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Materials Research

Print version ISSN 1516-1439On-line version ISSN 1980-5373

Mat. Res. vol.4 no.3 São Carlos July 2001

http://dx.doi.org/10.1590/S1516-14392001000300005 

Chirality and Helicity of Poly-Benzyl-L-Glutamate in Liquid Crystals and a Wave Structure that Mimics Collagen Helicity in Crimp

Benedicto de Campos Vidal*, Maria Luiza Silveira Mello

Department of Cell Biology, Institute of Biology, UNICAMP, 
13083-970 Campinas - SP, Brazil

*e-mail: vidal@unicamp.br

Received: November 18, 2000; Revised: June 23, 2001

 

Ideal biocompatible polymers must show a mimetic superstructure with biological supra-organization. Collagen-rich structures like tendons and ligaments are materials with various levels of order, from molecules to bundles of fibers, which affect their biomechanical properties and cellular interactions. Poly-benzyl-L-glutamate (PBLG) displaying helicity was used here to test the development of wave-like structures as those occurring in collagen fibers. Birefringence of PBLG under various crystallization conditions was studied with a l/4 compensator according to Sénarmont. Qualitative observations were plainly sufficient to conclude that the PBLG fibrils were supra-organized helically as a chiral object. During crystallization stretched PBLG formed a helical superstructure with characteristic striation resembling waves (crimp). Supported by optical anisotropy findings, a twisted grain boundary liquid crystal type is proposed as a transition phase in the formation of the PBLG chiral object. A similarity with the wavy organization (crimp) of collagen bundles is proposed.

Keywords: poly-benzyl-L-glutamate, wave-like superstructure, liquid crystal, optical anisotropy

1. Introduction

Many types of molecules have been studied for their possible use as thin films with polar order and piezo-pyroelectrical properties, particularly in photo-optical and electromagnetic applications and in the imaging of spatially resolved chemical libraries1-7. The most important properties in producing these supramolecular constructs are their mesophasic characteristics of self-assembly and chirality. These make it possible to examine the structure-function relationships in depth, particularly the relationship between optical characteristics, molecular order and the various types of birefringence.

The chirality of certain macromolecules allows the formation of helical superstructures6,8. Actually, non-chiral molecules can also generate chiral objects, provided that polar order and geometry of such molecules are present, e.g. rod-like/banana-like molecules are required to construct a chiral layer, the chirality of the layer acting as a chiral object itself that can in turn produce a helical superstructure9.

Atomic force microscopy suggested that collagen molecules exist as a chiral construct in collagen bundles10,11. To study similarities with collagen, the use of poly-benzyl-L-glutamate (PBLG) as a model (a reducionist approach) could shed some light to this question.

The polypeptide polyglutamic acid and its benzyl ester, poly-benzyl-L-glutamate(PBLG), have been used as a model for studying polar order, self-assembly, helicity, piezo-pyroelectric properties and for determining the conditions that lead to pyro-piezoelectricity2,12,13. It has been demonstrated that the superstructure of PBLG fibers has crystalline and textural birefringence14. Based on these data it is possible to determine that 58.8% of the total birefringence was accounted by crystalline birefringence. These properties are important when seeking to correlate the presence of waves (crimp) in the superstructure of PLBG with the molecule’s chirality and order.

In this study, mesophase chiral polymers of PBLG were examined for optical anisotropies which would suggest a helical supra-organization. The occurrence of wave-like structures (crimp) caused by mechanical stretching on the PBLG mesophase during crystallization are assumed to be related to the helical chiral PBLG characteristics and mimic those previously reported for collagen crimp15,16.

2. Material and Methods

A viscous solution of poly-(-benzyl-L-glutamate) (PBLG) was prepared by dissolving 100 mg of PBLG (Sigma (150-300)x103) in 1 mL of chloroform. Drops of this solution were placed on slides and left to dry. In some cases, the drops were placed close to each other so that their peripheries came into contact. In other cases, the drops were allowed to spread on the surface of bidistilled water on which they dried. Stretching the drops, while evaporating the chloroform, was done using 26G x 1/2" needles in order to obtain stretched fibers of various diameters.

Optical anisotropy was assessed using dry as well as Cargille oil-imbibed PBLG. A Zeiss-Pol photomicroscope was used. The l/4 mica plate Sénarmont compensator was used to determine the birefringence signal of the PBLG fibers and detect their orientation in the PBLG superstructures, by placing the Sénarmonts compensator gamma (direction of vibration) parallel to the analyser azimuth (known also as plane of light polarization, PLP). In this case no birefringence of the compensator is introduced. The function of the compensator is to transform helically polarized light emerging from the object into a plane polarized light, which will be compensated by rotating the analyser. The compensation produced quantitative data not used for this work since the qualitative results were plainly sufficient to allow description of the events and to support inferences.

