H. Chen et al. / Polymer 52 (2011) 400e408
407
presence of the layered structures for P-AOLAxO6OPPOn polymers
Fig. 5). This is in good agreement with cholesterol initiated O-LLA
materials, which form layered phase reported by Samuel I. Stupp.
(
3.6. CD spectra of P-AOLAxO6OPPOn
All the CD spectra of P-AOLAxO6OPPOn materials showed
typical positive cotton effect, a peak can be observed for each
polymer around 210 nm, the absorption of C]O groups of O-LLA
2
ꢁ1
segments, with [
indicated that stable helical structure has formed for these poly-
mers because the [ ] value is comparative with any high Mw PLLA
q
] ¼ 4000e5000 deg*cm decimol (Fig. 6.). This
q
materials with good helical structure. The CD spectra give clear
evidence that the P-AOLAxO6OPPOn materials may show strong
optical rotation power if they are proper treated to form ordered
films. Considering that LC materials can self-organized easily to
form ordered materials, the study of P-AOLAxO6OPPOn may be
used as optical materials in the future.
4. Conclusions
Series of mesogenic biphenol derivatives with active HO-group
have been used as initiators successively to form Oligomeric L-LA
materials with controlled molecular weight by adjusting the feed
2
ratios by Ring-Opening Polymerization of LLA with SnOct catalyst.
Main Chain polymers P-AOLAxO6OPPOn were finally prepared by
freeradical polymerization of these polymerizable macromonomers
esters thatobtained byattaching acrylic grouptothese Oligomeric L-
LA materials correspondingly. These macromolecules can be
1
prepared with a controlled LLA length confirmed by H NMR and
GPC. All these materials can form good LC smectic phase from
a-crystal. The O-LLA segments are in helical structure and this makes
the resulting polymer materials good candidate of optical materials.
Fig. 6. Typical CD spectra of P-AOLAxO6OPPO4 and P-AOLAxO6OPPO8.
Acknowledgements
PLLA. The
c
c values are important for the preparation of layered
This work was financially supported by the National Natural
Foundation of China (No. 20304006) and Key Technologies R&D
Program of Shandong Province, China (No. 200810002017). The
authors also thank much for the kind help of Prof. Zaijun Lu of
ShandongUniversity for GPC measurements and kind discussions.
The authors thank the Prof. Minghua Liu, Dr. Penglei Chen (Institute
of Chemistry, ChineseAcademy of Sciences (CAS)).
phase, because the crystals of PLLA are often spherulites.
3.5. Phase behaviors of P-AOLAxO6OPPOn
X-Ray diffraction characterizations were performed to confirm
the LC phase structure which may exist in P-AOLAxO6OPPOn and
several were listed in Fig. 5. Peaks in the wide angle region, strong
ꢀ
ꢀ
ꢀ
one at 2
q
¼ 16.86 and those weak peaks at 2
q
¼ 19.05 , 22.46
References
(
(
corresponding to d ¼ 5.26 Å, 4.65 Å, 3.96 Å), were found to be the
110), (100), (203), (205) diffractions of a-form crystal of PLLA as have
[
[
1] Zhao YL, Shuai XT, Chen CF, Xi F. Chem Mater 2003;15:2836e43.
2] Goddard H, Kenneth KM, Sosely OS. Eur Pat Appl 1988;830866(A2):25.
been reported by Miyata [41,42]. This is rational result for PLLA
materials which formed -crystal from solution and bulk. This
implies that the LC phase of P-AOLAxO6OPPOn was apparently
formed from the melting of PLLA -crystals. Unfortunately, no
a
[3] Bhardwaj R, Blanchard J. Int J Pharm 1998;170:109.
[
[
4] Winet H, Bao JY. J Biomed Mater Res 1998;40:567.
5] Hedrick JL, Trollsas M, Hawker CJ, Atthoff B, Claesson H, Heise A, et al.
Macromolecules 1998;31:8691.
a
obvious peaks of layered structure were found by temperature
variable X-ray diffraction measurements without or with only short
time annealing, while samples after overnight annealing have peaks
appeared in small angle region. Because of the high molecular
weight, the chemical bonding attachment at both ends of PLLA
segments and the higher viscosity of P-AOLAxO6OPPOns, the
ordering of the PLLA segments to form mesophases was much
slower than those of common side chain Liquid Crystal Polymers and
also chol-LAxOH samples. Thus reasonable frozen mesophases
should exist after annealing overnight long and quenching to ice-
cold metal plate and be observed by X-Ray Diffraction measure-
ments. The weak peaks found at d ¼ 6.49 nm for P-AOLA40O6OPPO4
[6] Breitenbath A, Kissel T. Polymer 1998;39:3261.
[
[
[
7] Fujiwara T, Miyamoto M, Kimura Y, Sakurai S. Polymer 2001;42:1515.
8] Lee D, Teraoka I, Fujiwara T, Kimura Y. Macromolecules 2001;34:4949.
9] D’Angelo S, Galletti P, Maglio G, Malinconico M, Morelli P, Palumbo R, et al.
Polymer 2001;42:3383.
[10] Nijenhuis J, Grijpma DW, Pennings AJ. Macromolecules 1992;25:6419.
11] Kister G, Cassanas G, Vert M. Polymer 1998;39:267.
12] Degee P, Dubois P, Jerome R. Macromol Symp 1997;123:67.
[13] Leengslag JW, Pennings AJ. Makromol Chem 1987;188:1809.
[
[
[14] Spassky N, Wisniewski M, Pluta C, LeBorgne A. Macromol Chem Phys
1996;197:2627.
[
15] Okihara T, Tsuji M, Kawaguchi A, Katayama K, Tsuji H, Hyon SH, et al.
J Macromol Sci Phys 1991;B30:119.
[16] Miyata T, Masuko T. Polymer 1997;38:4003.
17] Green MM, Park JW, Sato T, Teramoto A, Lifson S, Selinger RLB, et al. Angew
Chem Int Ed 1999;38:3138e54.
18] Rowan AE, Nolte RJM. Angew Chem Int Ed 1998;37:63e8.
[
ꢀ
annealing at 80 C overnight and that at d ¼ 7.61 nm for
[
ꢀ
P-AOLA10O6OPPO8 annealing at 80 C overnight indicating the
[19] Nakano T, Okamoto Y. Chem Rev 2001;101:4013e38.