1
a) B. Wessling, DE 34 22 316 and corresponding international patents
(Zipperling Kessler & Co.)
b) B. Wessling, Ad. Mater. 5 (4), 300 - 305 (1993)
2 the first reports of "soluble" and "moldable" conductive polymers were published by
R. L. Elsenbaumer, K. Jen, R. Obodi, Polym. Master. Sci. Eng. 53, 79 (1985)
R. L. Elsenbaumer, K. Jen, R. Obodi, Synthetic Metals 15, 169 (1986)
3L. Shacklette, C. Han, "Solubility and dispersion characteristics of Polyaniline", Mat. Res. Soc: Symp. Proc. 328, 157 - 166 (1994), a paper in which the authors tried to determine the solubility parameter of polyaniline, emeraldine base and salt (EB, ES)
4for entering this field of science, many textbooks are available, like
a) S. Ross, I. Morrison: "Colloidal Systems and Interfaces", J.- Wiley 1988
b) D. Everett "Basic Principles of Colloid Science", Royal Society of Chemistry, 1988
from which I took some ideas for this paragraph
5for a deeper discussion, cf. any good textbook about macromolecular science
6 quantitative figures are generally rare in the field of solution or dispersion properties, and - if available - differing; as it is not the goal to calculate precisely but to support qualitative arguments by appropriate data; they are taken as average numbers from tables being found in
- R. Weast, M. Astle (eds.) Handbook of Chemistry and Physics, 62nd edition, CRC press 1981
- A. Barton, Handbook of Solubility Parameters and other Cohesion Parameters, CRC Press1985
- J. Brandrup, E. Immergut (eds.), Polymer Handbook 2nd edition, J. Wiley 1975
7R. Pelster, G. Nimtz, B. Wessling, Phys. Rev. B 49, 12718 - 12 723
8G. Nimtz, P. Marquardt, H. Gleiter, J. Cryst. Growth, 86, 66 (1988)
P. Marqurdt, G. Nimtz, Phys. Rev. B, 40, 7996 (1989)
9Hollemann, Wiberg "Anorganische Chemie", W. de Gruyter, 1971
10Cotton, Wilkinson, "Anorganische Chemie", Verlag Chemie 1970
11this value was estimated by using the Born-Haber cycle for HCl (gas) using known values.
12Y. Fu, R. Elsenbaumer, Chemistry of Materials (Am. Chem. Soc.) 6 (5), 671 (1994)
13B. Wessling, Synthetic Metals 45, 119 - 145 (1991)
14B. Wessling, Z. Phys. Chem. 191, 119 - 135 (1995)
15see [6], ref. c) Handbook of Chemistry and Physics
16E. Bosch, Z. Phys. 137, 89 - 103 (1954)
17B. Wessling, Polym. Sci. Engin. 31 (16), 1200 - 1206 (1991) and also cf. [2]; for a broader discussion of dissipative structures in such systems, cf. B. Wessling, in: S. Nalwa (ed.) Handbook of Organic Conductive Molecules and Polymers, Vol III, J. Wiley (in press)
18B, Wessling, Synthetic Met. 41-43, 907 - 910 (1991)
19and analogous for PAni with other counter-ions than HCl, provided that the monomer/counterion relation is 0.5, so that no shell of detergent-like counterions forms, as is the case with DBSA, CSA and others.
20In the meantime we have succeeded in preparing several different types of stable water dispersions of polyaniline, but only by using a non-conventional approach; cf. data sheet Ormecon Chemie
21P. Kinlen, ICSM 1996 Snowbird/USA, Synthetic Met., in press
22XICP-OS01, Experimental Product Data Sheet, Monsanto, 1996
23"Neste Conductive Polymer", technical information about experimental product Polyaniline, Neste Oy, 1995
24R. Strey, G. Porte, P. Bassereau, Langmuir 6, 1635 - 1639 (1990)
M. Kahlweit, R. Strey, G. Busse, J. Phys. Chem. 94, 3881 (1990)
25J. Frommer, R. Elsenbaumer, R. Chance, Org. Coat. Appl. Pol. sci. Proc., 48, 552 (1983)
J. Frommer, Acc. Chem. Res. 19, 2 - 9 (1986)
26A. Andreatta, Y. Cao, J. Chiang, A. Heeger, P. Smith Synthetic Met. 26, 383 - 389 (1988)
27Y. Cao, P. Smith, A. Heeger, Synthetic Met. 57, 3514 (1993)
A. MacDiarmid, A. Epstein, Synthetic Met. 65, 103 - 116 (1994)
28A. Andreatta, Synthetic Met. 41 (3), 1063 (1991); however, from this presentation at the ICSM Göteborg, the author only published the abstract and not the viscosity data presented at the conference
29C. Gettinger, A. Heeger, D. Pine, Y. Cao, Synthetic Met. 74, 81 - 88 (1995)
30because it provides a high shear stress, which is necessary for dispersion, as was shown theoretically [14]
31cf. [1], examples 1, 3, 4
32it should be noted, that the authors mentioned: "In our experiments, we did not observe any measurable effects on the size of the polymer radius until considerably higher water/aniline fractions (about 1000); even at these concentrations the size of the radius was reduced only by a factor of 2." This is in accordance with the consideration, that water is soluble in m-cresol and only a portion is being adsorbed on the PAni particles.
