Electrospinning Physical Gels: The Case of Stereocomplex PMMA
Electrospinning Physical Gels: The Case of Stereocomplex PMMA
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DOI:
10.1021/ma9005395
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发表时间:
2009-07-14
期刊:
影响因子:
5.5
通讯作者:
Srinivasarao, Mohan
中科院分区:
文献类型:
--
作者:
Crne, Matija;Park, Jung Ok;Srinivasarao, Mohan
DiscussionThe viscoelasticity and spinnability of a polymer solution are closely related to the solvent type, temperature, and polymer concentration. For a good solvent, where polymerrsolvent interaction is favored over polymerrpolymer interaction, the chains behave like a single molecule belowC*, the overlap concentration, related to molecular weight as C*∼ Mra∼ Mr0. 5 from the Berry number and MarkrHouwinkrSakurada equation. 22 As the name suggests, polymer chains start to overlap beyond the overlap concentration, and hence the viscosity of the system increases steeply with concentration above it. It has been shown that the formation of stereocomplex helices increases the persistence length and makes the polymer chain more rodlike. 23 In that case, the MarkrHouwink coefficient a becomes larger, 24 and the overlap occurs at a much lower concentration C*. Thus, gelation can occur at a lower concentration than the C* calculated for a Gaussian or a flexible chain. While the increase in viscosity is linear with concentration for dilute regime, it increases by C4, 5 in the semidilute regime. This is due to presence of entanglements that act as temporary cross-links and hence also impart gel-like elasticity to the polymer solution. Gupta et al. have determined that a-PMMA solutions in DMF need a concentration ratioC/C* of at least 4 to produce smooth electrospun fibers. 21 The C/C* ratio of the 5 wt% stereocomplexing mixture that produced smooth fibers was 2 in our case, which is much lower than reported for linear a-PMMA polymers. We can attribute this to the helix formation and physical gelation during the electrospinning process. It has been shown previously that physical gels require a lower concentration to electrospin smooth, continuous fibers. 25 In our case, the comparison with a-PMMA is all the more relevant, as the only difference between the a-PMMA solution and the stereocomplex PMMA solution is the occurrence of physical gelation. Although stereocomplex-like interactions in atactic PMMA solutions in strongly complexing solvents (DMF is a strongly complexing solvent) have been detected by spectroscopic methods (NMR, FTIR) 26r28 and DSC, 28, 29 the observation of physical gelation was not reported. Most likely the length of the isoatactic and syndiotactic sequences in atactic PMMA polymers was not sufficient to facilitate the formation of long helices and subsequent packing into bundles and gelation. For illustration, the average length of isotactic sequences reported in atactic PMMA was 1.33 r1. 53 monomer units, 28 while it takes 9 isotactic monomer units for one pitch of the helix. 30 During gelation, the polymer chains interact with each other and aggregate into a 3D percolated structure, essentially increasing the effective molecular weight of the system. The polymer chains can do this even below the critical overlap concentration C*. Therefore, C* is not the most important parameter that describes the interactions of a physical gel. The elastic modulus also increases during the gelation process. Recently, Yu et al. have determined that the elasticity of the fluid is more important for electrospun jet stability than the number of entanglements. 31 With solutions that will form physical gels, either argument can explain their peculiar behavior. The polymer chains associate in the solution, forming a crosslinked network. This structure increases the elasticity of the fluid