Abstract
Porod's law extended to the sixth-order term can be written I = (Kp/s4 + K6/s6)U2(s,σ) where I is the scattered intensity, s = 2(sinθ)/λ, θ being half the scattering angle and λ the wavelength used; U2(s, σ) describes the interphase profile and σ is a measure of the width of the interphase transition zone. Kp and K6 are two constants. In the same way as Kp can be related to the specific area, K6 is related to a pure number θ called here `angulosity'. For an angulous body, θ always is negative and can easily be calculated when its geometry is simple. It does not depend on the dimensions of the body. It is shown in the present paper that K6/Kp = θ/2π2S so that, in a two-phase system, the ratio K6/Kp represents the angulosity per unit area S of the interface between the phases. A least-squares analysis of the experimental small-angle X-ray scattering (SAXS) curve gives the values of Kp, K6 and σ. The method was successfully applied in the case of telechelic ionomers to characterize their ionic aggregates. These aggregates present a larger angulosity than that of a parallelepiped. Their volume is relatively small and only contains a small number of ions. The results agree with the results obtained by other techniques. It can be concluded from this that the introduction of the s−6 term into Porod's law is judicious and allows the structure of the phases to be better characterized.
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