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Figure 3
Distance distribution functions obtained by indirect method from experimental SAXS patterns of PU/PMMA latex particles presented in the Fig. 2[link] (left-hand side column of the plots) and compared with those calculated for the model core–shell particles (Rc = 300 Å, R = 370 Å, ξc = 0.379 e Å−3 and ξs = 0.364 e Å−3) surrounded by different contrast media (right-hand side column of the plots). Figures on the plots indicate mass density (in g cm−3) of the corresponding sucrose solution. Both experimental and simulated sets of distance distribution functions have been normalized by the maximum value obtained in its own p(r) corresponding to the latex particles diluted in water (ρm ≃ 1.0 g cm−3). The distance distribution functions obtained from the experiment have been fitted with the equation of p(r) corresponding to the ensemble of core–shell particles with normal distribution of electron densities of both the core and the shell, equation (1)[link] (the obtained parameters are: Rc = 258 Å, R = 365 Å, ξc = 0.381 e Å−3, ξs = 0.366 e Å−3, σc = 0.017 e Å−3 and σs = 0.005 e Å−3). The model and the parameters are discussed later in the text.

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