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Pulsating flows of viscous fluid in flat channel for given harmonic fluctuation of flow rate

Kuralboy NavruzovUrgench State University, Urgench, UzbekistanMuhammadi TurayevKattakurgan branch of Samarkand State University, Samarkand, UzbekistanZoxid ShukurovKattakurgan branch of Samarkand State University, Samarkand, Uzbekistan
E3S Web of Conferencesjournal2023en
ABI

Abstract

In research work, it is pointed out the issue of a pulsating flow of a viscous incompressible fluid in a flat channel for a given harmonic fluctuation of the fluid flow rate. The study of the generation of pulsating current is used in biological mechanics, in particular, in the use of microchip systems. In addition, to ensure a constant flow of liquid, pneumatic micropumps that periodically squeeze liquid from empty volumes are widely used. In such systems, the installation of pulsating flow is shown to be economically beneficial. The transfer function of the amplitude-phase rate response is determined; with the help of these functions, the ratio of the tangential shear pressure on the channel fence to the average acceleration over the channel section is determined. In Figure 1, it can be seen that the ratio of K H = 0 of in τ HC /τ 0 KC is close to one and α 0 2 is less than one. If α 0 2 takes on values greater than unity, then the ratio of to K H = 0 to τ HC /τ 0 KC is greater than unity, and it has been shown to increase with increasing frequency of dimensionless oscillation. It was shown that in an unsteady flow of liquid, even in cases where liquid acceleration is equal to zero, it was studied that the stress on the wall of the channel exceeds its quasi-stationary value. τ HC /τ 0 KC with the increase of the ratio K H , the increase of the parameter is explained by the fact that the change of the tensile stress on the wall advances in phases concerning the average speed along the section. Calculations determine that the non-stationary shear pressure on the channel fence increases non-monotonically with the acceleration of the liquid particle at low oscillation frequencies. The shear pressure reaches its maximum value, then decreases with increasing dimensionless oscillation rate, and asymptotically approaches the values without accelerated flow.

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