4482
I.S. Chung et al. / Polymer 51 (2010) 4477e4483
4. Conclusions
The nitro leaving group activated by trifluoromethyl group at
P1
P2
P3
meta position undergoes SNAr reaction quantitatively. The
quantum mechanical calculation for the energy state suggests that
the nitro displacement reaction is an energetically favorable
process. High molecular weight poly(arylene ether)s were prepared
from
2,20-bis(trifluoromethyl)-4,40-dinitro-1,10-biphenyl
with
several bisphenols. The synthesized polymers were amorphous and
dissolved well in a wide range of organic solvents regardless of the
position of trifluoromethyl pendent groups. They showed good
thermal stability as well as low refractive index and birefringence.
0
100
200
Temperature (oC)
300
400
Acknowledgment
Fig. 4. DSC curves of the polymers (Heating rate: 10 ꢀC/min, in N2 flow).
This work was supported by the National Research Foundation
of Korea through NRL (R0A-2008-000-20121-0) and ERC (R11-
2007-050-04001-0), Nano/Bio Science and Technology Program
(2005-01321, MEST, Korea), and the KRIBB Research Initiative
Program.
Thermal properties of the poly(arylene ether)s were evaluated
by TGA and DSC, and the results are summarized in Table 3.
Thermal analyses show that the polymers have high thermal
stability. Dynamic TGA shows 5% weight loss occurred for P1, P2,
and P3 at 493, 481, and 502 ꢀC in nitrogen, and 451, 428, and 463 ꢀC
in air, respectively. None of the poly(arylene ether)s showed crys-
tallization or melt transition in DSC measurement. The Tgs of the
polymers depends on the structure of bisphenol comonomer unit
(Fig. 4.). The Tgs of P1, P2, and P3 are 176, 181, and 199 ꢀC, respec-
tively. The Tg of P3 approaches that of PPOÔ (Tg ¼ 210 ꢀC [50]) even
though they do not have any pendent group near the ether linkage.
P1 display a Tg comparable to that of the poly(arylene ether) made
from bisphenol A and 4,40-dibromobiphenyl by Ullmann conden-
sation (Tg ¼ 166 ꢀC [51], 175 ꢀC [52]). It seems that the presence of
two trifluoromethyl groups appears to have minimal effect on Tg in
this case. However, while the Tg of P3 are comparable to that of the
poly(arylene ether) made from 3,30-bis(trifluoromethyl)-4,40-dini-
trobiphenyl and 4,40-biphenol, P1 and P2 display about 10 ꢀC
higher Tgs than those of the poly(arylene ether) from 3,30-bis(tri-
fluoromethyl)-4,40-dinitrobiphenyl with bisphenol A or bisphenol
AF (Tg ¼ 167 ꢀC [27]).
References
[1] Cotter RJ. In: Cotter RJ, editor. Engineering plastics: a handbook of polyaryl
ethers. Amsterdam: Gordon and Breach Publishers; 1995. p. 1e52.
[2] Theil F. Angew Chem Int Ed 1999;38:2345e7.
[3] Kricheldorf HR. In: Kricheldorf HR, editor. Handbook of polymer synthesis.
New York: Marcel Dekker; 1992. p. 545e615.
[4] Mati S, Mandal B. Prog Polym Sci 1986;12:111e53.
[5] Chung IS, Eom HJ, Kim SY. Polym Bull 1998;41:631e7.
[6] Labadie JW, Hedrick JL, Ueda M. In: Labadie JW, Hedrick JL, editors. Step
growth polymers for high-performance materials, new synthetic method (ACS
symposium Series 624). Washington, D.C: ACS; 1996. p. 210e25.
[7] Bunnett JF, Zahler RE. Chem Rev 1951;49:273e412.
[8] Bartoli G, Todesco PE. Acc Chem Res 1977;10:125e32.
[9] Terrier F. Nucleophilic aromatic displacement: the influence of the nitro
group. New York: VCH Publishers; 1991 [chapter 1].
[10] Bartoli G, LaTrofa A, Naso F, Todesco PE.
J Chem Soc Perkin Trans I;
1972:2671e2.
[11] Kornblum N, Cheng L, Kerber RC, Kestner MM, Newton BN, Pinnick WP, et al.
J Org Chem 1976;41:1560e4.
[12] Idoux JP, Madenwald ML, Garcia BS, Chu DL, Gupton JT.
