2005
DOI: 10.1016/j.jcis.2004.06.032
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Invalidity of deriving interparticle distance in clay–water systems using the experimental structure factor maximum obtained by small-angle scattering

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Cited by 7 publications
(6 citation statements)
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“…SAXS curves from a series of NIPAAM–Laponite solutions (with clay contents ≤2 wt %) are shown in Figure S5. As expected from dilute dispersions of randomly oriented thin discs, the scattering intensity in the middle- q range follows a power law (i.e., I ( q ) ∝ q –α , where α = 2) . The scattering curve from a 1.0 wt % Laponite–H 2 O solution without monomer, also present in Figure S5, practically overlaps with that of the 1.0 wt % solution with monomer, demonstrating the negligible contribution from the monomer to the overall SAXS signal.…”
Section: Resultssupporting
confidence: 59%
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“…SAXS curves from a series of NIPAAM–Laponite solutions (with clay contents ≤2 wt %) are shown in Figure S5. As expected from dilute dispersions of randomly oriented thin discs, the scattering intensity in the middle- q range follows a power law (i.e., I ( q ) ∝ q –α , where α = 2) . The scattering curve from a 1.0 wt % Laponite–H 2 O solution without monomer, also present in Figure S5, practically overlaps with that of the 1.0 wt % solution with monomer, demonstrating the negligible contribution from the monomer to the overall SAXS signal.…”
Section: Resultssupporting
confidence: 59%
“…As expected from dilute dispersions of randomly oriented thin discs, the scattering intensity in the middle-q range follows a power law (i.e., I(q) ∝ q −α , where α = 2). 27 The scattering curve from a 1.0 wt % Laponite−H 2 O solution without monomer, also present in Figure S5, practically overlaps with that of the 1.0 wt % solution with monomer, demonstrating the negligible contribution from the monomer to the overall SAXS signal. Three of the curves, 1.0, 1.5, and 2.0 wt %, were fitted using the form factor for thin discs 28 (eq 1), where R and 2H are the radius and thickness of the particles, respectively, J 1 (x) is the first-order Bessel function, α is the angle between the axis of the disc and the scattering vector q, (ρ e,clay − ρ e,H 2 O ) is the electron density contrast between the Laponite platelets and water, N clay is the number of clay platelets per unit volume, and v clay is the volume of a single disc.…”
Section: Resultsmentioning
confidence: 86%
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“…∆ρ, P(q), and S exp (q) are the scattering length density difference between the clay particles and the matrix, the form factor of the clay particles, and the experimental structure factor, respectively [20][21][22][23][24]. Here the magnitude of the wavevector q is defined by the following equation.…”
Section: Structures Of Clay/paas Hydrogelsmentioning
confidence: 99%
“…The values, in general, decreased by increasing the polyP dose and remained negative in the entire concentration range studied. This tendency can be explained by referring to previous studies on LRD-phosphate systems. , It was also suggested that the progressive adsorption of polyP on the positively charged edges of LRD (as illustrated in Scheme , middle), leads to an increase in the overall negative particle charge at higher polyP doses . Variations in the degree of polymerization did not yield any significant changes in the electrophoretic mobilities.…”
Section: Resultsmentioning
confidence: 63%