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Small-angle X-ray scattering on spinodal,nucleotic or coarsening processes in two-phase systems containing spherical,fibrillar or lamellar inhomogeneities
Authors:A Jánosi
Institution:1. Institute of Physical Chemistry, University of Graz, Heinrichstrasse 28, A-8010, Graz, Austria
Abstract:We study the effects of some of the most important and typical structural changes in two-phase systems on selected structural parameters obtained from small-angle x-ray scattering (SAXS) measurements. To limit the present study, it was assumed that the Phase, 1, embedded in the matrix
  1. is monodispersed and homogeneous,
  2. possesses one of the three most extreme shapes (spherical, fibrillar or lamellar) and
  3. changes its behaviour
  1. through type change (spinodal or nucleotic or coarsening), without changing the shape,
  2. through a change of the shape only, or
  3. through a) (type change) and b) (shape change) simultaneously.
To find the type of change for three basically different shapes of Phase 1 and to calculate its intensity (amount of the change) the following three SAXS parameters must be compared before and after the treatment of the system:
  1. chord lengthl 1 (and/or radius of gyrationR),
  2. volume partw 1 of the Phase 1, and
  3. relative inner surfaceS v of the system.
It is shown by this comparison that by the pure type change in the case of
  1. spinodal change, all three SAXRS parameters are increasing or decreasing simultaneously and proportional to a power of the intensity of the change,
  2. nucleotic change,l 1 (and/orR) is unchanged, the other two (w 1 andS v ) are increasing or decreasing simultaneously and directly proportional to the intensity,
  3. coarsening change,w 1 is unchanged and anincreasing ofl 1 is always accompanied by adecreasing ofS v and vice versa.
In addition to this type change, the cases of mere changes of the shape (“shape change”) and finally of simultaneous type and/or shape change are studied. For the case of pure shape change the alteration of the dimensions (chord lengthl 1 and/or radius of gyrationR) must be followed. The limitations of the analyses of the simultaneous type and/or shape change are discussed in detail.
Keywords:
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