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Oscillating Flat-Plate Flow for Maxwellian Fluids

Oscillating Flat-Plate Flow for Maxwellian Fluids [Pg.299]

Stokes second problem deals with the behavior of a semi-infinite fluid if the wall bounding the fluid performs harmonic oscillations in its plane. This problem is stated as a problem without initial data [181,482] only the boundary condition [Pg.299]

The problem is reduced to solving a linear partial differential equation of hyperbolic type (the telegraph equation [482]) in the region t 0, 0 Y oo. Specifically, we have the equation [Pg.299]

Strictly speaking, to obtain a unique solution in an infinite region, condition (6.10.17) must be supplemented by the Sommerfeld radiation condition [234, 317], so as to eliminate waves coming from infinity. The solution of this problem has the form [Pg.299]

Obviously, the oscillation frequency is the same and is equal to ui at any point of the half-space, whereas the amplitude and the phase of the oscillations varies with the spatial coordinate Y. [Pg.299]




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