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Hydrodynamic radius

The hydrodynamic radius of a macromolecule or colloid particle has two meanings. Some books use it as a synonym for the Stokes radius. ^[1]

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Others books define a theoretical hydrodynamic radius $R h y d$ . They consider the macromolecule or colloid particle to be a collection of $N$ subparticles. This is done most commonly for polymers; the subparticles would then be the units of the polymer. $R h y d$ is defined by

$\frac{1}{R_{hyd}} \ \stackrel{\mathrm{def}}{=}\ \frac{1}{N^{2}} \langle \sum_{i \neq j} \frac{1}{r_{ij}} \rangle$

where $r i j$ is the distance between subparticles $i$ and $j$ , and where the angular brackets $\langle \ldots \rangle$ represent an ensemble average. ^[2] The theoretical hydrodynamic radius $R h y d$ was originally an estimate by John G. Kirkwood of the Stokes radius of a polymer.

The theoretical hydrodynamic radius $R h y d$ arises in the study of the dynamic properties of polymers moving in a solvent. It is often similar in magnitude to the radius of gyration.

Notes

^ Gert R. Strobl (1996). The Physics of Polymers Concepts for Understanding Their Structures and Behavior. Springer-Verlag. ISBN 3-540-60768-4. Section 6.4 page 290.
^ J. Des Cloizeaux and G. Jannink (1990). Polymers in Solution Their Modelling and Structure. Clarendon Press. ISBN 0-19-852-036-0. Chapter 10, Section 7.4, pages 415-417.