b Faculty of Science, Universiti Tunku Abdul Rahman, Jln Universiti, Bandar Barat, Kampar 31900, Malaysia;
c Centre for Biodiversity Research, Universiti Tunku Abdul Rahman, Jln Universiti, Bandar Barat, Kampar 31900, Malaysia;
d Liquid Crystal Research Laboratory, School of Chemical Sciences, Universiti Sains Malaysia, Minden 11800, Malaysia;
e Department of Materials Science & Engineering, National Chiao Tung University, Hsinchu 300, Taiwan, China
1. Introduction
The electronic conducting behaviours of liquid crystals (LCs) have received tremendous attention since the discovery of high hole mobility in the hexagonal columnar phase of hexapenthyloxytriphenylene [1, 2, 3, 4, 5]. Recently,calamitic LCs became another potential material for applications in electronic devices due to the presence of some ordered mesophases,such as SmA,SmC,SmB and SmE. The two-dimensional (2D) arrangement (layers) in smectics is more tolerant with regard to defects than the onedimensional (1D) ordered discotic columns,thus resulting in an improved performance [6]. The electronic conducting behaviour of calamitic LCs was first examined in the SmA phase of 2-phenylbenzothiazole derivatives. Existence of a layer(ed) structure in all smectic LCs induces π-π stacking interactions which can facilitate the hopping of charge carrier mobility [7, 8, 9].
In our previous studies,we successfully synthesized and isolated a series of homologues of smectic LCs containing the benzothiazole moiety [10, 11, 12, 13]. Incorporation of benzothiazole ring into calamitic LCs,as the mesogenic core,enabled them to easily exhibit mesophase transitions due to the more polarizable nature of the heteroatoms,sulfur and nitrogen [14]. In this paper,we report another new homologous series of benzothiazole liquid crystals (Scheme 1). Three core units (one benzothiazole and two phenyl rings) were connected via a Schiff base and ester linkers which can increase the molecular broadness and anisotropy.
Download:
|
|
Scheme 1. Synthetic route for the target compounds. (i) EtOH,(ii) CnH2n+1Br,K2CO3, CH3COCH3,(iii) H2O:EtOH (1:1),KOH,conc. HCl,(iv) DCC,DMAP,DCM,DMF. Yield of C2H5O-7BSPEP (29%),C2H5O-8BSPEP (33%),C2H5O-9BSPEP (37%),C2H5O-10BSPEP (41%),C2H5O-12BSPEP (48%),and C2H5O-14BSPEP (55%). |
The synthetic protocol towards (producing/creating) the title compounds,6-ethoxy-2-[4-(4-alkyloxybenzoyloxy)benzylidenamino]-benzothiazoles (C2H5O-nBSPEP,where n = 7,8,9,10,12, 14) is illustrated in Scheme 1. 2-Amino-6-ethoxybenzothiazole was condensed with 4-hydroxybenzaldehyde upon refluxing in ethanol for 3 h to yield intermediate A [11]. Etherification of ethyl-4-hydroxybenzoate in acetone with the appropriate 1-bromoalkane and acidification using concentrated HCl produced intermediate B [15]. Intermediates A and B were then subjected to Steglich esterification with the appropriate fatty acid in the presence of DCC and DMAP according to previously reported procedures [16] to yield title compounds C2H5O-nBSPEP. All the crude products were purified by repeated recrystallization using ethanol until constant melting points were obtained. The yields of the final products were between 29% and 55% (Scheme 1). Structural elucidation of the title compounds was carried out via elemental analysis,FT-IR,NMR, and EI-MS spectroscopic techniques [17].
3. Results and discussionThe liquid crystalline textures of the title compounds were observed by polarizing optical microscope and phase identification was made by comparing the observed textures with those reported in the literature [18, 19].
Transition temperatures and corresponding enthalpy changes were determined using a differential scanning calorimeter and the data tabulated in Table 1.
Referring to Table 1,all synthesized compounds exhibited both liquid crystal phase and nematic phase. A higher ordered SmC phase emerged from dodecyloxy derivatives,which contain a relatively longer flexible chain. Due to the thermally unstable properties of these compounds,all the transition temperatures can be only obtained from the heating cycle in DSC analysis. This is due to the partial decomposition of the compounds during heating,a phenomenon also reported in the work of Wei et al. [20].
Representative optical photomicrographs of C2H5O-12BSPEP are shown in Fig. 1. The presence of the nematic phases in C2H5O-12BSPEP is evidenced by a typical marble-like texture upon cooling the compound from the isotropic liquid phase. Upon further cooling the nematic phase to a lower temperature,a higher ordered SmC phase formed and exhibited the transition bar textures which in turn confirmed the conversion from the nematic to the SmC phase (Fig. 1b) [21].