3. Results

After drying on slides and on the surface of water, the PBLG solution formed fibrillar films that showed positive birefringence as determined by Sénarmonts compensation.

Isolated drops as well as drops touching each other showed rings of different superstructures, from the periphery directed towards the center of the drop. At the drop periphery or at touching surfaces, a thin fibrillar membrane was seen, the fibrils of which were detected by birefringence and formed a frame structure as shown by using Sénarmont’s compensator. The fibrils were intertwined helically at various levels, giving rise to a hierarchy of fibers with increased degrees of packing towards the center of the drop. Details of the coiled coils were observable with Sénarmont’s compensation. The various levels of rings exhibited different degrees of helically intertwined fibrils, fibers and bundles of fibers, all of which produced varying degrees of compactness. A very compact ring of fibers was formed in the center of the drop, because of the higher concentration of PBLG (Fig. 1).

 

 

Tubular, columnar or cord-like structures were formed when the periphery of two drops touched one another. The resulting birefringent layers were similar (but not identical) to those previously described17,18 and resembled DNA cords19, being almost parallel one to another along the area of contact between them (Figs. 1 and 2). The direction and orientation of the fibrils in these bands were established by determining the birefringence characteristics. The cord-like structures exhibited antiparallel position-orientation in which one cord-like structure had its birefringence compensated, while the other maintained its birefringence (Figs. 1 and 2). Internally, each cord showed an alternating compensation of the birefringence of the fibrillar components seen as a striated-like aspect since compensated and non-compensated birefringent fibrillar striations alternate (Fig. 2).

 

 

Stretching PBLG liquid crystals during drying revealed a distinct bright birefringence with a wave appearance (crimp) demonstrated with the compensator (Fig. 3A and 3B), indicating the alternating directions of the molecular order of the fibrillar superstructure. The bands also showed areas of fusion essential for maintaining the fitness of the wave (crimp) superstructure.

 

 

4. Discussion

Chiral molecules forming a molecular assembly have been reported to generate helical superstructures that may be related to the Cotton effect1. The report of Akagi and co-workers1 is a striking instance of correlation among chirality, birefringence striae or bands and fibrous helical morphologies detected by scanning electron microscopy. Polyglutamic acid in an -helix conformation and PLGA-acridine orange complexes in solution also exihibit a Cotton effect that is comparable to the optical anisotropic properties of PLGA-toluidine blue complexes20.

The results of the present study are in agreement with the report quoted above1, and clearly establish the hierarchy of helicity from fibrillar membrane structures to twisted coils and then in a final rope or tube-like morphology that reflects helical layers corresponding to helical periods. The stretching caused the formation of striae (bands) as if an helical spring was stretched. These structures form an ordered network superstructure with fibrillar characteristics which is in agreement with reports of a twist-grain-boundary (TGB) phase exhibiting a helical twist21-23. TGB phases often occur between smectic and cholesteric or isotropic phases23.

The observations in the present study were based on crystallized dry PBLG in which a concentration gradient was formed by rapid chloroform evaporation from the drop meniscus on the surface of the slides. The mechanisms involved in the formation of the rope-like superstructure in the regions where drops contacted at their periphery may be similar to those occurring at cell walls during the formation of equispaced lines parallel to the sides of the cells18. Whatever the mechanism, intermolecular forces of the self-assembly process, polarity and the helical geometry of the molecules must be considered.

The supramolecular organization involved is the source of textural (form or structural) birefringence, and obeys physical refraction and birefringence theories24-27. The textural aspect depends on the molecular geometry, on the partial volume and/or the aggregation and orientation of the molecules contained in the fibers or bundles. The exhibited textural/form birefringence14 appears by virtue of the helical arrangement of the constituent molecules21 and their geometry. The wave-like structure appearing under stress/strain is related to the elastic phase behaviour of a TGB, including zig-zag defect formation28. Accurate, controlled conditions, established a relationship between shear and the striations formed perpendicular to the direction of shear29. The results obtained here agreed with the latter study. The differences between these two reports may reflect the tougher conditions of shear, higher concentration of PBLG, type of solvent, the conditions of chloroform evaporation, and the use of a fine needle to stretch the solution during solvent evaporation.

The piezoelectric effect reported for PBLG films, considered as being a prototype material13 derives from the characteristics and properties of the ordered superstructure described above. The organization of the PBLG molecules resembles that of the helical, wave morphology of collagen bundles (crimp)15,16. Atomic force microscopy has confirmed the hierarchical supramolecular organization of collagen in a helical coil of coils3,11.

