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Answers for “矩阵的行列式是什么?”

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Algebraically, for a matrix [abcd]\begin{bmatrix} a & b \\ c & d \end{bmatrix}, the determinant is ad−bcad - bc. Geometrically, adad captures the primary rectangular bounds, while subtracting bcbc corrects for overlapping triangular regions created by off-diagonal shearing components.

Conditions: Matrix is 2x2; Entries are real numbers

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The determinant is computed using the standard 2×22\times 2 rule ad−bcad - bc. For the matrix A=[3112]A = \begin{bmatrix} 3 & 1 \\ 1 & 2 \end{bmatrix}, this means multiplying the main diagonal entries (3⋅23 \cdot 2) and subtracting the product of the off-diagonal entries (1⋅11 \cdot 1).

Conditions: The matrix is 2×22\times 2.; Entries are real numbers.

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A2×2A 2\times 2 transformation matrix maps the standard basis vectors to its own columns. Specifically, the first column of the matrix is the image of the vector [1,0]T[1, 0]^T, and the second column is the image of the vector [0,1]T[0, 1]^T.

Conditions: The matrix is 2×22\times 2.; Working in standard Cartesian coordinates.

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Each column of a2×2a 2\times 2 matrix can be read as the coordinates of a vector in the 2D plane. For the matrix A=[3112]A = \begin{bmatrix} 3 & 1 \\ 1 & 2 \end{bmatrix}, the first column [31]\begin{bmatrix} 3 \\ 1 \end{bmatrix} represents the vector from the origin to the point (3,1), and the second column [12]\begin{bmatrix} 1 \\ 2 \end{bmatrix} represents the vector from the origin to the point (1,2).

Conditions: The matrix is 2×22\times 2.; Working in standard Cartesian coordinates.

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To find the area of the transformed region, multiply the original area by the absolute value of the determinant of the transformation matrix. The formula is: New Area=Old Area⋅∣det⁡(A)∣\text{New Area} = \text{Old Area} \cdot |\det(A)|.

Conditions: The transformation is linear and represented by a2×2a 2\times 2 matrix.; The original area is known.; Use ordinary Euclidean area in standard orthonormal coordinates.

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A 3D linear transformation is fully determined by tracking where the standard basis vectors (i^\hat{i}, j^\hat{j}, and k^\hat{k}) land. The coordinates of these three transformed vectors are recorded as column vectors to form a 3x3 matrix.

Conditions: Working in three-dimensional Cartesian space; Using the standard basis vectors aligned with x, y, and z axes; The transformation is linear (preserves grid lines parallel/evenly spaced and fixes origin)

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Starting from Av=λvAv = \lambda v, we rewrite the right side as (λI)v(\lambda I)v and move all terms to one side to get (A−λI)v=0(A - \lambda I)v = 0. Since we seek non-zero solutions for vv, the matrix (A−λI)(A - \lambda I) must squash space into a lower dimension (have a non-trivial null space).

Conditions: vv is a non-zero eigenvector; AA is a square matrix; II is the identity matrix