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MHT-CET Maths · Determinants and Matrices

Cayley–Hamilton, Matrix Polynomials and Powers

Every 2 × 2 matrix satisfies A² − (trace)A + |A|I = 0 — so A⁻¹ is a combination αI + βA, a factored polynomial in A gives A⁻¹ in one line, and powers of A cycle.

Why this matters

17 PYQs at 35% HARD, and one stem — A⁻¹ = αI + βA for a given 2 × 2 matrix — has been set four times in three years, asked for α − β, α + β, x and y, or 2x + 3y. The rest of the page is the same theorem read differently: a matrix given by (A − 3I)(A − 5I) = 0, an inverse of A + 3I from A² − 4A + 3I = 0, and a power A²⁰²⁹ that collapses because A³ is a scalar. Nothing here needs the adjoint; that is the point of the page.

Concept 1 of 4: Cayley–Hamilton for 2 × 2: A² − (tr A)A + |A|·I = 0

A matrix satisfies its own characteristic equation. For 2×22 \times 2 that equation is λ2−(trace)λ+det⁡=0\lambda^2 - (\text{trace})\lambda + \det = 0, so A2A^2 is always a combination of AA and II — which is why every higher power and the inverse reduce to αI+βA\alpha I + \beta A.

Definition

  • Trace tr⁡A=a+d\operatorname{tr}A = a + d; determinant ∣A∣=ad−bc|A| = ad - bc. Then A2−(a+d)A+(ad−bc)I=OA^2 - (a + d)A + (ad - bc)I = O.
  • For A=(1−123)A = \begin{pmatrix} 1 & -1 \\ 2 & 3 \end{pmatrix}: trace 44, determinant 55, so A2−4A+5IA^2 - 4A + 5I is the null matrix — no multiplication needed.
  • Consequences: A2=(tr⁡A)A−∣A∣IA^2 = (\operatorname{tr}A)A - |A|I; multiply by A−1A^{-1}: A=(tr⁡A)I−∣A∣A−1A = (\operatorname{tr}A)I - |A|A^{-1}, so A−1=(tr⁡A)I−A∣A∣A^{-1} = \dfrac{(\operatorname{tr}A)I - A}{|A|}.
  • Verify the theorem on any 2×22 \times 2 once by direct multiplication; after that, quote it.

Cayley–Hamilton (2 × 2)

A2−(tr⁡A) A+∣A∣ I=OA−1=(tr⁡A) I−A∣A∣A^2 - (\operatorname{tr}A)\,A + |A|\,I = O \qquad A^{-1} = \frac{(\operatorname{tr}A)\,I - A}{|A|}
  • tr⁡A\operatorname{tr}Asum of the diagonal entries
  • OOthe zero matrix

Worked example

For A=(2113)A = \begin{pmatrix} 2 & 1 \\ 1 & 3 \end{pmatrix}, find A2−5A+5IA^2 - 5A + 5I without computing A2A^2.
Practise this conceptself-check · 4 quick reps

The same idea in a real exam question:

MHT-CET · 2021 · May Shift 1 · Q117Moderate

Example 1 · Determinants and Matrices · Cayley–Hamilton, Matrix Polynomials and Powers

If matrix A=(1−123)A = \begin{pmatrix}1&-1\\2&3\end{pmatrix}, then A2−4A+5IA^2 - 4A + 5I is where II is a unit matrix.

Sign of the determinant term

It is A2−(tr⁡A)A+∣A∣IA^2 - (\operatorname{tr}A)A + |A|I: minus the trace, PLUS the determinant. Writing −∣A∣I-|A|I turns a null-matrix answer into a wrong 'symmetric matrix' option.

Concept 2 of 4: A⁻¹ = αI + βA: Read α and β From the Theorem

Rearranging Cayley–Hamilton gives A−1=tr⁡A∣A∣I−1∣A∣AA^{-1} = \dfrac{\operatorname{tr}A}{|A|}I - \dfrac{1}{|A|}A. So α=tr⁡A∣A∣\alpha = \dfrac{\operatorname{tr}A}{|A|} and β=−1∣A∣\beta = -\dfrac{1}{|A|}, with no adjoint and no entry-matching.

Definition

  • From A2−tA+dI=OA^2 - tA + dI = O (t=tr⁡At = \operatorname{tr}A, d=∣A∣d = |A|): A−1=tdI−1dAA^{-1} = \dfrac{t}{d}I - \dfrac1d A. Hence α=td\alpha = \dfrac{t}{d}, β=−1d\beta = -\dfrac1d.
  • A=(12−14)A = \begin{pmatrix} 1 & 2 \\ -1 & 4 \end{pmatrix}: t=5t = 5, d=6d = 6, so α=56\alpha = \dfrac56, β=−16\beta = -\dfrac16; then 4(α−β)=44(\alpha - \beta) = 4, 4(α+β)=834(\alpha + \beta) = \dfrac83.
  • A=(12−51)A = \begin{pmatrix} 1 & 2 \\ -5 & 1 \end{pmatrix} with A−1=xA+yIA^{-1} = xA + yI: t=2t = 2, d=11d = 11, so x=−111x = -\dfrac{1}{11}, y=211y = \dfrac{2}{11}, and 2x+3y=4112x + 3y = \dfrac{4}{11}.
  • Cross-check by entry-matching if time allows: the (1,2)(1,2) entry of αI+βA\alpha I + \beta A is 2β2\beta, which must equal the (1,2)(1,2) entry of adj⁡A∣A∣\dfrac{\operatorname{adj}A}{|A|}.
  • Read what is asked: α−β\alpha - \beta, α+β\alpha + \beta, (x,y)(x, y) or a weighted sum — the same matrix has been asked all four ways.

