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JEE Main 2022
Matrices & Determinants
Matrices and Determinants
Medium

Question

Let S={mZ:Am2+Am=3IA6}S=\left\{m \in \mathbf{Z}: A^{m^2}+A^m=3 I-A^{-6}\right\}, where A=[2110]A=\left[\begin{array}{cc}2 & -1 \\ 1 & 0\end{array}\right]. Then n(S)n(S) is equal to __________.

Answer: 2

Solution

1. Core Concept: The Cayley-Hamilton Theorem and Matrix Powers

The problem involves powers of a 2×22 \times 2 matrix AA. For such matrices, the Cayley-Hamilton Theorem is an extremely powerful tool. It states that every square matrix satisfies its own characteristic equation. This theorem allows us to express higher powers of a matrix in terms of lower powers, often leading to a simple general form for AnA^n.

Given the matrix A=[2110]A = \begin{bmatrix} 2 & -1 \\ 1 & 0 \end{bmatrix}.

First, we find the characteristic equation of AA. The characteristic equation is given by det(AλI)=0\det(A - \lambda I) = 0, where II is the identity matrix and λ\lambda represents the eigenvalues.

det([2110]λ[1001])=0\det \left( \begin{bmatrix} 2 & -1 \\ 1 & 0 \end{bmatrix} - \lambda \begin{bmatrix} 1 & 0 \\ 0 & 1 \end{bmatrix} \right) = 0 det([2λ11λ])=0\det \left( \begin{bmatrix} 2-\lambda & -1 \\ 1 & -\lambda \end{bmatrix} \right) = 0 (2λ)(λ)(1)(1)=0(2-\lambda)(-\lambda) - (-1)(1) = 0 2λ+λ2+1=0-2\lambda + \lambda^2 + 1 = 0 λ22λ+1=0\lambda^2 - 2\lambda + 1 = 0 This is (λ1)2=0(\lambda-1)^2 = 0, meaning λ=1\lambda=1 is an eigenvalue with algebraic multiplicity 2.

By the Cayley-Hamilton Theorem, the matrix AA must satisfy this equation: A22A+I=OA^2 - 2A + I = O where OO is the zero matrix. This equation is fundamental as it allows us to simplify any power of AA. From this, we can write: A2=2AIA^2 = 2A - I

2. Deriving a General Expression for AnA^n

Our goal is to find a general formula for AnA^n that holds for all integers nn. Let's look for a pattern using the relation A2=2AIA^2 = 2A - I.

  • For n=0n=0: A0=IA^0 = I
  • For n=1n=1: A1=AA^1 = A
  • For n=2n=2: A2=2AIA^2 = 2A - I (from Cayley-Hamilton)
  • For n=3n=3: A3=AA2=A(2AI)=2A2A=2(2AI)A=4A2IA=3A2IA^3 = A \cdot A^2 = A(2A - I) = 2A^2 - A = 2(2A - I) - A = 4A - 2I - A = 3A - 2I
  • For n=4n=4: A4=AA3=A(3A2I)=3A22A=3(2AI)2A=6A3I2A=4A3IA^4 = A \cdot A^3 = A(3A - 2I) = 3A^2 - 2A = 3(2A - I) - 2A = 6A - 3I - 2A = 4A - 3I

Observing the pattern, it appears that An=nA(n1)IA^n = nA - (n-1)I for n1n \ge 1. Let's check for n=0n=0: A0=0A(01)I=IA^0 = 0A - (0-1)I = I. This holds.

Now, let's verify this formula for negative integer powers. From A22A+I=OA^2 - 2A + I = O, we can multiply by A1A^{-1} (since det(A)=(2)(0)(1)(1)=10\det(A) = (2)(0) - (-1)(1) = 1 \ne 0, A1A^{-1} exists): A2I+A1=OA - 2I + A^{-1} = O So, A1=2IAA^{-1} = 2I - A.

Let's check our conjectured formula An=nA(n1)IA^n = nA - (n-1)I for n=1n=-1: A1=(1)A(11)I=A(2)I=A+2IA^{-1} = (-1)A - (-1-1)I = -A - (-2)I = -A + 2I. This matches perfectly!

