1987
DOI: 10.1107/s0021889887087107
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Scattering from fractals

Abstract: The concepts of dilation symmetry and the fractal dimension are introduced, and from these basic concepts scattering functions are computed for surface and mass fractals. It is then shown how the fractal structure of various random media has been elucidated from scattering measurements, and how these observations relate to specific models of fractal geometry. Examples include colloidal aggregates, gels, soot and the fractal porosity of rocks of various sorts.

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Cited by 568 publications
(393 citation statements)
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“…This value of D is similar to the value of 1.75 which has been predicted by a computer simulation for cluster-cluster aggregation [8]. In this process an assembly of Brownian particles stick together upon contact to form clusters.…”
Section: I(h) =Ah -Dsupporting
confidence: 71%
See 1 more Smart Citation
“…This value of D is similar to the value of 1.75 which has been predicted by a computer simulation for cluster-cluster aggregation [8]. In this process an assembly of Brownian particles stick together upon contact to form clusters.…”
Section: I(h) =Ah -Dsupporting
confidence: 71%
“…The deviation from Porod's law (I(h) = b * h -4) have been observed by many authors for different types of silica (for example aerogels [5], colloidal aggregates [6], silica gels formed by controlled hydrolysis of tetra ethyl orthosilicates [7]). Especially the excellent review articles of Martin and Hurt [8] and Ramsay [9] give a good overall picture of the fractal properties of silica gels derived from SAXS or SANS spectra in the Porod region.…”
Section: I(h) =Ah -Dmentioning
confidence: 99%
“…The analysis of the limiting power law in the Porod region of the scattering curves can provide some information on the interface in the TEOS/PCL hybrid materials. Indeed, in case of fractal structures, the SAXS intensity l(s) agrees with the following power laws 17 where D m is the mass fractal dimension and D s is the surface fractal dimension. Figure 10 shows that each scattering profile approaches a limiting slope of 1.7 for curve A and 1.6 for curve B, respectively, indicating that the interface structure is mass fractal whatever the reactivity of the PCL end-groups.…”
Section: Resultsmentioning
confidence: 49%
“…Over limited range of aggregate radii the mass of the fractal aggregate, m, is directly related to the radius of a circumscribing sphere within the aggregate, l , to the power of d f (Martin and Hurd 1987;Knöchel et al 1997):…”
Section: Aggregate Structurementioning
confidence: 99%