Gelation

Gelation (gel transition) is the formation of a gel from a system with polymers.[1][2] Branched polymers can form links between the chains, which lead to progressively larger polymers. As the linking continues, larger branched polymers are obtained and at a certain extent of the reaction links between the polymer result in the formation of a single macroscopic molecule. At that point in the reaction, which is defined as gel point, the system loses fluidity and viscosity becomes very large. The onset of gelation, or gel point, is accompanied by a sudden increase in viscosity.[3] This "infinite" sized polymer is called the gel or network, which does not dissolve in the solvent, but can swell in it.[4]

Polymers prior (no gel) and after crosslinking (gel)

BackgroundEdit

Gelation is promoted by gelling agents. Gelation can occur either by physical linking or by chemical crosslinking. While the physical gels involve physical bonds, chemical gelation involves covalent bonds. The first quantitative theories of chemical gelation were formulated in the 1940s by Flory and Stockmayer. Critical percolation theory was successfully applied to gelation in 1970s. A number of growth models (diffusion limited aggregation, cluster-cluster aggregation, kinetic gelation) were developed in the 1980s to describe the kinetic aspects of aggregation and gelation.[5]

Quantitative approaches to determine gelationEdit

It is important to be able to predict the onset of gelation, since it is an irreversible process that dramatically changes the properties of the system.

Average functionality approachEdit

According to the Carothers equation number-average degree of polymerization   is given by

 

where   is the extent of the reaction and   is the average functionality of reaction mixture. For the gel   can be considered to be infinite, thus the critical extent of the reaction at the gel point is found as

 

If   is greater or equal to  , gelation occurs.

Flory Stockmayer approachEdit

Flory and Stockmayer used a statistical approach to derive an expression to predict the gel point by calculating when   approaches infinite size. The statistical approach assumes that (1) the reactivity of the functional groups of the same type is the same and independent of the molecular size and (2) there are no intramolecular reactions between the functional groups on the same molecule.[6][7]

Consider the polymerization of bifunctional molecules  ,   and multifunctional  , where   is the functionality. The extends of the functional groups are  and  , respectively. The ratio of all A groups, both reacted and unreacted, that are part of branched units, to the total number of A groups in the mixture is defined as  . This will lead to the following reaction

 

The probability of obtaining the product of the reaction above is given by  , since the probability that a B group reach with a branched unit is   and the probability that a B group react with non-branched A is  .

This relation yields to an expression for the extent of reaction of A functional groups at the gel point

 

where r is the ratio of all A groups to all B groups. If more than one type of multifunctional branch unit is present and average   value is used for all monomer molecules with functionality greater than 2.

Note that the relation does not apply for reaction systems containing monofunctional reactants and/or both A and B type of branch units.

Erdős–Rényi modelEdit

Gelation of polymers can be described in the framework of the Erdős–Rényi model or the Lushnikov model, which answers the question when a giant component arises.[8]

Random graphEdit

The structure of a gel network can be conceptualised as a random graph. This analogy is exploited to calculate the gel point and gel fraction for monomer precursors with arbitrary types of functional groups. Random graphs can be used to derive analytical expressions for simple polymerisation mechanisms, such as step-growth polymerisation, or alternatively, they can be combined with a system of rate equations that are integrated numerically.

See alsoEdit

ReferencesEdit

  1. ^ Oliveira, J.T.; Reis, R.L. (2008). "Hydrogels from polysaccharide-based materials: Fundamentals and applications in regenerative medicine". Natural-Based Polymers for Biomedical Applications. pp. 485–514. doi:10.1533/9781845694814.4.485. ISBN 9781845692643.
  2. ^ Ahmed, Enas M. (2015). "Hydrogel: Preparation, characterization, and applications: A review". Journal of Advanced Research. 6 (2): 105–121. doi:10.1016/j.jare.2013.07.006. PMC 4348459. PMID 25750745.
  3. ^ Odian, George (2004). Principles of Polymerization. doi:10.1002/047147875x. ISBN 0471274003.
  4. ^ Chanda, Manas (2006). Introduction to Polymer Science and Chemistry. doi:10.1201/9781420007329. ISBN 9781420007329.[page needed]
  5. ^ 20-, Rubinstein, Michael, 1956 December (2003). Polymer physics. Colby, Ralph H. Oxford: Oxford University Press. ISBN 978-0198520597. OCLC 50339757.CS1 maint: numeric names: authors list (link)[page needed]
  6. ^ Stockmayer, Walter H. (February 1943). "Theory of Molecular Size Distribution and Gel Formation in Branched‐Chain Polymers". The Journal of Chemical Physics. 11 (2): 45–55. Bibcode:1943JChPh..11...45S. doi:10.1063/1.1723803.
  7. ^ Flory, Paul J. (November 1941). "Molecular Size Distribution in Three Dimensional Polymers. I. Gelation". Journal of the American Chemical Society. 63 (11): 3083–3090. doi:10.1021/ja01856a061.
  8. ^ Buffet, E.; Pulé, J. V. (1991-07-01). "Polymers and random graphs". Journal of Statistical Physics. 64 (1): 87–110. Bibcode:1991JSP....64...87B. doi:10.1007/BF01057869. ISSN 1572-9613. S2CID 120859837.