Abstract

The high-speed photography, large eddy simulation, and coupled level set and volume-of-fluid methods were used to study the initial flow structures, the wave morphologies, and the instantaneous velocity distributions of three-dimensional jets from non-circular nozzles at different viewing sections under low pressure conditions. Two non-circular nozzles, including square and triangular orifice shapes, were designed based on the principle of the equal flow rate at the same pressure. The results showed that the surface waves of the square and triangular jets increased as the working pressures increased due to the air resistance increments, and more fluid band structures and droplets appeared. For the different viewing sections of the jets from the square and triangular nozzles, the surface wave was distributed symmetrically on both sides of the jets for the square nozzles. The jet flowing from the orifice’s symmetrical angles had better aggregation than the jet flowing from the orifice’s edges. The amount of fluid that moved continuously with the jet increased with the entrainment of the air into the jet, and the jet’s instantaneous velocity gradually decreased. As the jet developed, the vortexes gradually spread and entrained the surrounding medium to transfer energy, causing it to decay exponentially along the jet axis. Moreover, the jet’s instantaneous velocity distributions at different vertical sections along the jet’s direction were completely clear from the three-dimensional view. The shapes of the instantaneous velocity parabola in different vertical sections were analyzed in detail, and zigzag-shaped parabolas from the triangular jet were observed.

Highlights

  • Liquid jet refers to the discharge of fluid flow from a nozzle mixing with the surrounding air after the free control of the solid boundary

  • Using the different nozzles’ flow rate coefficients, we found that the circular nozzle had the largest average flow rate coefficients, while the triangular nozzle produced the smallest average flow rate coefficients, which agreed with the conclusion cited by Hua et al (2018)

  • Jet exit velocity (m/s) scitation.org/journal/adv different square jet sections, the jet surface wave fluctuated violently at the angle 1 section compared with the angle 2 section

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Summary

Introduction

Liquid jet refers to the discharge of fluid flow from a nozzle mixing with the surrounding air after the free control of the solid boundary. Jets can be classified as high-pressure jets (≥500 kPa), intermediate-pressure jets (200 kPa–500 kPa), and low-pressure jets (≤200 kPa) according to the working pressure and nozzle configurations (Gilley and Watts, 1977). High-pressure jets are normally found in the field with low-quality requirements where the intensity of dripping water is high. Gao (2000; 2006) and Chu (2014) indicated that spray irrigation equipment should be directed toward low pressures, and non-circular nozzles are more effective for the dispersal of water jets. Sprinkler nozzles can be classified as hollow cone nozzles, solid cone nozzles, non-circular nozzles, and so on according to the shape. Non-circular nozzles can reduce the working pressure of sprinklers and improve the hydraulic performance with variable jet shape, manageable jet intensity, and more effective jet areas. The study of the breakup characteristics of non-circular jets is of great interest and value not just for irrigation engineering applications and for gas dynamics

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