Special: identity I (1's on the diagonal), diagonal, scalar, symmetric (AT=A), skew-symmetric (AT=−A, zero diagonal).
Operations: add/subtract need the same order; AB needs (cols of A) = (rows of B).
(AT)T=A, (AB)T=BTAT, IA=A; trace = sum of diagonal entries.
Beyond-NCERT JEE Formulae
Cayley-Hamilton Theorem
Every square matrix satisfies its own characteristic equationdet(A−λI)=0. For a 2×2 matrix this becomes
A2−(trA)A+∣A∣I=O.
Rearranging delivers the inverse with no separate adjoint computation:
A−1=∣A∣1[(trA)I−A],∣A∣=0.
Higher powers collapse the same way: multiply the identity by A to get A3=(trA)A2−∣A∣A, and keep reducing so that every power stays in the shape An=pA+qI.
[JEE Tip] The moment a question wants A−1, a high power An, or a relation such as A3=pA+qI, reach for Cayley-Hamilton — it beats direct multiplication almost every time.
Characteristic-Equation Facts (2x2)
For a 2×2 matrix the characteristic equation is
λ2−(trA)λ+∣A∣=0.
Its roots are the eigenvaluesλ1 and λ2, and comparing coefficients gives
λ1+λ2=trA,λ1λ2=∣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 — the order flips, exactly like (AB)−1 and (AB)T.
Inverse of the adjoint:(adjA)−1=adj(A−1)=∣A∣A.
Determinant of a double adjoint:∣adj(adjA)∣=∣A∣(n−1)2 for an n×n matrix.
The 2x2 shortcut: here (n−1)2=1, and in fact adj(adjA)=A itself — taking the adjoint twice returns the original matrix.
[JEE Tip] For general order n, adj(adjA)=∣A∣n−2A; setting n=2 recovers adj(adjA)=A.
Solved Examples — Beyond-NCERT Formulae
Example 1 — Inverse of a 2x2 via Cayley-Hamilton
Find A−1 for A=(2112) without building the adjoint separately.
Step 1. Trace and determinant: trA=2+2=4 and ∣A∣=2⋅2−1⋅1=3.
Step 2. Cayley-Hamilton gives A2−4A+3I=O, so 3I=4A−A2=A(4I−A).
Step 3. Therefore A−1=31(4I−A)=31(2−1−12).
Check.AA−1=31(3003)=I, as required.
Example 2 — Computing A3 by reduction
Let A=(1123). Find A3 without cubing directly.
Step 1.trA=4 and ∣A∣=1⋅3−2⋅1=1, so Cayley-Hamilton gives A2=4A−I.
Step 2. Multiply by A and substitute: A3=4A2−A=4(4A−I)−A=15A−4I.
Step 3. Hence A3=15(1123)−4I=(11153041).
The characteristic relation replaced two matrix multiplications with a single scalar reduction.
Example 3 — The zero-matrix verification
Confirm A2−(trA)A+∣A∣I=O for A=(2134).
Step 1.trA=6 and ∣A∣=8−3=5.
Step 2. Compute A2=(761819) and 6A=(1261824).
Step 3. Then A2−6A+5I=(7−12+56−618−1819−24+5)=(0000)=O, so the theorem checks out.
Example 4 — A 3x3 characteristic equation
For A=201111102, write its characteristic equation and use it to find A−1.
Step 1. For order 3 the characteristic equation is λ3−(trA)λ2+Sλ−∣A∣=0, where S is the sum of the three principal 2×2 minors.
Step 2. Here trA=5, then S=2+3+2=7 and ∣A∣=3, so λ3−5λ2+7λ−3=0.
Step 3. By Cayley-Hamilton A3−5A2+7A−3I=O, so 3I=A(A2−5A+7I) and A−1=31(A2−5A+7I).
Step 4. With A2=504414405 this yields A−1=3120−1−13−1−102.
Example 5 — The adjoint reversal law
For A=(1324) and B=(2103), verify adj(AB)=adjBadjA.
Step 1.AB=(410612), so adj(AB)=(12−10−64).
Step 2. Separately, adjA=(4−3−21) and adjB=(3−102).
Step 3. Then adjBadjA=(3−102)(4−3−21)=(12−10−64), matching Step 1.
Order matters: the reversed product adjAadjB=(14−10−42) is different, so the flip in the law is essential.
Example 6 — Eigenvalues from the characteristic equation
Find the eigenvalues of A=(4213) and check them against the trace and determinant.
Step 1.trA=7 and ∣A∣=12−2=10, so the characteristic equation is λ2−7λ+10=0.
Step 2. Factoring, (λ−2)(λ−5)=0, so λ1=2 and λ2=5.
Step 3. Cross-check: λ1+λ2=7=trA and λ1λ2=10=∣A∣, confirming the roots.
Example 7 — Taking the adjoint twice
For A=(3214), show that adj(adjA)=A and find (adjA)−1.
Step 1.adjA=(4−2−13).
Step 2. Taking the adjoint again, adj(adjA)=(3214)=A, exactly as the 2x2 rule predicts.
Step 3. Since ∣A∣=12−2=10, the identity (adjA)−1=∣A∣A gives (adjA)−1=101(3214).
Example 8 — A high power through eigenvalues
Compute A5 for A=(01−23) using the characteristic equation.
Step 1.trA=3 and ∣A∣=0⋅3−(−2)⋅1=2, so λ2−3λ+2=0 with roots λ=1 and λ=2.
Step 2. Write A5=pA+qI. The same scalar relation holds at each eigenvalue, so 15=p+q and 25=2p+q.
Step 3. Subtracting the first equation from the second, p=32−1=31, then q=1−31=−30, giving A5=31A−30I.