1985;50:1876e8.
J Org Chem
In-plane and outeof plane refractive indices (nxy and nz) of the
polymers were measured using a prism coupling waveguide tech-
nique with a laser beam having 632.8 nm wavelength (474.58 THz),
and the results are summarized in Table 5. All of the synthesized
polymers show refractive indices (nav) in the range of 1.592e1.624
[13] Tamai S, Yamaguchi K, Ohta M. Polymer 1996;37:3683e92.
[14] Eastmond GC, Paprotny J. J Mater Chem; 1997:1321e6.
[15] Hawker CJ, Chu F. Displacement of the fluorine-leaving groups activated by
ketone and sulfone group at the meta position was utilized in the synthesis of
hyperbranched polymers that does not require complete conversion.
Macromolecules 1996;29:4370e80.
[16] Himmelberg P, Fossum E.
J
Polym Sci Part
A
Polym Chem
with low birefringence (
a material at optical frequencies can be estimated from the
refractive index n according to Maxwell’s equation,
y n2. The
value at 1 MHz has been evaluated as
y 1.10 n2av, including an
additional contribution of approximately 10% from the infrared
absorption [53]. The values estimated from average refractive
D) below 0.006. A dielectric constant (3) of
2005;43:3178e87.
[17] Beek Dv, Fossum E. Recently, displacement of the fluorine-leaving
groups activated by ketone and sulfone group at the meta position was
utilized in the synthesis of linear polymers. Macromolecules
2009;42:4016e22.
[18] Kaiti S, Himmelberg P, Williams J, Abdellatif M, Fossum E. Macromolecules
2006;39:7909e14.
3
3
3
3
[19] Labadie JW, Hedrick JL. Macromolecules 1990;23:5371e3.
[20] Kim SY, Labadie JW. Polym Prepr (Am Chem Soc Div Polym Chem) 1991;32
(1):164e5.
[21] Banerjee S, Maier G, Burger M. Macromolecules 1999;32:4279e89.
[22] Banerjee S, Maier G. Chem Mater 1999;11:2179e84.
[23] Maier G. Prog Polym Sci 2001;26:3e65.
[24] Lee MS, Kim SY. Macromol Rapid Commun 2005;26:52e6.
[25] Banerjee S, Komber H, Häussler L, Voit B. Macromol Chem Phys
2009;210:1272e82.
[26] Ghosh A, Banerjee S, Komber H, Lederer A, Häussler L, Voit B. Macromolecules
2010;43:2846e54.
indices of the resulting polymer films were in the range of
2.81e2.90. The low dielectric constants may be attributed to the
existence of the trifluoromethyl groups in the main chain.
Table 5
Refractive indices of the synthesized polymers.a
b
c
d
Polymer
nxy
nz
nav
De
3f
dg
(mm)
P1
P2
P3
1.6210
1.6030
1.6238
1.6184
1.5917
1.6194
1.6201
1.5992
1.6223
0.0026
0.0059
0.0044
2.89
2.81
2.90
5.8
4.3
4.1
[27] Carter KR, Kim SY, Labadie JW. Polym Prepr (Am Chem Soc Div Polym Chem)
1993;34(1):415e6.
[28] Park SK, Kim SY. Macromolecules 1998;31:3385e7.
[29] Lee HS, Kim SY. Macromol Rapid Commun 2002;23:665e71.
[30] Kim YJ, Chung IS, Kim SY. Macromolecules 2003;36:3809e11.
[31] Lee MS, Kim SY. Macromolecules 2005;38:5844e5.
[32] Kim YJ, Kakimoto M, Kim SY. Macromolecules 2006;39:7190e2.
[33] Hougham G. In: Hougham G, Cassidy PE, Johns K, Davidson T, editors. Fluo-
ropolymers (Part 2). New York: Plenum Press; 1999. p. 233e76.
[34] Chung IS, Kim SY. Macromolecules 2000;33:3190e3.
a
Measured at 632.8 nm (474.58 THz).
nxy: In-plane refractive index.
nz: Out-of plane refractive index.
b
c
d
e
f
nav: Average refractive index (nav ¼ (2 nav þ nav)/3).
D
: Birefringence (
D
¼ nxy ꢁ nz).
Dielectric constant estimated from the refractive index:
Film thickness.
3
y 1.10 n2av
.
g