2012
DOI: 10.1039/c2ra00913g
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Thermally excited vortical flow in a microsized nematic cell

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Cited by 4 publications
(7 citation statements)
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“…According to these calculations the highest value of |∇ n(x, z)| is reached in the vicinity of the orientational defect and its effect extends up to 3/4 of the thickness of the nematic volume. [13,26,27], respectively. The heating occurs during the dimensionless time τ in = 1.6 × 10 −4 (∼0.29 ms), whereas the value of dimensionless heat flux coefficient…”
Section: Laser Excited Vortical Flow In Microsized Nematic Channelsmentioning
confidence: 99%
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“…According to these calculations the highest value of |∇ n(x, z)| is reached in the vicinity of the orientational defect and its effect extends up to 3/4 of the thickness of the nematic volume. [13,26,27], respectively. The heating occurs during the dimensionless time τ in = 1.6 × 10 −4 (∼0.29 ms), whereas the value of dimensionless heat flux coefficient…”
Section: Laser Excited Vortical Flow In Microsized Nematic Channelsmentioning
confidence: 99%
“…q 0 is equal to 0.05. The distribution of the velocity v in the microscopic HAN channel with the orientational defect located at −L ≤ x ≤ L, z = −1, when the heat flux q is directed at two values of the angle α, 20 • and 40 • with respect to the lower bounding surface, is characterized by maintaining of vortices as shown in Figure 18a,b [13,26,27], respectively. Here, 1 mm of the arrow length is equal to 1.8 µm/s.…”
Section: Laser Excited Vortical Flow In Microsized Nematic Channelsmentioning
confidence: 99%
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