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HAL Id: jpa-00210083

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Submitted on 1 Jan 1985

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Nematic 4-cyanophenyl esters incorporating a lateral fluorine atom

Hp. Schad, S.M. Kelly

To cite this version:

Hp. Schad, S.M. Kelly. Nematic 4-cyanophenyl esters incorporating a lateral fluorine atom. Journal

de Physique, 1985, 46 (8), pp.1395-1404. �10.1051/jphys:019850046080139500�. �jpa-00210083�

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1395

Nematic 4-cyanophenyl esters incorporating a lateral fluorine atom Hp. Schad and S. M. Kelly

Brown Boveri Research Center, CH-5405 Baden, Switzerland

(Reçu le 4 fevrier 1985, accepte le 28 mars 1985)

Résumé.

2014

Les propriétés diélectriques, diamagnétiques et élastiques de divers esters de fluoro-2 et fluoro-3 p-

cyanophényle ont été étudiées. Les esters sont dérivés des acides benzoiques, cyclohexacarboxyliques ou bicyclo- octancarboxyliques. Pour permettre la comparaison, les propriétés des esters non fluorés correspondants ont été

mesurées. Nous discutons du changement des propriétés des esters, soit qu’ils diffèrent par la composition du noyau de la partie acide ou par la position de l’atome de fluor. Les propriétés physiques dépendent largement de la pré-

sence et de la position de l’atome de fluor. Un de ces esters présente une très forte anisotropie diélectrique.

Abstract.

2014

We have investigated the dielectric, diamagnetic, and elastic properties of various 2-fluoro- and 3- fluoro-4-cyanophenyl esters. The esters are derivatives of benzoic, cyclohexane or bicyclooctane acids. For compari-

son we also measured the same properties of the corresponding non fluorinated esters. The change in the properties of the esters with either variation of the ring in the acid part of the ester with fixed position of the fluorine atom or

with variation of the position of the fluorine atom with fixed ring structure is discussed. The physical properties of

the esters have been found to be strongly dependent upon the presence and position of the fluorine atom. A very

large value for the dielectric anisotropy of one of the esters has been determined.

J. Physique 46 (1985) 1395-1404 Ao8T 1985;

Classification Physics Abstracts 61. 30G

1. Introduction..

Compounds with one strong dipole (usually provided by a nitrile function) in a terminal position are essen-

tial components of nematic mixtures for liquid crystal displays such as the twisted nematic [1] and the guest- host displays [2]. These compounds exhibit large

dielectric anisotropies which are compatible with

the low threshold voltage values required for these electrooptic effects. The values and the temperature dependence of the dielectric and elastic constants of the nematic phases of these compounds are very

important for the optimum performance of the above mentioned displays. In order to study the effect on

these parameters of an additional dipole attached to

the same ring as the nitrile group we have synthesized

ester derivatives of 2-fluoro- and 3-fluoro-4-hydroxy-

benzonitrile. The acid part of the esters contains either

a 1,4-disubstituted benzene, or a cyclohexane, or a bicyclooctane ring. The synthesis and liquid crystal

transition temperatures of these esters are reported

elsewhere [3, 4]. In this publication we report values for the dielectric and elastic constants and the dia- magnetic anisotropy of representative homologues of

these compounds.

The strong terminal dipole moment of the cyano

group generally gives rise to strong molecular correla- tion [5]. In a simple model such cyano compounds

can be described as a binary mixture consisting of virtually uncorrelated molecules (monomers) and pairwise associated molecules (dimers) which are in dynamic, temperature dependent equilibrium [6].

