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Scattering by a homogeneous solute

The solution consists of only one solvent and one solute. In this case, it is not necessary to use any index for the solute and we write [Pg.263]

we write the structure function as the sum of intramolecular and intermolecular contributions [see (7.2.25)] [Pg.264]

Let M = Nm be the molecular mass of the solute molecules. Now, the result (7.2.58) reads [Pg.264]

The appearance of Avogadro s number in this expression results from the definition (7.2.57) of the constant K. This can be justified as follows. In ordinary space, the correlation function g(r) — 1 differs practically from zero only in a range of the same order as the size R of the molecules, let us say for instance 10 nm. Therefore, the Fourier transform //n(0) is a volume of the order of 103 nm3, but the product //n(0) is a macroscopic volume ( 104 cm3) which can be more directly measured, for instance, by looking at the osmotic pressure. [Pg.264]


Scattering by a homogeneous solute in the zero-angle limit The solute is homogeneous if all the monomers are the same. [Pg.272]


See other pages where Scattering by a homogeneous solute is mentioned: [Pg.263]    [Pg.124]   


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