Quick Recap — Matrices

  • Order m×nm\times n = rows ×\times columns; square if m=nm=n.
  • Special: identity II (1's on the diagonal), diagonal, scalar, symmetric (AT=AA^T=A), skew-symmetric (AT=AA^T=-A, zero diagonal).
  • Operations: add/subtract need the same order; ABAB needs (cols of AA) = (rows of BB).
  • (AT)T=A(A^T)^T=A, (AB)T=BTAT(AB)^T=B^TA^T, IA=AIA=A; trace = sum of diagonal entries.

Beyond-NCERT JEE Formulae

Cayley-Hamilton Theorem

Every square matrix satisfies its own characteristic equation det(AλI)=0\det(A-\lambda I)=0. For a 2×22\times2 matrix this becomes

A2(trA)A+AI=O.A^2-(\operatorname{tr}A)\,A+|A|\,I=O.

Rearranging delivers the inverse with no separate adjoint computation:

A1=1A[(trA)IA],A0.A^{-1}=\dfrac{1}{|A|}\big[(\operatorname{tr}A)\,I-A\big],\qquad |A|\ne0.

Higher powers collapse the same way: multiply the identity by AA to get A3=(trA)A2AAA^3=(\operatorname{tr}A)\,A^2-|A|\,A, and keep reducing so that every power stays in the shape An=pA+qIA^n=pA+qI.

[JEE Tip] The moment a question wants A1A^{-1}, a high power AnA^n, or a relation such as A3=pA+qIA^3=pA+qI, reach for Cayley-Hamilton — it beats direct multiplication almost every time.

Characteristic-Equation Facts (2x2)

For a 2×22\times2 matrix the characteristic equation is

λ2(trA)λ+A=0.\lambda^2-(\operatorname{tr}A)\,\lambda+|A|=0.

Its roots are the eigenvalues λ1\lambda_1 and λ2\lambda_2, and comparing coefficients gives

λ1+λ2=trA,λ1λ2=A.\lambda_1+\lambda_2=\operatorname{tr}A,\qquad \lambda_1\lambda_2=|A|.

So the sum of the eigenvalues equals the trace and their product equals the determinant — an instant check on any eigenvalue you compute.

Adjoint Identities Beyond the Basics

  • Reversal law: adj(AB)=adjBadjA\operatorname{adj}(AB)=\operatorname{adj}B\,\operatorname{adj}A — the order flips, exactly like (AB)1(AB)^{-1} and (AB)T(AB)^T.
  • Inverse of the adjoint: (adjA)1=adj(A1)=AA(\operatorname{adj}A)^{-1}=\operatorname{adj}(A^{-1})=\dfrac{A}{|A|}.
  • Determinant of a double adjoint: adj(adjA)=A(n1)2|\operatorname{adj}(\operatorname{adj}A)|=|A|^{(n-1)^2} for an n×nn\times n matrix.
  • The 2x2 shortcut: here (n1)2=1(n-1)^2=1, and in fact adj(adjA)=A\operatorname{adj}(\operatorname{adj}A)=A itself — taking the adjoint twice returns the original matrix.

[JEE Tip] For general order nn, adj(adjA)=An2A\operatorname{adj}(\operatorname{adj}A)=|A|^{\,n-2}A; setting n=2n=2 recovers adj(adjA)=A\operatorname{adj}(\operatorname{adj}A)=A.

Solved Examples — Beyond-NCERT Formulae

Example 1 — Inverse of a 2x2 via Cayley-Hamilton

Find A1A^{-1} for A=(2112)A=\begin{pmatrix}2&1\\1&2\end{pmatrix} without building the adjoint separately.

Step 1. Trace and determinant: trA=2+2=4\operatorname{tr}A=2+2=4 and A=2211=3|A|=2\cdot2-1\cdot1=3.

Step 2. Cayley-Hamilton gives A24A+3I=OA^2-4A+3I=O, so 3I=4AA2=A(4IA)3I=4A-A^2=A(4I-A).

