Dendrimers: Difference between revisions

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:<math>R_G \propto N^{1/3}</math>
:<math>R_G \propto N^{1/3}</math>


where <math>N</math> is the number of monomers.
where <math>N</math> is the number of monomers. This implies a compact structure.
====Ideal dendrimer====
====Ideal dendrimer====
For an ''ideal'' dendrimer, consisting of non-interacting monomers, <math>R_G</math> is given by <ref>[http://dx.doi.org/10.1039/FT9969204151 Wilfried Carl "A Monte Carlo study of model dendrimers", Journal of the Chemical Society, Faraday Transactions '''92''' pp. 4151-4154 (1996)]</ref>
For an ''ideal'' dendrimer, consisting of non-interacting monomers, <math>R_G</math> is given by <ref>[http://dx.doi.org/10.1039/FT9969204151 Wilfried Carl "A Monte Carlo study of model dendrimers", Journal of the Chemical Society, Faraday Transactions '''92''' pp. 4151-4154 (1996)]</ref>
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:<math>R_{G \mathrm{ideal} } \propto \sqrt{PG}</math>
:<math>R_{G \mathrm{ideal} } \propto \sqrt{PG}</math>
====Chen-Cui scaling law====
The Chen-Cui scaling law is given by <ref>[http://dx.doi.org/10.1021/ma9514636 Zheng Yu Chen and Shi-Min Cui "Monte Carlo Simulations of Star-Burst Dendrimers", Macromolecules '''29''' pp. 7943-7952 (1996)]</ref>:
:<math>R_G \propto  (PG)^{1-\nu}N^{2\nu-1}</math>
where <math>\nu</math> is the [[Flory exponent]].


==Specific dendrimers==
==Specific dendrimers==

Revision as of 19:25, 14 November 2013

A single dendrimer molecule (G4 PAMAM, solvent not shown)

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. This implies a compact structure.

Ideal dendrimer

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


Chen-Cui scaling law

The Chen-Cui scaling law is given by [7]:


where is the Flory exponent.

Specific dendrimers

See also

References

Related reading