A hollow steel sphere with bore radius and outer radius holds an internal pressure

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

Bending, Ringing, Breaking and Flowing, Ch Hooke's law for an isotropic solid

Problem

A hollow steel sphere with bore radius a=50 mma = 50\,\mathrm{mm} and outer radius b=100 mmb = 100\,\mathrm{mm} holds an internal pressure p=100 MPap = 100\,\mathrm{MPa}, with its outer surface free. With no body force, the radial solution of the Navier equation in a sphere is u(r)=Ar+B/r2u(r) = Ar + B/r^2. ((a)) In spherical coordinates the radial strain is εrr=du/dr\varepsilon_{rr} = \mathrm du/\mathrm dr, and the two angular strains are both u/ru/r. Use the isotropic law to show that σrr=3KA−4GB/r3\sigma_{rr} = 3KA - 4GB/r^3 and σθθ=3KA+2GB/r3\sigma_{\theta\theta} = 3KA + 2GB/r^3. ((b)) Fit AA and BB to the two boundary conditions and show that σθθ=[pa3/(b3−a3)](1+b3/2r3)\sigma_{\theta\theta} = [pa^3/(b^3-a^3)](1 + b^3/2r^3), the spherical result quoted in the chapter. ((c)) Evaluate the hoop stress at the bore, and compare it with the bore hoop stress of a long tube with the same radii and pressure.

Browse the problem library