Step 3. Therefore A1=13(4IA)=13(2112)A^{-1}=\dfrac{1}{3}\big(4I-A\big)=\dfrac{1}{3}\begin{pmatrix}2&-1\\-1&2\end{pmatrix}.

Check. AA1=13(3003)=IA\,A^{-1}=\dfrac{1}{3}\begin{pmatrix}3&0\\0&3\end{pmatrix}=I, as required.

Example 2 — Computing A3A^3 by reduction

Let A=(1213)A=\begin{pmatrix}1&2\\1&3\end{pmatrix}. Find A3A^3 without cubing directly.

Step 1. trA=4\operatorname{tr}A=4 and A=1321=1|A|=1\cdot3-2\cdot1=1, so Cayley-Hamilton gives A2=4AIA^2=4A-I.

Step 2. Multiply by AA and substitute: A3=4A2A=4(4AI)A=15A4IA^3=4A^2-A=4(4A-I)-A=15A-4I.

Step 3. Hence A3=15(1213)4I=(11301541)A^3=15\begin{pmatrix}1&2\\1&3\end{pmatrix}-4I=\begin{pmatrix}11&30\\15&41\end{pmatrix}.

The characteristic relation replaced two matrix multiplications with a single scalar reduction.

Example 3 — The zero-matrix verification

Confirm A2(trA)A+AI=OA^2-(\operatorname{tr}A)\,A+|A|\,I=O for A=(2314)A=\begin{pmatrix}2&3\\1&4\end{pmatrix}.

Step 1. trA=6\operatorname{tr}A=6 and A=83=5|A|=8-3=5.

Step 2. Compute A2=(718619)A^2=\begin{pmatrix}7&18\\6&19\end{pmatrix} and 6A=(1218624)6A=\begin{pmatrix}12&18\\6&24\end{pmatrix}.

Step 3. Then A26A+5I=(712+51818661924+5)=(0000)=OA^2-6A+5I=\begin{pmatrix}7-12+5&18-18\\6-6&19-24+5\end{pmatrix}=\begin{pmatrix}0&0\\0&0\end{pmatrix}=O, so the theorem checks out.

Example 4 — A 3x3 characteristic equation

For A=(211010112)A=\begin{pmatrix}2&1&1\\0&1&0\\1&1&2\end{pmatrix}, write its characteristic equation and use it to find A1A^{-1}.

Step 1. For order 33 the characteristic equation is λ3(trA)λ2+SλA=0\lambda^3-(\operatorname{tr}A)\,\lambda^2+S\,\lambda-|A|=0, where SS is the sum of the three principal 2×22\times2 minors.

Step 2. Here trA=5\operatorname{tr}A=5, then S=2+3+2=7S=2+3+2=7 and A=3|A|=3, so λ35λ2+7λ3=0\lambda^3-5\lambda^2+7\lambda-3=0.

Step 3. By Cayley-Hamilton A35A2+7A3I=OA^3-5A^2+7A-3I=O, so 3I=A(A25A+7I)3I=A\big(A^2-5A+7I\big) and A1=13(A25A+7I)A^{-1}=\dfrac{1}{3}\big(A^2-5A+7I\big).

Step 4. With A2=(544010445)A^2=\begin{pmatrix}5&4&4\\0&1&0\\4&4&5\end{pmatrix} this yields A1=13(211030112)A^{-1}=\dfrac{1}{3}\begin{pmatrix}2&-1&-1\\0&3&0\\-1&-1&2\end{pmatrix}.

Example 5 — The adjoint reversal law

For A=(1234)A=\begin{pmatrix}1&2\\3&4\end{pmatrix} and B=(2013)B=\begin{pmatrix}2&0\\1&3\end{pmatrix}, verify adj(AB)=adjBadjA\operatorname{adj}(AB)=\operatorname{adj}B\,\operatorname{adj}A.

