) - (2)(K) = 0 (λ)((1+λ))2K=0(-\lambda)(-(1 + \lambda)) - 2K = 0 λ(1+λ)2K=0\lambda(1 + \lambda) - 2K = 0 λ+λ22K=0\lambda + \lambda^2 - 2K = 0 Rearranging in standard quadratic form: λ2+λ2K=0\lambda^2 + \lambda - 2K = 0 This is the characteristic equation of matrix AA.

3. Apply the Cayley-Hamilton Theorem

According to the Cayley-Hamilton Theorem, matrix AA satisfies its own characteristic equation. So, substitute AA for λ\lambda and II for the constant term: A2+A2KI=0A^2 + A - 2KI = 0 This equation is a fundamental property of matrix AA. We can express A2A^2 in terms of AA and II: A2=2KIA()A^2 = 2KI - A \quad (**) This expression for A2A^2 will be useful for simplifying higher powers of AA.

4. Express A4A^4 in terms of AA and II using the Cayley-Hamilton Relation

We have an expression for A2A^2. To get A4A^4, we can square A2A^2: A4=(A2)2A^4 = (A^2)^2 Substitute the expression for A2A^2 from ()(**): A4=(2KIA)2A^4 = (2KI - A)^2 Expand the square, remembering that matrix multiplication is not commutative in general, but II commutes with any matrix (IA=AI=AIA = AI = A), and scalar multiplication works as expected: (XY)2=X2XYYX+Y2(X - Y)^2 = X^2 - XY - YX + Y^2 Here X=2KIX = 2KI and Y=AY = A. (2KIA)2=(2KI)(2KI)(2KI)AA(2KI)+A2(2KI - A)^2 = (2KI)(2KI) - (2KI)A - A(2KI) + A^2 =4K2I22KIA2KIA+A2= 4K^2I^2 - 2KIA - 2KIA + A^2 Since I2=II^2 = I and IA=AIA = A: =4K2I2KA2KA+A2= 4K^2I - 2KA - 2KA + A^2 A4=4K2I4KA+A2A^4 = 4K^2I - 4KA + A^2 Now, substitute A2=2KIAA^2 = 2KI - A (from ()(**)) back into this equation to reduce the power of AA further: A4=4K2I4KA+(2KIA)A^4 = 4K^2I - 4KA + (2KI - A) Group terms with II and AA: A4=(4K2+2K)I(4K+1)A()A^4 = (4K^2 + 2K)I - (4K + 1)A \quad (***) Now we have an expression for A4A^4 solely in terms of AA, II, and KK.

5. Equate the Two Expressions for A4A^4 and Solve for K

We have two expressions for A4A^4:

  1. From the given equation (*): A4=2I3AA^4 = 2I - 3A
  2. From the Cayley-Hamilton Theorem (***): A4=(4K2+2K)I(4K+1)AA^4 = (4K^2 + 2K)I - (4K + 1)A