33Y. Cao, P. Smith, Polymer 34 (15), 3139 - 3143 (1993)
34cf. our theory of the mesoscopic metallic character of polyaniline and ICPs in general: [7]
35R. Cahn, P. Hansen, E. Kramer, eds. "Materials Science and Technology", vol 12; Verlag Chemie 1993
36for more details, B. Wessling, in: R. Elsenbaumer, J. Reynolds, T.Skotheim (eds.) Handbook of Conducting Polymers, Marcel Dekker, in press
37the concentration at which a log(conductivity) vs. concentration plot has its curve inflection point
38from our non-equilibrium theory of dispersion in heterogeneous polymer systems it is understandable, that smaller particles are not possible in polymeric media, as the polymer matrix has to wet the particles being dispersed, which cannot be performed on a surface with such a small radius that, e.g. 10 nm particles would have
39a summary of still actively proposed arguments for this opinion can be found in
- J. Chien, "Polyacetylene", Academic Press 1984
- H. Shirakawa, Y. Zhang, T. Okuda, K. Sakamaki, K. Akagi, Synthetic Met. 65 (2-3), 93 - 102 (1994) and other articles in this issue
40I started this debate with publishing the first comparison of a TEM showing fibrillar polyacetylene and a SEM taken from the same sample, showing a globular morphology, cf. B. Wessling, Makromol Chem. 185, 1265 - 1275 (1984)
41N. Theophilou, D. Swanson, A. MacDiarmid, J. Manotvani, B. Annis, A. Epstein, in: H. Kuzmany, M. Mehring, S. Roth (eds.) "Electronic Properties of Conjugated Polymers III", Springer Series in Solid State Science 91 (1989), 14-18
42Synthetic Metals 65 (2-3) 91 - 262 (1994)
43Y. Liao, K. Kwei, K. Levon, Macromol. Chem. Phys. 196, 3107 - 3116 (1995)
44Macromol. Rapid Commun. 16, 393 - 397 (1995)
45L. Dai, J. White, J. Polym Sci., B Polym. Phys. 31, 3 - 15 (1993)
46SAXS:
47P. Garrin, J. Aimé, D. Reibel, C. Mathis, Synthetic Metals 51, 37 - 44 (1992)
48SANS:
49M. Aldissi, L. Dai, J. Kerr, R. Thomas, J. White, Synthetic Met. 28 (3), D69 (1989)
50G. Heffner, D. Pearson, Synthetic Metals 44, 341 - 347 (1991)
51also R. Elsenbaumer [1] and L. Shacklette [3, and personal communication] always observed "insoluble" portions and precipitates independant from the concentration range they worked in
52which means nothing less than there is no dilution effect resulting in a more complete dissolution, in other words: this is not a true solution, but a nice dispersion!
53which means no more than they had submicron particles - not visible by eye or microscope - responsible for the transparent coloured "solution" and bigger particles which were visible; when the particle size was small enough, than the critical gelation concentration was very low, cf. 5. 1. 3.
54tetrabutylammonium-p-toluenesulfonate
55R. Gregory, International Conference on Science and Technology of Synthetic Metals 1996, Snowbird (Salt Lake City, US), Synthetic Met. in press
56DMPU:
57P. Edwards, Acc. Chem. Res. 15, 87 - 93 (1982)
58B. Wessling, R. Hiessgen, D. Meissner, Acta Polymer. 44, 132 - 134 (1993)
59E. Domalski, E. Hering, J. Phys. Chem. Ref. data 22 (4), 1993, table 2, p. 866ff
60 Y. Cao, A. Heeger, Synthetic Met. 52, 193 - 200 (1992)