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Small amplitude sinusoidal fluctuation

An isotropic elastic solid with a nominally flat, traction-free surface is subjected to an initial equilibrium stress field. Suppose that the shape of the free surface S in the undeformed reference configuration of the material is not actually a plane, but that it is slightly wavy. The nominally flat surface coincides with the plane y = 0 and the position of the actual surface varies with respect to y = 0 in the x—direction. At time t, the position of the surface at coordinate x is given hy y = h x,t). For the discussion in this section, it is assumed that the slope of the surface is small everywhere, that is, h,x C 1 at all points on the surface. The boundary condition which must be enforced on the wavy surface is that the traction is zero. [Pg.624]

If Oij is the stress field evaluated at a point on the surface and nj is the outward unit normal vector there then CTijUj = 0 at that point. This condition must be enforced pointwise on the wavy surface, and this will be done for the case of small amplitude surface slope. A sketch of a small por- [Pg.624]

Prior to perturbation of surface shape, an equilibrium state of stress [Pg.625]

The total stress field for the perturbed shape of the surface is of the form [Pg.625]

Then (8.44) indicates that the boundary conditions on the additional stress field a x,y) due to perturbation of the shape of the free surface to y = h x, t) will be [Pg.625]


See other pages where Small amplitude sinusoidal fluctuation is mentioned: [Pg.624]    [Pg.624]    [Pg.140]    [Pg.427]    [Pg.65]    [Pg.424]    [Pg.107]    [Pg.105]   


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