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Articles

An experimental and computational study of calamitic and bimesogenic liquid crystals incorporating an optically active [2,2]-paracyclophane

Pages 1567-1573 | Received 25 Jan 2018, Accepted 13 Mar 2018, Published online: 22 Mar 2018

Figures & data

Figure 1. The DFT(B3LYP/6-311G(dp)) optimised geometry of both the S (left) and R (right) forms of 4-fluoro[2,2]paracyclophane.

Figure 1. The DFT(B3LYP/6-311G(dp)) optimised geometry of both the S (left) and R (right) forms of 4-fluoro[2,2]paracyclophane.
short-legendScheme 1.

Figure 2. Plot of the reciprocal pitch (1/P, μm−1) as a function of concentration (wt %) for binary mixtures of 1 in 5CB.

Figure 2. Plot of the reciprocal pitch (1/P, μm−1) as a function of concentration (wt %) for binary mixtures of 1 in 5CB.

Figure 3. The molecular structures of compound 2 (Cr 138.3 Iso) and the related dimer CB6OCB (Cr 102 TB 110.5 N 154.2 Iso. Liq.) [Citation15,Citation17].

Figure 3. The molecular structures of compound 2 (Cr 138.3 Iso) and the related dimer CB6OCB (Cr 102 TB 110.5 N 154.2 Iso. Liq.) [Citation15,Citation17].

Table 1. Transition temperatures (°C) and pitch lengths (PN*, μm) for mixtures AI and extrapolated values (*) for compound 1. Measurements were performed at 20°C for all materials which correspond to the reduced temperatures (Tr, TN-Iso/T) indicated.

Table 2. Transition temperatures (°C), associated enthalpies of transition [kJ mol−1] and pitch lengths (PN*, μm) for mixtures AF and extrapolated values (*) for compound 2. # The pitch of mixture A was too long (>100 μm) to be measured by the Cano Wedge method. Measurements were performed at 20°C for all materials which corresponds to the reduced temperatures (Tr, TN-Iso/T) indicated.

Figure 4. Plot of the reciprocal pitch (1/P, μm−1) as a function of concentration (wt %) for binary mixtures of 2 in 5CB.

Figure 4. Plot of the reciprocal pitch (1/P, μm−1) as a function of concentration (wt %) for binary mixtures of 2 in 5CB.

Figure 5. Plot of the energy relative to the lowest conformer (kJ mol−1) as a function of the indicated torsional angle (τ, °) for p-terphenyl (a) and (R) 4-biphenyl-[2,2]-paracyclophane (b) as calculated at the wB97XD/6-31G(d,p) level of DFT. Spline fits (solid lines) are presented as a guide to the eye.

Figure 5. Plot of the energy relative to the lowest conformer (kJ mol−1) as a function of the indicated torsional angle (τ, °) for p-terphenyl (a) and (R) 4-biphenyl-[2,2]-paracyclophane (b) as calculated at the wB97XD/6-31G(d,p) level of DFT. Spline fits (solid lines) are presented as a guide to the eye.

Figure 6. (A) The wB97XD/6-31G(d,p) minimised geometry of compound 2; (B) histogram plot of the probability of a given bend angle – defined as the angle between the long axis of each mesogenic unit – for CB6OCB and compound 2 determined using the AM1 semi empirical method as described in ref [Citation15].

Figure 6. (A) The wB97XD/6-31G(d,p) minimised geometry of compound 2; (B) histogram plot of the probability of a given bend angle – defined as the angle between the long axis of each mesogenic unit – for CB6OCB and compound 2 determined using the AM1 semi empirical method as described in ref [Citation15].

Figure 7. A hypothetical [2,2] paracyclophane in which both rings are incorporated into the mesogenic unit. When three of the four R groups are different the resulting material is chiral.

Figure 7. A hypothetical [2,2] paracyclophane in which both rings are incorporated into the mesogenic unit. When three of the four R groups are different the resulting material is chiral.
Supplemental material

TLCT_1453559_Supplemental data

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