Equating these two expressions: 2I3A=(4K2+2K)I(4K+1)A2I - 3A = (4K^2 + 2K)I - (4K + 1)A Rearrange the terms to group II and AA matrices: 2I(4K2+2K)I=3A(4K+1)A2I - (4K^2 + 2K)I = 3A - (4K + 1)A [2(4K2+2K)]I=[3(4K+1)]A[2 - (4K^2 + 2K)]I = [3 - (4K + 1)]A (24K22K)I=(34K1)A(2 - 4K^2 - 2K)I = (3 - 4K - 1)A (22K4K2)I=(24K)A(2 - 2K - 4K^2)I = (2 - 4K)A Factor out common terms: 2(2K2+K1)I=2(12K)A-2(2K^2 + K - 1)I = 2(1 - 2K)A Divide both sides by 2: (2K2+K1)I=(12K)A-(2K^2 + K - 1)I = (1 - 2K)A Factor the quadratic expression 2K2+K12K^2 + K - 1: We look for two numbers that multiply to 2×(1)=22 \times (-1) = -2 and add to 11. These are 22 and 1-1. 2K2+2KK1=2K(K+1)1(K+1)=(2K1)(K+1)2K^2 + 2K - K - 1 = 2K(K+1) - 1(K+1) = (2K-1)(K+1) Substitute this back: (2K1)(K+1)I=(12K)A-(2K-1)(K+1)I = (1 - 2K)A Notice that (12K)=(2K1)(1 - 2K) = -(2K - 1). So we can write: (2K1)(K+1)I=(2K1)A-(2K-1)(K+1)I = -(2K - 1)A Move all terms to one side: (2K1)A(2K1)(K+1)I=0(2K-1)A - (2K-1)(K+1)I = 0 Factor out (2K1)(2K-1): (2K1)[A(K+1)I]=0(2K-1)[A - (K+1)I] = 0 For this equation to hold, one of the factors must be zero. Case 1: 2K1=02K - 1 = 0 This implies 2K=12K = 1, so K=12K = \frac{1}{2}.

Case 2: A(K+1)I=0A - (K+1)I = 0 This would mean A=(K+1)IA = (K+1)I. If A = \left( {\matrix{ 0 & 2 \cr K & { - 1} \cr } } \right) were equal to (K+1)I = \left( {\matrix{ K+1 & 0 \cr 0 & {K+1} \cr } } \right), then comparing the elements: 0=K+1K=10 = K+1 \Rightarrow K = -1 2=02 = 0 (This is a contradiction!) This means that AA cannot be a scalar multiple of the identity matrix. Therefore, the second factor A(K+1)IA - (K+1)I cannot be the zero matrix.

Since A(K+1)I0A - (K+1)I \neq 0, the only possibility is that the first factor is zero. 2K1=0K=122K - 1 = 0 \Rightarrow K = \frac{1}{2}.

6. Verify with Options

The calculated value K=12K = \frac{1}{2} matches option (A).


Tips and Common Mistakes:

  • Matrix Algebra: Always remember that matrix multiplication is generally not commutative (ABBAAB \neq BA). However, the identity matrix II commutes with any matrix (AI=IA=AAI = IA = A). Also, scalar multiplication works just like with numbers, e.g., (cM)2=c2M2(cM)^2 = c^2M^2.
  • Cayley-Hamilton Theorem: This theorem is a powerful tool for simplifying matrix polynomials. It allows you to reduce any power of a matrix AA to a linear combination of lower powers of AA (down to An1A^{n-1} for an n×nn \times n matrix) and the identity matrix II.
  • Factoring: When you reach an equation like (2K1)[A(K+1)I]=0(2K-1)[A - (K+1)I] = 0, it's crucial to analyze both factors. Don't immediately assume the scalar factor is the only one that can be zero. However, in matrix equations, if MN=0M \cdot N = \mathbf{0} (zero matrix), it doesn't necessarily mean M=0M = \mathbf{0} or N=0N = \mathbf{0}. But if one factor is a scalar, say cM=0c \cdot M = \mathbf{0} where MM is a non-zero matrix, then the scalar cc must be zero. In our case, A(K+1)IA - (K+1)I is a matrix, and if it's not the zero matrix, then the scalar factor (2K1)(2K-1) must be zero.
  • Careful Substitution: Be meticulous when substituting matrix expressions, especially when squaring or multiplying. A small error can propagate through the entire solution.

Summary and Key Takeaway:

This problem demonstrates an effective application of the Cayley-Hamilton Theorem. By first simplifying the given matrix equation and then using the characteristic equation to find a polynomial relation for AA (via Cayley-Hamilton), we can express higher powers of AA in terms of AA and II. Equating these expressions leads to a simpler equation involving AA, II, and the unknown KK. By comparing coefficients of AA and II (or by careful factorization), we can solve for KK. The ability to reduce

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