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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

10 PYQs at 50% HARD, and one stem — A⁻¹ = αI + βA for the same 2 × 2 matrix — has been set five 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

Intuition

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.
Practice this conceptself-check · 4 quick reps

From the bank · past-year question

Example 1Determinants and MatricesMODERATE
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.

[Q117 · May Shift 1 · 2021]

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

Intuition

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.
Practice this conceptself-check · 4 quick reps

From the bank · past-year question

Example 2Determinants and MatricesMODERATE
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) =

[Q127 · 19 April Shift II · 2025]

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

Intuition

(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.
Practice this conceptself-check · 4 quick reps

From the bank · past-year question

Example 3Determinants and MatricesHARD
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

[Q101 · 4th May Shift 1 · 2023]

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

Intuition

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}.
Practice this conceptself-check · 4 quick reps

From the bank · past-year question

Example 4Determinants and MatricesHARD
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}=

[Q144 · 11th May Shift 2 · 2024]

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

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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

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