“…The evolution of both the velocity v = u î + w k = −∇ × ĵψ and the temperature χ(τ = τ in , x, z) fields over the nematic microvolume with the orientational defect located on the lower boundary of the HAN channel as the function of the angle α are shown in Figures 18-23, respectively. The distribution of the velocity field v in the microscopic nematic volume with the orientational defect located at −L ≤ x ≤ L, z = −1, when the laser beam is directed at the values of the angle α equal to 20 • and 40 • (Figure 18a,b), 60 • and 80 • (Figure 19a,b), 90 • (Figure 20), 100 • and 120 • (Figure 21a,b), 140 • and 160 • (Figure 22a,b) are shown in Figures 18-22[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 coefficientQ 0 = d…”