The terminal position of the nitrile dipole leads to antiparallel configurations with the exact form of the

overlap depending on the charge separation within

the molecules and on steric factors. A consequence of the antiparallel arrangement of the molecules is that the dipole moment of the dimer is zero and the effective dielectric constants are smaller than without association. This is because only the dipole of the

monomer contributes to the orientational part of the

polarization. A second consequence is that the

length/breath ratio of the dimer is greater than that of the monomer (depending on the geometrical aniso-

tropy of the dimer). Thus the nematic to isotropic phase transition temperature (TNI) is higher than

without association [4]. The degree of the molecular correlation and the form of the dimers of the fluoro- substituted esters and their influence on the physical properties (in particular on the dielectric constants and nematic-isotropic transition temperatures) are

of marked interest.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:019850046080139500

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2. ExperimentaL

The experimental methods for the determination of the liquid crystal transition temperatures, density, dielectric, diamagnetic, and elastic constants have been described and discussed elsewhere [5].

The accuracy of the data is ± 0.2 OC for the transi- tion temperatures (TNI), + 0.1 for the dielectric constants, ± 0.001 for the refractive index of the

isotropic phase (ni), ± 4 % for the diamagnetic ani- sotropy (Ax), and ± 4 % for the elastic constants (k11’ k22, k33). The derived correlation factor (g) is

accurate within ± 5 %. The particle number density N

is calculated from the relationship p/M. L, where p is the density ( ± 5 x 104), M is the molecular mass, and L is Avogadro’s number.

3. Results and discussion.

The molecular structures of the compounds inves- tigated and values for some of their physical properties

are shown in tables la-d. The data for the isotropic phases (indicated by the index i) were measured just

above the nematic to isotropic transition and those for the itematic phases at t,,(= TITNI)

=

0.95. The complete data of the temperature dependences of the dielectric, diamagnetic, and elastic. properties are given in table III. The data for two of the non fluoro- substituted compounds (4 and 7) have been already published [5, 7] but are recorded in the tables for purposes of comparison.

3.1 DIELECTRIC CONSTANTS.

-

The temperature dependence of the dielectric constants is shown for the benzoates (compounds 1-3) in figure 1, for the heptyl homologue of the cyclohexane compounds (4-6)

in figure 2, for the pentyl homologue of the cyclohexane compounds (7-9) in figure 3, and for the bicyclooctane compounds (10 and 11) in figure 4. The « saturation » in the dielectric anisotropy As = E - B1. at lower temperatures for the 2-substituted esters (X,

=

F;

X2

=

H) is most unusual (see also Fig. 5) and will be

discussed below (E is the dielectric constant with the electric field parallel to the optical axis and B 1. that

perpendicular). Associating liquids are well described

by the formalism given by Kirkwood and Froehlich [8]

who introduced a factor g to represent the degree of

the correlation of the molecular dipoles ( g

=

1 means

no correlation and g

=

0 means complete correlation).

The factor g can be regarded (using the simple model

of unassociated molecules (monomers) and associated

molecular pairs (dimers)) as the proportion of the

free molecules in the binary mixture [6]. The tempera-

ture dependence of g is a consequence of the temperature dependent equilibrium. Values for g

can be calculated from the Kirkwood-Froehlich

equation [9] provided the parameters referred to below are known. The density, the refractive index and the dielectric constants can be determined experi- mentally. The molecular dipole moments of the free molecule can normally be calculated from tabu-

Fig. 1.

-

The dielectric constants ell, s, and 8; of compounds

1 to 3 as functions of reduced temperature. For every com-

pound E is represented by the upper curve and El by the

lower curve.

Fig. 2.

-

The dielectric constants of compounds 4 to 6 as

functions of reduced temperature.

lated group and bond moments [10,11]. In the case of

the fluorine substituted esters an approximation must

be made, since the resulting dipole moment depends

on the orientational correlation of the dipoles of the

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1397

Fig. 3.

-

The dielectric constants of compounds 7 to 9 as functions of reduced temperature.

Fig. 4.

-

The dielectric constants of compounds 10 and 11

as functions of reduced temperature.

ester group and the fluorine atom. As the rotation of the phenyl part of the molecule about the carbon- oxygen single bond of the ester group is sterically

hindered an average between the extreme cases of free rotation and antiparallel arrangement of the

Fig. 5.

