The Navier-Stokes equations for incompressible flow in their Lagrangian form are taken as a starting point. A perturbation technique is then used to obtain first- and second-order sets of equations, and the general procedure for solving the equations to any order is given. The first-order equations yield interesting two- and three-dimensional motions that have some of the properties of ‘stirring’ ‘eddies’ and ‘turbulence’; it is suggested that various problems in turbulent motion might possibly be re-examined by means of these equations.
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Willard J. Pierson (1962) studied this question.
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