Pseudovector

pseudovector

[¦sü·dō′vek·tər] (physics) A quantity which transforms as a vector under space rotations but which transforms as a vector, together with a change in sign, under a space inversion. Also known as axial vector. A quantity which transforms as a four-vector under Lorentz transformations, but with an additional sign change under space reflection or time reflection or both.

Pseudovector

(or axial vector), a vector in an oriented space that is transformed into the opposite vector when the orientation of the space is reversed. An example of a pseudovector is the vector product of two vectors.

Pseudovector

a vector determined to within an arbitrary numerical factor (vector direction). For example, the homogeneous coordinates x₁, x₂, x₃, x₄ of a point in three-dimensional space with a fixed coordinate system can be considered as the components (coordinates) of a four-dimensional pseudovector.

单词	pseudovector
释义	pseudovector pseudovector (ˌsjuːdəʊˈvɛktə) n (Mathematics) maths a variable quantity, such as angular momentum, that has magnitude and orientation with respect to an axis. The components are even functions of the coordinates. Also called: axial vector Compare pseudoscalar, scalar¹, tensor², vector¹ Pseudovector pseudovector [¦sü·dō′vek·tər] (physics) A quantity which transforms as a vector under space rotations but which transforms as a vector, together with a change in sign, under a space inversion. Also known as axial vector. A quantity which transforms as a four-vector under Lorentz transformations, but with an additional sign change under space reflection or time reflection or both. Pseudovector (or axial vector), a vector in an oriented space that is transformed into the opposite vector when the orientation of the space is reversed. An example of a pseudovector is the vector product of two vectors. Pseudovector a vector determined to within an arbitrary numerical factor (vector direction). For example, the homogeneous coordinates x₁, x₂, x₃, x₄ of a point in three-dimensional space with a fixed coordinate system can be considered as the components (coordinates) of a four-dimensional pseudovector.
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