A remarkable shell structure is described that, due to a particular combination of
geometry and initial stress, has zero stiffness for any finite deformation along a
twisting path; the shell is in a neutrally stable state of equilibrium. Initially the shell
is straight in a longitudinal direction, but has a constant, nonzero curvature in the
transverse direction. If residual stresses are induced in the shell by, for example,
plastic deformation, to leave a particular resultant bending moment, then an
analytical inextensional model of the shell shows it to have no change in energy along
a path of twisted configurations. Real shells become closer to the inextensional
idealization as their thickness is decreased; experimental thin-shell models have
confirmed the neutrally stable configurations predicted by the inextensional theory. A
simple model is described that shows that the resultant bending moment that leads
to zero stiffness gives the shell a hidden symmetry, which explains this remarkable
property.