Inverse as a combination

A−1=αI+βA  with  α=tr⁡A∣A∣, β=−1∣A∣A^{-1} = \alpha I + \beta A \ \text{ with } \ \alpha = \frac{\operatorname{tr}A}{|A|},\ \beta = -\frac{1}{|A|}

Worked example

For A=(3124)A = \begin{pmatrix} 3 & 1 \\ 2 & 4 \end{pmatrix}, write A−1=αI+βAA^{-1} = \alpha I + \beta A and find α+β\alpha + \beta.
Practise this conceptself-check · 4 quick reps

The same idea in a real exam question:

MHT-CET · 2025 · 19 April Shift II · Q127Moderate

Example 2 · Determinants and Matrices · Cayley–Hamilton, Matrix Polynomials and Powers

If A=[12−14]A=\begin{bmatrix} 1 & 2 \\ - 1 & 4 \end{bmatrix} and A−1=αI+βAα,β∈RA^{- 1}=\alpha I+\beta A\alpha,\beta\in R where II is the identity matrix of order 2 , hen 4(α+β)=4(\alpha+\beta) =

α from the wrong entry

Matching the (1,1)(1,1) entry gives α+β\alpha + \beta, not α\alpha — for (12−14)\begin{pmatrix} 1 & 2 \\ -1 & 4 \end{pmatrix} that is 23\frac23, and reading it as α\alpha makes 4(α−β)=1034(\alpha - \beta) = \frac{10}{3}, which is offered. α=tr⁡A/∣A∣=56\alpha = \operatorname{tr}A/|A| = \frac56.

Concept 3 of 4: A Factored Polynomial in A Gives A⁻¹ in One Line

(A−3I)(A−5I)=O(A - 3I)(A - 5I) = O expands to A2−8A+15I=OA^2 - 8A + 15I = O. Multiply through by A−1A^{-1} and the inverse appears: 15A−1=8I−A15A^{-1} = 8I - A. No entries, no adjoint — the relation IS the inverse.

Definition

  • Expand the given factorisation (matrices with II commute, so ordinary algebra applies): (A−3I)(A−5I)=A2−8A+15I(A - 3I)(A - 5I) = A^2 - 8A + 15I.
  • Multiply by A−1A^{-1} (AA non-singular): A−8I+15A−1=OA - 8I + 15A^{-1} = O, so A−1=8I−A15A^{-1} = \dfrac{8I - A}{15}, i.e. 158A−1=I−18A\dfrac{15}{8}A^{-1} = I - \dfrac18A; and αA+βA−1=4I\alpha A + \beta A^{-1} = 4I is matched by α=12\alpha = \dfrac12, β=152\beta = \dfrac{15}{2}, sum 88.
  • Inverse of a shifted matrix: from A2−4A+3I=OA^2 - 4A + 3I = O, write A2−4A+3I=(A+3I)(A−7I)+24IA^2 - 4A + 3I = (A + 3I)(A - 7I) + 24I, so (A+3I)(A−7I)=−24I(A + 3I)(A - 7I) = -24I and (A+3I)−1=7I−A24(A + 3I)^{-1} = \dfrac{7I - A}{24}. Choose the second factor so that the product's constant term matches.
  • The technique: treat AA like a number in polynomial identities, but never divide by a matrix — multiply by the inverse instead.

From a polynomial relation to the inverse

A2−pA+qI=O (q≠0) ⇒ A−1=pI−Aq(A+kI)−1: write A2−pA+qI=(A+kI)(A−mI)+cIA^2 - pA + qI = O \ (q \ne 0) \ \Rightarrow\ A^{-1} = \frac{pI - A}{q} \qquad (A + kI)^{-1}:\ \text{write } A^2 - pA + qI = (A + kI)(A - mI) + cI

Worked example

If AA is non-singular and (A−2I)(A−4I)=O(A - 2I)(A - 4I) = O, express A−1A^{-1} in terms of AA and II.
Practise this conceptself-check · 4 quick reps

The same idea in a real exam question:

MHT-CET · 2023 · 4th May Shift 1 · Q101Hard

Example 3 · Determinants and Matrices · Cayley–Hamilton, Matrix Polynomials and Powers

Suppose A is any 3×33\times3 non-singular matrix and (A−3I)(A−5I)=O(A-3I)(A-5I)=O where I=I3I=I_3 and O=O3O=O_3. Here O3O_3 represent zero matrix of order 3 and I3I_3 is an identity matrix of order 3. If αA+βA−1=4I\alpha A + \beta A^{-1} = 4I, then α+β\alpha + \beta is equal to

Concluding A = 3I or A = 5I

(A−3I)(A−5I)=O(A - 3I)(A - 5I) = O does NOT force either factor to be zero — matrices have zero divisors. The information is the polynomial relation, and only that.