Acknowledgments

This investigation was supported by grants of Brazilian research agencies CNPq and FAPESP.

References

1. Akagi, K.; Piao, G.; Kaneko, S.; Sakamaki, K.; Shirakawa, H.; Kyotani, M. Science, v. 282, p. 1683-1686, 1998.        [ Links ]

2. Athenstaedt, H. Ann. N.Y. Acad. Sci. v. 238, p. 7-25, 1974.        [ Links ]

3. Cornelissen, J.J.L.M.; Fisher, M.; Sommerdick, N.A.J.M.; Nolte, R.J.M. Science, v. 280, p. 1427-1430, 1998.        [ Links ]

4. Gupta, V.K.; Skaife, J.J.; Dubrovsky, T.B.; Abbot, N.L. Science, v. 279, p. 2077-2080, 1998.        [ Links ]

5. Haller, I. J. Am. Chem. Soc., v. 100, p. 8050-8055, 1978.        [ Links ]

6. Jenekhe, S.A.; Chen, X.L. Science, v. 279, p. 1903-1906, 1998.        [ Links ]

7. Whitesell, J.K.; Chang, H.K. Science, v. 261, p. 73-76, 1993.        [ Links ]

8. Drzaic, P.S. Liq. Cryst., v. 26, p. 623-627, 1999.        [ Links ]

9. Heppke, G.; Moro, D., Science, v. 279, p. 1872-1873, 1998.        [ Links ]

10. Baranauskas, V.; Vidal, B.C.; Parizotto, N.A. Appl. Biochem. Biotech., v. 69, p. 91-96, 1998.        [ Links ]

11. Vidal, B.C.; Baranauskas, V.; Parizotto, N.A. 5th International Congress on Cell Biology, Madrid, p. 64, July/1992.        [ Links ]

12. Fukada, E., Ann. N.Y. Acad. Sci., v. 238, p. 7-24, 1974.        [ Links ]

13. Jaworeck, T.; Neher, D.; Wegner, G.; Wiringa, R.H.; Schouten, A.J. Science, v. 279, p. 57-60, 1998.        [ Links ]

14. Vidal, B.C. Cell. mol. Biol., v. 32, p. 109-112, 1986.        [ Links ]

15. Vidal, B.C. C.R. Acad. Sci. Paris, Life sciences, v. 318, p. 173-178, 1995.        [ Links ]

16. Vidal, B.C. C.R. Acad. Sci. Paris, Life sciences, v. 318, p. 831-836, 1995.        [ Links ]

17. Hartshorne, N.H. The Microscopy of Liquid Crystals, Microscope Publications Ltd., London, 1974.        [ Links ]

18. Robinson, C. Tetrahedron, v. 13, p. 219-234, 1961.        [ Links ]

19. Livolant, F. J. Phys., v. 48, p. 1051-1066, 1987.        [ Links ]

20. Vidal, B.C. Histochemie, v. 30, p. 102-107, 1972.        [ Links ]

21. Goodby, J.W.; Waugh, M.A.; Stein, S.M.; Chin, E.; Pindak, R.; Patel, J.S. Nature, v. 337, p. 449-452, 19899        [ Links ]

22. Isaert, N.; Navailles, L.; Barois, P.; Nguyen, H.T. J. Phys. II France, v. 4, p. 1501-1518, 1994.        [ Links ]

23. Li, M-N.; Nguyen, H.T.; Sigaud, G. Liq. Cryst., v. 20, p. 361-365, 1996.        [ Links ]

24. Cassim, J.Y.; Taylor, E.W. Biophys. J., v. 5, p. 532-552, 1965.        [ Links ]

25. Cassim, J.Y.; Tobias, P.S.; Taylor, E.W. Biochim. Biophys. Acta, v. 168, p. 463-471, 1968.        [ Links ]

26. DeVoe, H. J. Chem. Phys., v. 41, p. 393-400, 1964.        [ Links ]

27. DeVoe, H. J. Chem. Phys. v. 43, p. 3199-3208, 1965.        [ Links ]

28. Radcliffe, M.; Brostrom, M.L.; Epstein, K.A.; Rappaport, A.G.; Thomas, B.N.; Shao, R.; Clark, N.A. Liq. Cryst., v. 26, p. 789-794, 1999.        [ Links ]

29. Kiss, G.; Porter, R.S. Mol. Cryst. Liq. Cryst., v. 60, p. 267-280, 1980.        [ Links ]

 

FAPESP helped in meeting the publication costs of this article

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