Abstract:Zvetkow twist viscosity measurements are reported for a series of cyanobiphenyl liquid crystals and their cutectic mixtures in the nematic phase. The values obtained exhibit a n odd-even variation. If the data are plotted against a reduced density, they divide into two groups, one corresponding to the odd and the other to the even series. This is attributed to effects of the configuration of the alkyl chain on the molecular packing density in the nematic phase. Using the Maier-Saupe theory, interaction energie… Show more
“…Close agreement is observed between the measurements reported in this paper and those of Seidler et al [14] at the highest temperatures, but significant differences are observed as the temperature is lowered. Torsion angle [16]; -Seidler et al [14]; X Beens [17].…”
Section: Temperature-dependent Density Measurementssupporting
confidence: 90%
“…The constants obtained from the fitting of the data to Equation (3) are listed in Table 2 3.2 Viscosity coefficient measurements The principle viscosity coefficients; η 1 , η 2 , η 3, and η 45 were measured for all the liquid crystal materials using the oscillating plate viscometer method (OPV) following the procedures outlined in the previous paper [1]. The rotational viscosity coefficients γ 1 were measured using a modified version of the method described by Seidler et al [14] and described in the previous paper [1]. In this experiment the magnetic field is rotated relative to the suspended sample.…”
Section: Temperature-dependent Density Measurementsmentioning
confidence: 99%
“…Oscillatory plate viscometer measurements used refinement of the method described by Seidler et al [14]. The current equipment uses a larger magnet which is suspended in a cradle, allowing rotation of the magnetic field axis and the plane of the plate oscillation and allowing measurement of the viscosity coefficients of the principle axes as described in the previous paper [1].…”
Oscillating plate and rotational viscosity measurements are reported for a series of liquid crystals and include n-p-cyano-p-hexylbiphenyl (K18), 4-n-hepthyl-4 -cyanobiphenyl (K21), ethyl-cyclohexyl-ethyl-6-fluoron-propyl-biphenyl (I32), n-propyl-cyclohexyl-ethyl-6-fluoro -n-butyl-biphenyl (I43) and a n-pentyl-cyclohexylcyanophenyl : n-heptyl-cyclohexyl-cyanophenyl mixture. Rotational viscosity measurements were carried out over a temperature range from ambient to ∼90 • C. Comparison of the values at a temperature of 5 K above the below the clearing point indicate an odd-even effect as the chain length of the hydrocarbon tail is altered. The principle viscosities η 1 , η 2 , η 3 and η 45 were measured using an oscillating plate viscometer and the temperature dependences used to calculate the activation energies for flow in the various directions. The magnitude of the activation energy is shown to change with the length of the hydrocarbon chain. The incorporation of the cyclohexyl group imparts flexibility and reduces the activation energy flow, whilst the presence of the fluoro group increases the interactions between molecules, and this is reflected in higher values of the viscosity. The change of viscosity with alignment angle is explored for two of the systems studied and the fit to theory investigated. The Leslie-Ericksen coefficients are calculated for these systems and discussed in terms of changes in the molecular interactions.
“…Close agreement is observed between the measurements reported in this paper and those of Seidler et al [14] at the highest temperatures, but significant differences are observed as the temperature is lowered. Torsion angle [16]; -Seidler et al [14]; X Beens [17].…”
Section: Temperature-dependent Density Measurementssupporting
confidence: 90%
“…The constants obtained from the fitting of the data to Equation (3) are listed in Table 2 3.2 Viscosity coefficient measurements The principle viscosity coefficients; η 1 , η 2 , η 3, and η 45 were measured for all the liquid crystal materials using the oscillating plate viscometer method (OPV) following the procedures outlined in the previous paper [1]. The rotational viscosity coefficients γ 1 were measured using a modified version of the method described by Seidler et al [14] and described in the previous paper [1]. In this experiment the magnetic field is rotated relative to the suspended sample.…”
Section: Temperature-dependent Density Measurementsmentioning
confidence: 99%
“…Oscillatory plate viscometer measurements used refinement of the method described by Seidler et al [14]. The current equipment uses a larger magnet which is suspended in a cradle, allowing rotation of the magnetic field axis and the plane of the plate oscillation and allowing measurement of the viscosity coefficients of the principle axes as described in the previous paper [1].…”
Oscillating plate and rotational viscosity measurements are reported for a series of liquid crystals and include n-p-cyano-p-hexylbiphenyl (K18), 4-n-hepthyl-4 -cyanobiphenyl (K21), ethyl-cyclohexyl-ethyl-6-fluoron-propyl-biphenyl (I32), n-propyl-cyclohexyl-ethyl-6-fluoro -n-butyl-biphenyl (I43) and a n-pentyl-cyclohexylcyanophenyl : n-heptyl-cyclohexyl-cyanophenyl mixture. Rotational viscosity measurements were carried out over a temperature range from ambient to ∼90 • C. Comparison of the values at a temperature of 5 K above the below the clearing point indicate an odd-even effect as the chain length of the hydrocarbon tail is altered. The principle viscosities η 1 , η 2 , η 3 and η 45 were measured using an oscillating plate viscometer and the temperature dependences used to calculate the activation energies for flow in the various directions. The magnitude of the activation energy is shown to change with the length of the hydrocarbon chain. The incorporation of the cyclohexyl group imparts flexibility and reduces the activation energy flow, whilst the presence of the fluoro group increases the interactions between molecules, and this is reflected in higher values of the viscosity. The change of viscosity with alignment angle is explored for two of the systems studied and the fit to theory investigated. The Leslie-Ericksen coefficients are calculated for these systems and discussed in terms of changes in the molecular interactions.
“…However, because of the scatter in the values for elastic constant K reported in literature [41][42][43][44] only rough estimation can be made. For the typical average value K = 1 • 10-" N and with (Av) = 15 kHz and i = 0.1 Pa • s [42,[45][46][47][48] one obtains A = 2.0. 104 s -312 in agreement with experiment.…”
The proton spin-lattice relaxation time T, in the nematic liquid crystal 4-pentyl-4'-cyanobiphenyl confined in a glassy porous matrix has been measured in a wide Larmor frequency range of 1 • 102-2. 10 Hz employing the fast field-cycling NMR technique. A strong influence of the restricted geometry on the character of the T, dispersion was found. Our investigation clearly demonstrates the importance of the translationally induced molecular reorientations in inhomogeneous director field for the relaxation in the samples with 200 and 80 nm mean pore size. The experimental results are in a good agreement with the theoretical predictions. In the sample with 7 nm pore size the main contribution to the relaxation is ascribed to the slowing down of the molecular motion in the near-surface layer. Zero-field 'H NMR spectra of a microconfined liquid crystal are reported for the first time.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.