Concept 4 of 4: Powers of a Matrix: Find the Cycle

For A=(i110)A = \begin{pmatrix} i & 1 \\ 1 & 0 \end{pmatrix}, A3A^3 turns out to be iIiI, a scalar. Then A12=(iI)4=IA^{12} = (iI)^4 = I, and A2029A^{2029} is just AA — the exponent only matters modulo the cycle length.

Definition

  • Compute A2A^2, A3A^3, … until a scalar multiple of II (or II itself) appears. If Am=cIA^m = cI, then Amk=ckIA^{mk} = c^kI.
  • A=(i110)A = \begin{pmatrix} i & 1 \\ 1 & 0 \end{pmatrix}: A2=(0ii1)A^2 = \begin{pmatrix} 0 & i \\ i & 1 \end{pmatrix}, A3=iIA^3 = iI, so A12=i4I=IA^{12} = i^4I = I. 2029=12⋅169+12029 = 12\cdot169 + 1, hence A2029=AA^{2029} = A.
  • The inverse of A2029A^{2029} is then A−1=adj⁡A∣A∣A^{-1} = \dfrac{\operatorname{adj}A}{|A|} with ∣A∣=−1|A| = -1: −adj⁡A-\operatorname{adj}A.
  • Cayley–Hamilton is the general engine: A2=tA−dIA^2 = tA - dI lets any power be reduced to pA+qIpA + qI step by step; a cycle appears when AmA^m lands on cIcI.

Powers modulo a cycle

Am=cI ⇒ Amk+r=ckAr(i110)3=iI,i4=1A^m = cI \ \Rightarrow\ A^{mk + r} = c^k A^r \qquad \begin{pmatrix} i & 1 \\ 1 & 0 \end{pmatrix}^3 = iI,\quad i^4 = 1

Worked example

For A=(01−10)A = \begin{pmatrix} 0 & 1 \\ -1 & 0 \end{pmatrix}, find A101A^{101}.
Practise this conceptself-check · 4 quick reps

The same idea in a real exam question:

MHT-CET · 2024 · 11th May Shift 2 · Q144Hard

Example 4 · Determinants and Matrices · Cayley–Hamilton, Matrix Polynomials and Powers

If A=(i110)A=\begin{pmatrix}i&1\\1&0\end{pmatrix} where i=−1i=\sqrt{-1} and B=A2029B=A^{2029}, then B−1=B^{-1}=

Reducing 2029 modulo 3 instead of 12

A3=iIA^3 = iI is a scalar but NOT the identity; the cycle closes at A12=IA^{12} = I. Using 33 gives A2029=A1⋅i676=AA^{2029} = A^{1}\cdot i^{676} = A only by luck of the arithmetic — reduce modulo the exponent at which the power returns to II.

Summary — formulas & gotchas at a glance

A revision cheat-sheet for the formulas and gotchas above. Click any concept name to jump back to its full explanation.

Formulas (4)

  • Cayley–Hamilton for 2 × 2: A² − (tr A)A + |A|·I = 0

    Cayley–Hamilton (2 × 2)

    A2−(tr⁡A) A+∣A∣ I=OA−1=(tr⁡A) I−A∣A∣A^2 - (\operatorname{tr}A)\,A + |A|\,I = O \qquad A^{-1} = \frac{(\operatorname{tr}A)\,I - A}{|A|}
  • A⁻¹ = αI + βA: Read α and β From the Theorem

    Inverse as a combination

    A−1=αI+βA  with  α=tr⁡A∣A∣, β=−1∣A∣A^{-1} = \alpha I + \beta A \ \text{ with } \ \alpha = \frac{\operatorname{tr}A}{|A|},\ \beta = -\frac{1}{|A|}
  • A Factored Polynomial in A Gives A⁻¹ in One Line

    From a polynomial relation to the inverse

    A2−pA+qI=O (q≠0) ⇒ A−1=pI−Aq(A+kI)−1: write A2−pA+qI=(A+kI)(A−mI)+cIA^2 - pA + qI = O \ (q \ne 0) \ \Rightarrow\ A^{-1} = \frac{pI - A}{q} \qquad (A + kI)^{-1}:\ \text{write } A^2 - pA + qI = (A + kI)(A - mI) + cI
  • Powers of a Matrix: Find the Cycle

    Powers modulo a cycle

    Am=cI ⇒ Amk+r=ckAr(i110)3=iI,i4=1A^m = cI \ \Rightarrow\ A^{mk + r} = c^k A^r \qquad \begin{pmatrix} i & 1 \\ 1 & 0 \end{pmatrix}^3 = iI,\quad i^4 = 1

Watch out for (4)

Test yourself on Determinants and Matrices

15 past MHT-CET questions from this chapter, timed at 27 minutes and marked the way the exam marks it. You see your score and every answer the moment you finish. Free to start.