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The vector triple product is defined as ... A related identity regarding gradients and useful in vector calculus is Lagrange's formula of vector cross-product ...
The dotted vector, in this case B, is differentiated, while the (undotted) A is held constant. The utility of the Feynman subscript notation lies in its use in the derivation of vector and tensor derivative identities, as in the following example which uses the algebraic identity C⋅(A×B) = (C×A)⋅B:
There are two lists of mathematical identities related to vectors: Vector algebra relations — regarding operations on individual vectors such as dot product, cross product, etc. Vector calculus identities — regarding operations on vector fields such as divergence, gradient, curl, etc.
The following are important identities in vector algebra.Identities that only involve the magnitude of a vector ‖ ‖ and the dot product (scalar product) of two vectors A·B, apply to vectors in any dimension, while identities that use the cross product (vector product) A×B only apply in three dimensions, since the cross product is only defined there.
The Jacobi triple product identity is the Macdonald identity for the affine root system of type A 1, and is the Weyl denominator formula for the corresponding affine Kac–Moody algebra. Properties [ edit ]
The cross product with respect to a right-handed coordinate system. In mathematics, the cross product or vector product (occasionally directed area product, to emphasize its geometric significance) is a binary operation on two vectors in a three-dimensional oriented Euclidean vector space (named here ), and is denoted by the symbol .
The scalar triple product of three vectors is defined as ... The vector triple product is defined by [2] [3] ... This identity, ...
The first two identities abstract the skew symmetry and Jacobi identity for the triple commutator, while the third identity means that the linear map L u,v: V → V, defined by L u,v (w) = [u, v, w], is a derivation of the triple product. The identity also shows that the space k = span {L u,v : u, v ∈ V} is closed under commutator bracket ...