Dendrimers: Difference between revisions

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:<math>G_{\mathrm{max}} \approx 2.88 (\ln P + 1.5) </math>
:<math>G_{\mathrm{max}} \approx 2.88 (\ln P + 1.5) </math>
However, recent work by Zook and Pickett <ref>[http://dx.doi.org/10.1103/PhysRevLett.90.015502 Thomas C. Zook and Galen T. Pickett "Hollow-Core Dendrimers Revisited", Physical Review Letters '''90''' 015502 (2003)]</ref> has shown that the de Gennes and Hervet model was flawed.


====Dense core model====
====Dense core model====

Revision as of 17:31, 14 November 2013

Dendrimers. Dendrimers can be characterised by three parameters: functionality (), spacer length () and number of generations (). The number of monomers () in a dendrimer is given by

Density profile

Dense shell model

de Gennes and Hervet [1] calculated that for self-avoiding dendrimers in a good solvent, the density profile increases from a minimum at the centre of the dendrimer to a maximum at its outer surface, i.e. a dense outer shell with a hollow centre. Note this leads to a limit of

However, recent work by Zook and Pickett [2] has shown that the de Gennes and Hervet model was flawed.

Dense core model

Most studies support the dense core model of Lescanec and Muthukumar[3] despite early uptake of the dense shell model. Boris and Rubinstein pointed out that the structure of the dendrimer is a result of the competition between the entropy and excluded volume [4], neither of which terms favouring a hollow centre.

Radius of gyration

It has been suggested that the radius of gyration () scales as [5]

where is the number of monomers.

Ideal dendrimer

For an ideal dendrimer, consisting of non-interacting monomers, is given by [6]


Specific dendrimers

See also

References

Related reading