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Based on this relation and experimental results, intrinsic
birefringences of the polymers were obtained (Table 4).
copolymers with zero birefringence were in the range of
135–140 C.
ꢀ
The photoelastic birefringence versus the stress of the polymers
is shown in Figure 6. PMMA exhibited negative photoelastic bire-
fringence, and photoelastic birefringence constant C was approx-
imately ꢃ5.3 (TPaꢃ1). Its negative birefringence was shifted
to positive birefringence with an increase of TFPMI content.
Photoelastic coefficients of the copolymers are listed in Table 4.
ACKNOWLEDGMENTS
This research is supported by the Japan Society for the Promo-
tion of Science (JSPS) through its ‘‘Funding Program for World-
leading Innovative R&D on Science and Technology (FIRST
Program).’’
Figure 7 shows intrinsic birefringence and photoelastic coeffi-
cient of TFPMI-co-MMA as a function of content of MMA unit
in the copolymers. Those relations can be written as follows:
REFERENCES AND NOTES
1 Brydson, J. A. Plastic Materials; Butterworth Scientific:
London, 1982; p 376–377.
Poly(2,3,4-TFPMI-co-MMA):
2 Kine, B. B.; Novak, R. W. In Encyclopedia of Polymer Science
and Engineering, 2nd ed.; Mark, H. F., Ed.; Wiley: New York,
1986; Vol. 1, pp 234–235.
Dnor ¼ ꢃ0:18MMMA þ 13:13;
C ¼ ꢃ0:53MMMA þ 47:43:
(3)
(4)
3 Otsu, T.; Matsumoto, A.; Kubota, T.; Mori, S. Polym. Bull.
1990, 23, 43–50.
Poly(2,4,6-TFPMI-co-MMA):
4 Matsumoto, A.; Kubota, T.; Otsu, T. Macromolecules 1990,
23, 4508–4513.
Dnor ¼ ꢃ0:2MMMA þ 17:46;
C ¼ ꢃ0:74MMMA þ 69:03:
(5)
(6)
5 Otsu, T.; Tatsumi, A.; Matsumoto, A. J. Polym. Sci Polym.
Lett. Ed. 1986, 24, 113–117.
6 Matsumoto, A.; Kubota, T.; Otsu, T. Polym. Bull. 1990, 24,
459–466.
Here, MMMA is the content of MMA unit in the copolymers.
The ratios of 2,3,4-TFPMI/MMA for zero orientational bire-
fringence and zero photoelastic birefringence were calculated
to be 15/85 mol % (28/72 wt %) and 5/95 mol % (10/90 wt
%), respectively, by eqs 3 and 4. The intrinsic birefringence
and the photoelastic birefringence of poly(2,3,4-TFPMI) were
calculated to be 13 ꢂ 10ꢃ3 and 47 (TPaꢃ1) (Table 4).
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Phys. 1996, 35, 3896–3901.
The ratios of 2,4,6-TFPMI/MMA for zero orientational birefrin-
gence and zero photoelastic birefringence were calculated to
be 12/88 mol % (24/76 wt %) and 3/97 mol % (7/93 wt
%), respectively, by eqs 5 and 6. The intrinsic birefringence
and the photoelastic birefringence of poly(2,4,6-TFPMI) were
calculated to be 17 ꢂ 10ꢃ3 and 69 (TPaꢃ1) (Table 4).
These results show that 2,4,6-TFPMI unit exhibits higher ori-
entational and photoelastic birefringence effects than those
of 2,3,4-TFPMI.
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CONCLUSIONS
17 Tagaya, A.; Lou, L.; Ide, Y.; Koike, Y.; Okamoto, Y. Chin. Sci.
B, in press.
2,3,4- and 2,4,6-TFPMIs were synthesized and copolymerized
with MMA using AIBN as initiator in 1,4-dioxane or in bulk.
The glass transition temperatures of the copolymers were
high (133–195 ꢀC) depending on copolymer compositions.
The copolymers obtained were thermally stable. The orienta-
tional and photoelastic birefringences of copolymers of
TFPMIs and MMA were measured. The copolymers of MMA/
2,3,4-TFPMI would exhibit zero orientational and photoelas-
tic birefringences when the ratio of 2,3,4-TFPMI/MMA were
15/85 and 5/95 mol %, respectively. For the copolymers of
2,4,6-TFPMI/MMA, the ratios of copolymers with zero orien-
tational and photoelastic birefringences were determined to
be 12/88 and 3/97 mol %, respectively. The Tgs of these
18 Bruynes, C. A.; Jurriens, T. K. J. Org. Chem. 1982, 47,
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23, 4508–4513.
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18, 1410–1418.
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