-

The dielectric constants of compounds 2, 8, and 11 as functions of reduced temperature.

ketone function and the fluorine atom is assumed. The

experimental data for the refractive indices are listed in table I and the derived dipole moments and the

calculated correlation factors are collated in table II for compounds 1-9. The values of the dipole moments

of the molecules with the fluorine atom in 3-position (X I

=

H ; X2

=

F) are larger while those with the fluorine atom in 2-position (Xl

=

F; X2

=

H) are

smaller than those of the unsubstituted compounds (XI

=

X2

=

H). The same sequence is shown for the

isotropic dielectric constant E; and the dielectric anisotropies (see Table Ia-d), because the differences in the squares of the dipole moments which are deter- mining factors [8] are larger than the differences in the correlation factors of the esters. It is clear from the

g-values in table II that the degree of molecular asso-

ciation of the fluoro-substituted esters is lower than that of the non fluoro-substituted esters. In the

case of the cyclohexane esters (4-9) the 2-fluoro-

substituted compounds (5 and 8) show the lowest

degree of association. In the case of the benzoates

(1-3) the 3-fluoro-substituted ester (3) exhibits no

association whatsoever (g

=

1). The lack of associa-

tion combined with the large dipole moment of 6.1 D

leads to the very high positive dielectric anisotropy (As --- 50) found for this compound. The isotropic

dielectric constant si of compound 3 shows the 1/T dependence typical for non associating polar liquids.

The large dielectric anisotropy (As) of the ester (3) and

the small values for its elastic constants (see Tables I

and III) give rise to a very low threshold voltage

(0.3 V) for a twisted nematic display containing this

compound [12].

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Table I.

-

The physical properties of compound 1 to 12 (TNI transition temperatures ; molecular weight M ; particle

number density Ni’ and dielectric constant 8¡ in the isotropic phase ; the birefringence An, dielectric anisotropy A E and diamagnetic anisotropy A x, elastic constants of splay k11, twist k22, and bend k33 deformations in the nema- tic phase). The data for the isotropic phases were measured just above T NI and for the nematic phases at tr (

=

TI TNI) =

0.95.

Ia : Compounds 1 to 3.

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1399

TABLE I (continued).

(7)

Table II.

-

Calculated molecular dipole moment p of compounds 1 to 9 and correlation coefficient g.

Table III.

-

The dielectric constants, the diamagnetic anisotropy AX, and the elastic constants of compounds 1 to

11 as a function of temperature.

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1401

TABLE III (continued) -

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TABLE III (continued).

The temperature dependence of the association

(when present) may complicate the temperature beha- viour of the dielectric constants, as was found for the esters with substitution in the 2-position (see Fig. 6).

E; and 7

=

(E 11 + 2 sl)/3 exhibit a curved temperature dependence and for Ae a saturation is observed at a

low reduced temperature (see Fig. 5). Although the

association is presumed to be affected only weakly by

the long range order of the nematic phase, the ana- lysis is rather difficult due to the anisotropic internal

fields.

3.2 DIAMAGNETIC ANISOTROPY AND ELASTIC CONS- TANTS.

-

The diamagnetic anisotropy of the esters

exhibits the normal temperature dependence (see Fig. 7). The values for the benzoates are three times as

large as those of the cyclohexane and bicyclooctane compounds due to the presence of two aromatic rings.

The bicyclooctanes have slightly lower values than the

cyclohexane compounds (presumably due to a smaller particle number density).

The elastic constants of the esters containing

benzene (1-3), cyclohexane (4-6), and bicyclooctane (10, 11) rings are shown in figures 8-10. For each

ester k33 > kll > k22 (except (5) where, close to T, k33 kl l). The compounds with the fluorine atom in the 2-position (Xl

=

F; X2

=

H) possess the

largest elastic constants and those with the fluorine atom in the 3-position (Xi =’ H; X2

=

F) possess the smallest elastic constants. The k33/ki i ratio,

which is important for multiplexed addressing of

the twisted nematic display (it should be 1), is

shown in figure 11. As is usually found for bicyclo-

octane derivates [13, 14] the k33/ki l values of the bicyclooctane esters (10 and 11) are very large (> 2).

