A submarine hull is treated as an elastic solid whose outer surface is in contact…

PHYSICS · Multi-part · Fermi University Physics · Fluids & Continuum Physics · Solid continuum mechanics and complex fluids · Solid continuum mechanics and complex fluids

Bending, Ringing, Breaking and Flowing, Ch Strain and stress in a deformed solid

Problem

A submarine hull is treated as an elastic solid whose outer surface is in contact with seawater. The water, at rest, exerts on the hull a normal pressure p0p_0 (no shear, since a fluid at rest carries no shear stress) over a small patch of the outer surface whose outward unit normal, pointing from the hull into the water, is n\mathbf n. ((a)) Consider a thin pillbox of face area AA straddling the water-hull interface at this patch: its outer face, of area AA, lies just outside in the water; its inner face, also of area AA, lies just inside the hull; the side faces have area of order hh, where hh is the (vanishingly small) thickness of the pillbox. Balance the forces on this pillbox in the static limit h→0h\to0, in which the body-force term (volume Ah→0Ah\to0) and the side-face tractions (area →0\to0) do not survive. Hence derive the boundary condition satisfied by the Cauchy stress σij\sigma_{ij} just inside the hull at this surface, in terms of p0p_0 and njn_j. State what this condition becomes for an unloaded (vacuum-exposed) free surface, p0=0p_0=0. ((b)) The submarine is at a depth of 250 m250\,\mathrm m in seawater of density 1025 kg m−31025\,\mathrm{kg\,m^{-3}}; take the pressure at the sea surface as negligible next to the hydrostatic pressure at this depth, and use g=9.8 m s−2g=9.8\,\mathrm{m\,s^{-2}}. Evaluate p0p_0 and give the traction ti=σijnjt_i=\sigma_{ij}n_j on the hull's outer surface, as a multiple of n\mathbf n.

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