Step 1. AB=(461012)AB=\begin{pmatrix}4&6\\10&12\end{pmatrix}, so adj(AB)=(126104)\operatorname{adj}(AB)=\begin{pmatrix}12&-6\\-10&4\end{pmatrix}.

Step 2. Separately, adjA=(4231)\operatorname{adj}A=\begin{pmatrix}4&-2\\-3&1\end{pmatrix} and adjB=(3012)\operatorname{adj}B=\begin{pmatrix}3&0\\-1&2\end{pmatrix}.

Step 3. Then adjBadjA=(3012)(4231)=(126104)\operatorname{adj}B\,\operatorname{adj}A=\begin{pmatrix}3&0\\-1&2\end{pmatrix}\begin{pmatrix}4&-2\\-3&1\end{pmatrix}=\begin{pmatrix}12&-6\\-10&4\end{pmatrix}, matching Step 1.

Order matters: the reversed product adjAadjB=(144102)\operatorname{adj}A\,\operatorname{adj}B=\begin{pmatrix}14&-4\\-10&2\end{pmatrix} is different, so the flip in the law is essential.

Example 6 — Eigenvalues from the characteristic equation

Find the eigenvalues of A=(4123)A=\begin{pmatrix}4&1\\2&3\end{pmatrix} and check them against the trace and determinant.

Step 1. trA=7\operatorname{tr}A=7 and A=122=10|A|=12-2=10, so the characteristic equation is λ27λ+10=0\lambda^2-7\lambda+10=0.

Step 2. Factoring, (λ2)(λ5)=0(\lambda-2)(\lambda-5)=0, so λ1=2\lambda_1=2 and λ2=5\lambda_2=5.

Step 3. Cross-check: λ1+λ2=7=trA\lambda_1+\lambda_2=7=\operatorname{tr}A and λ1λ2=10=A\lambda_1\lambda_2=10=|A|, confirming the roots.

Example 7 — Taking the adjoint twice

For A=(3124)A=\begin{pmatrix}3&1\\2&4\end{pmatrix}, show that adj(adjA)=A\operatorname{adj}(\operatorname{adj}A)=A and find (adjA)1(\operatorname{adj}A)^{-1}.

Step 1. adjA=(4123)\operatorname{adj}A=\begin{pmatrix}4&-1\\-2&3\end{pmatrix}.

Step 2. Taking the adjoint again, adj(adjA)=(3124)=A\operatorname{adj}(\operatorname{adj}A)=\begin{pmatrix}3&1\\2&4\end{pmatrix}=A, exactly as the 2x2 rule predicts.

Step 3. Since A=122=10|A|=12-2=10, the identity (adjA)1=AA(\operatorname{adj}A)^{-1}=\dfrac{A}{|A|} gives (adjA)1=110(3124)(\operatorname{adj}A)^{-1}=\dfrac{1}{10}\begin{pmatrix}3&1\\2&4\end{pmatrix}.

Example 8 — A high power through eigenvalues

Compute A5A^5 for A=(0213)A=\begin{pmatrix}0&-2\\1&3\end{pmatrix} using the characteristic equation.

Step 1. trA=3\operatorname{tr}A=3 and A=03(2)1=2|A|=0\cdot3-(-2)\cdot1=2, so λ23λ+2=0\lambda^2-3\lambda+2=0 with roots λ=1\lambda=1 and λ=2\lambda=2.

Step 2. Write A5=pA+qIA^5=pA+qI. The same scalar relation holds at each eigenvalue, so 15=p+q1^5=p+q and 25=2p+q2^5=2p+q.

Step 3. Subtracting the first equation from the second, p=321=31p=32-1=31, then q=131=30q=1-31=-30, giving A5=31A30IA^5=31A-30I.

Step 4. Substitute: A5=31(0213)30I=(30623163)A^5=31\begin{pmatrix}0&-2\\1&3\end{pmatrix}-30I=\begin{pmatrix}-30&-62\\31&63\end{pmatrix}.