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Mathematics · Ch 7 — Matrices and Determinants

Determinants of Matrices of Different Order

7.3.1

Determinants of Matrices of Different Order

Order 1. For A=[a]A=[a], ∣A∣=a|A|=a — simply the single entry.

Order 2. For A=(a11a12a21a22)A=\begin{pmatrix}a_{11}&a_{12}\\ a_{21}&a_{22}\end{pmatrix}, ∣A∣=a11a22−a12a21|A|=a_{11}a_{22}-a_{12}a_{21} — product of the main-diagonal pair minus product of the other diagonal pair. E.g. ∣24−12∣=(2)(2)−(−1)(4)=4+4=8\begin{vmatrix}2&4\\-1&2\end{vmatrix}=(2)(2)-(-1)(4)=4+4=8, and ∣cos⁡θsin⁡θ−sin⁡θcos⁡θ∣=cos⁡2θ+sin⁡2θ=1\begin{vmatrix}\cos\theta&\sin\theta\\-\sin\theta&\cos\theta\end{vmatrix}=\cos^2\theta+\sin^2\theta=1.

Order 3 — minors and cofactors. For A=(a11a12a13a21a22a23a31a32a33)A=\begin{pmatrix}a_{11}&a_{12}&a_{13}\\a_{21}&a_{22}&a_{23}\\a_{31}&a_{32}&a_{33}\end{pmatrix}, the minor MijM_{ij} of entry aija_{ij} is the order-2 determinant obtained by deleting row ii and column jj; the cofactor is the signed minor Aij=(−1)i+jMijA_{ij}=(-1)^{i+j}M_{ij}. For instance, M11=∣a22a23a32a33∣=a22a33−a32a23M_{11}=\begin{vmatrix}a_{22}&a_{23}\\a_{32}&a_{33}\end{vmatrix}=a_{22}a_{33}-a_{32}a_{23} and A11=(−1)1+1M11=M11A_{11}=(-1)^{1+1}M_{11}=M_{11}, while A12=(−1)1+2M12=−M12A_{12}=(-1)^{1+2}M_{12}=-M_{12}.

Laplace expansion (Result 7.1/7.2). ∣A∣|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),|A| = a_{11}A_{11}+a_{12}A_{12}+a_{13}A_{13} \quad(\text{expanding along row 1}),

and equally ∣A∣=a21A21+a22A22+a23A23|A|=a_{21}A_{21}+a_{22}A_{22}+a_{23}A_{23} (row 2), or ∣A∣=a11A11+a21A21+a31A31|A|=a_{11}A_{11}+a_{21}A_{21}+a_{31}A_{31} (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

∣A∣=a11a22a33+a12a23a31+a13a21a32−a13a22a31−a11a23a32−a12a21a33|A|=a_{11}a_{22}a_{33}+a_{12}a_{23}a_{31}+a_{13}a_{21}a_{32}-a_{13}a_{22}a_{31}-a_{11}a_{23}a_{32}-a_{12}a_{21}a_{33}

(the three products running down-right minus the three products running down-left).

Worked illustration. For A=(13−24−5635−2)A=\begin{pmatrix}1&3&-2\\4&-5&6\\3&5&-2\end{pmatrix} (numbers per the textbook's own example), expanding along row 1 with the cofactors A11=−40,A12=−26,A13=5A_{11}=-40, A_{12}=-26, A_{13}=5 gives ∣A∣=1(−40)+3(−26)+(−2)(5)=−40−78−10=−128|A|=1(-40)+3(-26)+(-2)(5)=-40-78-10=-128; expanding instead along column 1 gives the same value −128-128, confirming Laplace expansion is expansion-path independent. …