Fig. 6.

-

The dielectric mean 8

=

(E I, + 2 El)/3 and si

of compounds 2, 8, and 11 as functions of reduced tempe-

rature.

Fig. 7.

-

The diamagnetic anisotropy of compounds 1 to 6, 10 and 11 as a function of reduced temperature.

The lowest value of k3-3/k11 is observed for the heptyl homologue of the 2-fluoro-substituted cyclohexane

ester (5). The corresponding pentyl homologue exhibits

a much higher k33/kll ratio (see Tables Ic and III).

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1403

Fig. 8.

r-

The elastic constant k 11 of splay deformation for

compounds 1-6, 10 and 11 as a function of reduced tempe-

rature.

Fig. 9.

-

The elastic constant k22 of the twist deformation for compounds 1-6, 10 and 11 as a function of reduced temperature.

Fig. 10.

-

The elastic constant k33 of the bend deformation for compounds 1-6, 10 and 11 as a function of reduced temperature.

Fig. 11.

-

The ratio k33/kll of compounds 1-6, 10 and 11

as a function of reduced temperature.

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Thus the ratio of the elastic constants k3 3/k 11 depends

much more directly on the length of the alkyl chain

than on the position of the fluorine substituent 3 . 3 CONCLUSION.

-

In this paper we have investigated

the variation in the dielectric, diamagnetic, and elastic

properties of 2-fluoro, 3-fluoro substituted 4-cyano- phenyl esters and their unsubstituted analogues with

either variation of the ring of the acid part with fixed

position of the fluorine atom or with variation of the

position of the fluorine atom with fixed ring structure.

The diamagnetic anisotropy was found to depend mainly on the ring structure and not on the position of

the fluorine substitution. The elastic constants of the 2-fluoro components are larger and those of the 3" j

fluoro components are smaller than those of the

unsubstituted analogues. The analysis of the dielectrics constants showed that in addition to differences in the

dipole moment the degree of molecular association also varied. The association is lowest for the ben- zoates

-

presumably due to steric effects

-

and is

completely absent for one ester. In that case the combi- nation of a large dipole moment with the lack of molecular association leads to large dielectric cons- tants and a dielectric anisotropy of nearly 50.

References

[1] SCHADT, M. and HELFRICH, W., Appl. Phys. Lett. 18 (1971) 127.

[2] SCHEFFER, T. J., Philos. Trans. R. Soc. London A309

(1983) 189.

[3] KELLY, S. M., Helv. Chim. Acta, 67 (1984) 1572.

[4] KELLY, S. M. and SCHAD, HP., Helv. Chim. Acta 67

(1984) 1580.

[5] SCHAD, HP. and OSMAN, M. A., J. Chem. Phys. 75 (1981) 880 and references therein.

[6] DANNHAUSER, W. and FLUECKINGER, A. F., J. Phys.

Chem. 68 (1964) 1814.

[7] SCHAD, HP. and OSMAN, M. A., J. Chem. Phys. 79 (1983) 5710.

[8] BOETTCHER, C. J. F. and BORDEWIJK, P., Theory of

Electric Polarization (Elsevier, Amsterdam) 1978,

vol. II.

[9] BORDEWIJK, P., J. Chem. Phys. 73 (1980) 595.

[10] McCLELLAN, A. L., Tables of Experimental Dipole

Moments (Freeman, San Francisco) 1963.

[11] MINKIN, V. I., OSIPOV, O. A. and ZHADANOV, Y. A., Dipole Moments in Organic Chemistry (Plenum,

New York) 1970.

[12] SCHAD, HP. and KELLY, S. M., J. Chem. Phys. 81 (1984) 1514.

[13] BRADSHAW, M. J., McDONNELL, D. G. and RAYNES,

E. P., Mol. Cryst. Liq. Cryst. 74 (1981) 1567.

[14] CONSTANT, J. and RAYNES, E. P., Mol. Cryst. Liq. Cryst.

74 (1981) 1383.

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