The formula An=nA(n1)IA^n = nA - (n-1)I is valid for all integers nZn \in \mathbf{Z}. This is a crucial simplification for the problem.

Tip: For 2×22 \times 2 matrices, finding a general form for AnA^n using the Cayley-Hamilton Theorem is often the most efficient method, especially when AA is diagonalizable or has a simple characteristic polynomial like in this case.

3. Substituting into the Matrix Equation

The given matrix equation is Am2+Am=3IA6A^{m^2}+A^m=3 I-A^{-6}. We will use our general formula An=nA(n1)IA^n = nA - (n-1)I for each term:

  • For Am2A^{m^2}: Replace nn with m2m^2. Am2=m2A(m21)IA^{m^2} = m^2 A - (m^2-1)I
  • For AmA^m: Replace nn with mm. Am=mA(m1)IA^m = mA - (m-1)I
  • For A6A^{-6}: Replace nn with 6-6. A6=(6)A(61)I=6A(7)I=6A+7IA^{-6} = (-6)A - (-6-1)I = -6A - (-7)I = -6A + 7I

Now, substitute these expressions back into the original equation: [m2A(m21)I]+[mA(m1)I]=3I[6A+7I][m^2 A - (m^2-1)I] + [mA - (m-1)I] = 3I - [-6A + 7I]

Combine terms on the left side: (m2+m)A(m21+m1)I=3I+6A7I(m^2+m)A - (m^2-1 + m-1)I = 3I + 6A - 7I (m2+m)A(m2+m2)I=6A4I(m^2+m)A - (m^2+m-2)I = 6A - 4I

4. Equating Coefficients and Solving for mm

We now have an equation of the form XA+YI=PA+QIXA + YI = PA + QI. Since AA and II are linearly independent matrices (unless AA is a scalar multiple of II, which is not the case here), we can equate the coefficients of AA and II on both sides of the equation.

Equating coefficients of AA: m2+m=6m^2+m = 6 Equating coefficients of II: (m2+m2)=4-(m^2+m-2) = -4

Let's solve the first equation: m2+m6=0m^2+m-6 = 0 This is a quadratic equation. We can factor it: (m+3)(m2)=0(m+3)(m-2) = 0 This gives two possible integer values for mm: m=3m=-3 or m=2m=2.

Now, let's check if these values also satisfy the second equation. From the second equation: m2+m2=4m^2+m-2 = 4 m2+m6=0m^2+m-6 = 0 This is the exact same quadratic equation as the first one! This gives us confidence in our solution. So, the values of mm that satisfy both conditions are m=3m=-3 and m=2m=2.

Common Mistake: Forgetting to check if the solutions derived from one coefficient match the other. If the equations for coefficients of AA and II yielded different sets of solutions, then there would be no integer mm satisfying the given matrix equation.

5. Determining n(S)n(S)

The set SS is defined as S={mZ:Am2+Am=3IA6}S=\left\{m \in \mathbf{Z}: A^{m^2}+A^m=3 I-A^{-6}\right\}. We found that the integer values of mm that satisfy the equation are m=3m=-3 and m=2m=2. Therefore, S={3,2}S = \{-3, 2\}.

The number of elements in SS, denoted by n(S)n(S), is 2.

Final Answer: The final answer is 2\boxed{2}.

6. Summary and Key Takeaway

This problem beautifully demonstrates the utility of the Cayley-Hamilton Theorem for simplifying matrix expressions involving powers. The key steps were:

  1. Derive the characteristic equation for matrix AA.
  2. Use Cayley-Hamilton Theorem to find a recurrence relation for AnA^n (e.g., A2=2AIA^2 = 2A-I).
  3. Establish a general formula for AnA^n (in this case, An=nA(n1)IA^n = nA - (n-1)I) valid for all integers nn. This is often the most challenging but rewarding step.
  4. Substitute this general formula into the given matrix equation.
  5. Simplify and equate coefficients of AA and II (due to their linear independence) to form scalar equations.
  6. Solve the resulting scalar equations for mm and identify the integer solutions.

Mastering the Cayley-Hamilton Theorem and recognizing patterns in matrix powers is essential for solving such problems efficiently in competitive exams like JEE.

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