Order 1. For A=[a], ∣A∣=a — simply the single entry.
Order 2. For A=(a11a21a12a22), ∣A∣=a11a22−a12a21 — product of the main-diagonal pair minus product of the other diagonal pair. E.g. 2−142=(2)(2)−(−1)(4)=4+4=8, and cosθ−sinθsinθcosθ=cos2θ+sin2θ=1.
Order 3 — minors and cofactors. For A=a11a21a31a12a22a32a13a23a33, the minorMij of entry aij is the order-2 determinant obtained by deleting row i and column j; the cofactor is the signed minor Aij=(−1)i+jMij. For instance, M11=a22a32a23a33=a22a33−a32a23 and A11=(−1)1+1M11=M11, while A12=(−1)1+2M12=−M12.
Laplace expansion (Result 7.1/7.2).∣A∣ equals the sum of the products of the entries of any one row (or column) with their corresponding cofactors, and this value is the same no matter which row/column you choose:
∣A∣=a11A11+a12A12+a13A13(expanding along row 1),
and equally ∣A∣=a21A21+a22A22+a23A23 (row 2), or ∣A∣=a11A11+a21A21+a31A31 (column 1), etc. For hand computation, expand along whichever row/column has the most zeros.
Sarrus' Rule (a direct order-3 shortcut, named after Pierre Frédéric Sarrus): repeat the first two columns to the right, then
(the three products running down-right minus the three products running down-left).
Worked illustration. For A=1433−55−26−2 (numbers per the textbook's own example), expanding along row 1 with the cofactors A11=−40,A12=−26,A13=5 gives ∣A∣=1(−40)+3(−26)+(−2)(5)=−40−78−10=−128; expanding instead along column 1 gives the same value −128, confirming Laplace expansion is expansion-path independent. …