1. D.B. Bogy, Edge-bonded dissimilar orthogonal elastic wedges under normal and shear loading, ASME J.Appl.Mech., Vol. 35 (1968), 460–466.
2. D.B. Bogy, The plane solution for joined dissimilar elastic semistrips under tension, ASME J.Appl.Mech., Vol. 42 (1975), 93–98.
3. Notice that only those stress components that act on the interface (and hence have a z-suffix) are continuous across the interface, because of the equilibrium requirement. The remaining three components will generally be discontinuous because of (24.8-24.10) and the dissimilar elastic properties.
4. This idea can also be extended to steady-state thermoelastic problems by adding in Solution P of Table 17.1, which leaves the expressions (24.11-24.13) for the interface stresses unchanged and requires a further symmetry relation between Ψ1, Ψ2 to satisfy the global condition of continuity of heat flux, qz1(x,y,0+) = qz2(x,y, 0-).
5. See for example J.R. Barber, The penny-shaped crack in shear and related contact problems, Int.J.Engng.Sci., Vol. 13, (1975), 815–829.