Surface and bulk compositions of various solids are given in Table 3.
In our present study the constitutive equations for the three-phase-lag dipolar thermoelastic solids are given.
Finally, our results point to the need to avoid that conflicting and confusing recommendations and advice regarding the timing of introduction of solids be given to parents.
Before the visit, parents were asked to complete a three day food diary to assess whether the infant was exclusively or partially breast fed and whether formula or solids were given.
The formula for Y in a general anisotropic solid is given.
The constitutive higher-order tensor defining the equivalent Mindlin solid is given in a surprisingly simple formula.
Moreover, by differentiating equation (1) with respect to t, it follows that the Eulerian velocity field of the solid is given for every t ≥ 0 by u S ( x, t ) = ξ ′ ( t ) + θ ′ ( t ) ( x − ξ ( t ) ) ⊥ + w ( x, t ) ∀ x ∈ S ( ξ ( t ), θ ( t ), t ), (8).
and the elastic self-energy, γ dis, of a fully circular dislocation loop in an infinite isotropic elastic solid is given by γ dis = G b 2 8 π 2 − v film 1 − v film ln 4 r r core − 2, (3).
The specific energy of each solid is given in separable form: it is the sum of a hydrodynamic part of the energy depending only on the density and the entropy, and an elastic part of the energy which is unaffected by the volume change.
Analytic expressions for the responses of the displacements and stresses for field points either inside or on the surface of the half-plane solid are given for general anisotropic materials.
