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Reynolds operator : ウィキペディア英語版
Reynolds operator
In fluid dynamics and invariant theory, a Reynolds operator is a mathematical operator given by averaging something over a group action, that satisfies a set of properties called Reynolds rules. In fluid dynamics Reynolds operators are often encountered in models of turbulent flows, particularly the Reynolds-averaged Navier–Stokes equations, where the average is typically taken over the fluid flow under the group of time translations. In invariant theory the average is often taken over a compact group or reductive algebraic group acting on a commutative algebra, such as a ring of polynomials. Reynolds operators were introduced into fluid dynamics by and named by .
==Definition==
Reynolds operators are used in fluid dynamics, functional analysis, and invariant theory, and the notation and definitions in these areas differ slightly. A Reynolds operator acting on φ is sometimes denoted by ''R''(''φ''), ''P''(''φ''), ''ρ''(''φ''), 〈''φ''〉, or . Reynolds operators are usually linear operators acting on some algebra of functions, satisfying the identity
: ''R''(''R''(''φ'')''ψ'') = ''R''(''φ'')''R''(''ψ'') for all ''φ'', ''ψ''
and sometimes some other conditions, such as commuting with various group actions.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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