Download:
|
|
Fig. 1. Optical photomicrographs (100×) of (a) nematic phase showing marble-like texture and (b) SmC phase exhibiting typical transition bar texture in C2H5O-12BSPEP. |
A plot of transition temperatures against the number of carbons in the alkoxy chain during the heating cycle is shown in Fig. 2. Firstly,it is evident that both melting (Cr-SmC/N) and clearing (N-I) points were greatly influenced by the length of alkoxy chain in the compounds. The fluctuation of melting and clearing points observed in C7 to C10 compounds was due to the odd-even effect. The odd-even effect can be explained by the fact that the extra carbon causes the chain to deviation from the linear structure,and this deviation from the linearity of the structure causes a reduced melting or clearing point. This fluctuation was commonly investigated for short chain derivatives in a homologous series [22, 23, 24, 25]. Secondly,a higher ordered SmC phase was observed only in the homologues with relatively longer chain members,C12 and C14 in this case. It can be understood that a longer terminal alkoxy chain may favour the lamellar arrangement in the smectic layer structure due to higher Van der Waals interactions and the possibilities of intertwining between alkoxy chains. Lastly,the nematic phase range (ΔN) was reduced and the SmC phase range (ΔSmA) was increased as the chain length increased. The increasing Van der Waals attractive forces provide stronger lateral attractive interactions,which in turn,resulted in formation of layer packing.
Download:
|
|
Fig. 2. Phase behaviour of C2H5O-nBSPEP. |
Conclusively,all the synthesized compounds exhibited liquid crystal behaviour in which nematic and SmC phases were observed. The length of the terminal alkoxy chain greatly affects properties,such as melting and clearing temperatures,and liquid crystal phase ranges. In our future work,molecular modifications on this homologous series will be planned in order to yield liquid crystal compounds with high thermal stability.
AcknowledgmentThe authors would like to thank Universiti Tunku Abdul Rahman for the financial supports and research facilities.
[1] | D. Adam, F. Closs, T. Frey, et al., Transient photoconductivity in a discotic liquid crystal, Phys. Rev. Lett. 70 (1993) 457-460. |
[2] | M.R. Huang, X.G. Li, J. Wang, Liquid crystalline polyaniline and its derivatives, Tongji Daxue Xuebao 31 (2003) 848-852 (in Chinese). |
[3] | X.G. Li, M.R. Huang, W. Duan, Y.L. Yang, Novel multifunctional polymers from aromatic diamines by oxidative polymerizations, Chem. Rev. 102 (2002) 2925-3030. |
[4] | X.G. Li, Q.F. Lu, M.R. Huang, Self-stabilized nanoparticles of intrinsically conducting co-polymers from 5-sulfonic-2-anisidine, Small 4 (2008) 1201-1209. |
[5] | X.G. Li, M.R. Huang, Facile optimal synthesis of inherently electroconductive polythiophene nanoparticles, Chem. Eur. J. 15 (2009) 6446-6455. |
[6] | W. Pisula, M. Zorn, J.Y. Chang, K. Mullen, R. Zentel, Liquid crystalline ordering and charge transport in semiconducting materials, Macromol. Rapid Commun. 30 (2009) 1179-1202. |
[7] | B.P. Chandra, N. Periasamy, J.N. Das, Triboluminescence, a new tool to investigate fracture-initiation time of crystals under stress, Pramana 8 (1977) 395-401. |
[8] | M. Funahashi, J. Hanna, Fast hole transport in a new calamitic liquid crystal of 2-(40-heptyloxyphenyl)-6-dodecylthiobenzothiazole, Phys. Rev. Lett. 78 (1997) 2184-2187. |
[9] | A. Ohno, A. Haruyama, K. Kurotaki, J. Hanna, Charge-carrier transport in smectic mesophases of biphenyls, J. Appl. Phys. 102 (2007) 083711. |
[10] | S.T. Ha, T.M. Koh, G.Y. Yeap, et al., Synthesis and mesomorphic properties of 2-(4-alkyloxyphenyl)benzothiazoles, Mol. Cryst. Liq. Cryst. 506 (2009) 56-70. |
