Dendrimers

From SklogWiki
Revision as of 19:25, 14 November 2013 by Carl McBride (talk | contribs) (→‎Radius of gyration: Added Chen-Cui result)
Jump to navigation Jump to search
A single dendrimer molecule (G4 PAMAM, solvent not shown)

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

N=1+fP(f−1)G+1−1f−2

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

Gmax≈2.88(lnP+1.5)

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 (RG) scales as [5]

RG∝N1/3

where N is the number of monomers. This implies a compact structure.

Ideal dendrimer

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


RGideal∝PG

Chen-Cui scaling law

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


RG∝(PG)1−νN2ν−1

where ν is the Flory exponent.

Specific dendrimers

See also

References

Related reading