If and are two vectors in , the cross product is the vector detailed in Definition 1.4.1.
Because this product yields a vector, some texts call it the vector product of two vectors.
Definition 1.4.1 - Cross Product
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Because it is no small feat to remember the order of all the subscripts in Definition 1.4.1, the following mnemonic (or memory device) is useful as the computational tool by which a cross product can be computed by hand.
The vector can be obtained as the determinant of the 3 × 3 matrix that has the unit basis vectors as the entries in the first row, the components of A in the second row, and of B in the third. The determinant is evaluated by a first-row Laplace expansion in which the three resulting 2 × 2 determinants are called minors. The signs in front of the minors alternate, and a signed minor is called a cofactor. The ith minor for the elements in the first row is the determinant of the array obtained by deleting that row and the ith column.
Note: An internet search for "Laplace expansion 3x3" will bring up a number of sites that review the process of evaluating a determinant by the row-expansion process.
Table 1.4.1 lists some of the cross product's properties that can be extracted from Definition 1.4.1.
Property
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Detail
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Anti-commutation
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Length
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Orthogonality
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is orthogonal to both A and B
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Right-handed System
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A, B, and form a right-handed system of vectors:
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Scalar Multiplication
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Distributive Laws
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and
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Associative Rule - 1
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Associative Rule - 2
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Table 1.4.1 Properties of the cross product
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A right-handed system of the three vectors A, B, and is modeled on the threads of a standard right-threaded screw or bolt that "advances" when rotated clockwise. (Woodworkers, plumbers, mechanics will tell their apprentices "right = tight, left = loose".) If the vector A is rotated into B, the direction of would be that of the advance of the screw turned in the same direction. In other words, if A and B were viewed in a plane facing the viewer with A to the left of B, then would point away from the viewer because the rotation of A into B would be clockwise; with A to the right of B, would point toward the viewer.
Some texts define the cross product by the length, orthogonality, and right-handedness properties, then derive the expression in Definition 1.4.1.