[11] | S.T. Ha, T.M. Koh, H.C. Lin, et al., Heterocyclic benzothiazole-based liquid crystals: synthesis and mesomorphic, Liq. Cryst. 36 (2009) 917-925. |
[12] | S.T. Ha, T.M. Koh, S.T. Ong, Y. Sivasothy, Synthesis and mesomorphic behavior of benzothiazole-based liquid crystals having terminal methoxyl group, Chin. Chem. Lett. 20 (2009) 1449-1452. |
[13] | S.T. Ha, T.M. Koh, G.Y. Yeap, et al., Mesogenic Schiff base esters with benzothiazole core: synthesis and phase transition studies, Phase Transitions 83 (2010) 195-204. |
[14] | L.L. Lai, C.H. Wang, W.P. Hsien, H.C. Lin, Synthesis and characterization of liquid crystalline molecules containing the quinoline unit, Mol. Cryst. Liq. Cryst. 287 (1996) 177-181. |
[15] | O.N. Kadkin, H. Han, Y.G. Galyametdinov, Synthesis, computational modelling and liquid crystalline properties of some [3]ferrocenophane-containing Schiff's bases and β-aminovinylketone: molecular geometry-phase behaviour relationship, J. Organomet. Chem. 692 (2007) 5571-5582. |
[16] | G.Y. Yeap, S.T. Ha, P.L. Boey, et al., Synthesis and mesomorphic properties of Schiff base esters ortho-hydroxy-para-alkyloxybenzylidene-para-substituted anilines, Mol. Cryst. Liq. Cryst. 452 (2006) 73-84. |
[17] | Analytical and spectroscopic data for the representative compound C2H5O-9BSPEP: EI-MS m/z (rel. int. %): 544 (22) [M+], 247 (100), IR vmax (KBr, cm-1): v 3056 (C-H aromatic); 2922, 2851 (C-H aliphatic); 1740 (C5O ester); 1609 (C5N thiazole), 1273 (C-O, aromatic ether) 1H NMR (400 MHz, CDCl3): d 0.9 (t, 3H, J = 6.6 Hz, CH3-), 1.3 (m, 10H, CH3-(CH2)5-(CH2)3-O-), 1.4 (t, 3H, J = 6.8 Hz, CH3-CH2-O-), 1.5 (p, 2H, J = 6.1 Hz,-CH2-CH2-CH2-O-), 1.8 (p, 2H, J = 7.1 Hz,-CH2-CH2-O-), 4.0 (t, 2H, J = 6.6 Hz,-CH2-O-), 4.1 (t, 2H, J = 7.1 Hz, CH3-CH2-O-), 7.0 (d, 2H, J = 8.8 Hz, Ar-H), 7.1 (d, 1H, J = 9.0 Hz, Ar-H), 7.3 (s, 1H, Ar-H), 7.4 (d, 2H, J = 8.6 Hz, Ar-H), 7.9 (d, 1H, J = 8.8 Hz, Ar-H), 8.1 (d, 2H, J = 8.6 Hz, Ar-H), 8.2 (d, 2H, J = 8.8 Hz, Ar-H), 9.0 (s, 1H,-N5CH-); 13C NMR (100 MHz, CDCl3): δ 14.23 (CH3-), 14.94 (CH3-CH2O-), 15.01, 22.77, 26.07, 29.17, 29.35, 29.46, 29.61, 31.97 for methylene carbons (CH3-(CH2)8-), 64.18 (-CH2O-), 68.47 (CH3-CH2O-), 105.14, 114.50, 116.22, 121.06, 122.70, 123.85, 131.44, 132.50, 133.98, 135.93, 146.06, 154.91, 156.04, 157.18 for aromatic carbons, 163.88 (N=CH, Schiff base), 164.47 (N=C, thiazole), 169.20 (-COO-). Anal. calcd. for C32H36N2O4S: C, 70.56, H, 6.66, N, 5.14; Found: C, 70.48, H, 6.74, N, 5.03. |
[18] | D. Demus, L. Richter, Textures of Liquid Crystals, Verlag Chemie, New York, 1978. |
[19] | I. Dierking, Textures of Liquid Crystals, Wiley-VCH, Weinheim, 2003. |
[20] | Q. Wei, L. Shi, H. Cao, L.P. Wang, H. Yang, Synthesis and mesomorphic properties of two series of new azine-type liquid crystals, Liq. Cryst. 35 (2008) 581-585. |
[21] | M.A. Guillevic, M.E. Light, S.J. Coles, et al., Synthesis of dinuclear complexes of rhenium(I) as potential metallomesogens, J. Chem. Soc. Dalton Trans. 9 (2000) 1437-1445. |
[22] | P.A. Henderson, R.T. Inkster, J.M. Seddon, C.T. Imrie, Highly non-linear liquid crystal tetramers, J. Mater. Chem. 11 (2001) 2722-2731. |
[23] | G.Y. Yeap, T.C. Hng, D. Takeuchi, et al., Non-symmetric liquid crystal dimers: high thermal stability in nematic phases enhanced by thiophene-2-carboxylate moieties, Mol. Cryst. Liq. Cryst. 506 (2009) 134-149. |
[24] | A.K. Prajapati, N.L. Bonde, Mesogenic benzothiazole derivatives with methoxy substituents, J. Chem. Sci. 118 (2006) 203-210. |
[25] | A.K. Prajapati, N.L. Bonde, Mesogenic benzothiazole derivatives with a polar nitro substituent, Mol. Cryst. Liq. Cryst. 501 (2009) 72-85. |