The Influences of the Nozzle Throat Length and the Orifice Grooving Degree on Internal Flow Field for a Multi-Entry Fan Nozzle Based on FLUENT

Wei Deng^1,2,3,4, Ruirui Zhang^1,2,3,4, Gang Xu^1,2,3,4, Longlong Li^1,2,3,4, Qin Tang^1,2,3,4, Min Xu^1,2,3,4

¹Beijing Research Center of Intelligent Equipment for Agriculture, Beijing, China.
²National Research Center of Intelligent Equipment for Agriculture, Beijing, China.
³Key Laboratory of Agri-Informatics, Ministry of Agriculture, Beijing, China.
⁴Beijing Key Laboratory of Intelligent Equipment Technology for Agriculture, Beijing, China.

DOI: 10.4236/eng.2019.1111052                

Abstract

Spray nozzle is a key component in equipment for plant protection and water-saving irrigation. The fan nozzle is a kind of spray nozzle, which is widely used in agriculture and forestry for irrigation and control of diseases, insects, and weeds. In consideration of the increasing velocity of the flow field, when the hydraulic pressure remains unchanged and the flow path becomes narrow, and because the increase of the velocity of spray drops can increase the penetrability of spray drops into the plant canopy, a kind of new fan nozzle with multi entries and simple inner structure was designed and the influences of its structure parameters on the inner flow field were analyzed using FLUENT software. The experimental results showed that the influence of the throat length on the inner flow field of the nozzle was insignificant, while the orifice grooving degree had a significant effect on inner flow field of the nozzle. The larger the grooving degree was, the smaller the pressure and velocity of internal flow field of the nozzle. The nozzle throat length had little influence on the velocity change of internal flow field. Positive correlation was shown between throat length and flow field velocity.

Keywords

Fan Nozzle, Orifice, Spray, FLUENT, Multi-Entry, Inner Flow Field

1. Introduction

China is an agricultural country. It is indispensable to strengthen the plant protection work during the process of developing China’s agricultural economy, because it is one of the important means to ensure high yield and stable yield of crops [1] [2] [3]. Currently, chemical control is the most effective prevention and treatment method among the three crop protection methods (physical control, chemical control, integrated control), and spraying agro-chemical pesticides is the most commonly used method in chemical control [4] [5] [6]. Especially in the face of a sudden outbreak of large-scale diseases, insects, and weed damage, spraying chemical pesticides is particularly effective [7] [8] [9]. Although the spray nozzle is only a small part of the spraying machine, its function cannot be ignored. The nozzle directly affects the spray quality. Only the nozzle with good performance can produce desired spray characteristics, such as the spray flow-rate, spray droplet size, droplet velocity, the uniformity of droplet deposition, and so on, further to improve the penetrability of the spray droplet and minimize the droplet drift and chemical loss [10] [11] [12], which is directly related to the key indicators of atomization quality [13] [14] [15] [16]. Optimizing the internal structure of plant-protection nozzles is one of the most important researches at home and abroad.

Deng Wei et al. [17] conducted relevant experimental research on the influence of different flow-rate control methods on the droplet movement velocity and droplet deposition rate of large nozzles. The research showed that suitable smaller droplet diameter spectra can be obtained and spray droplet velocity can be increased through adjusting spray duty cycle, spray pressure, and nozzle size using the method of PWM-based intermittent spray from enlarged nozzles operated at increased liquid pressure. So that, spray deposition rate could be improved. Xie Chen [18] compared the atomization process of two kinds of fan nozzles manufactured by foreign countries, which provided a reference for the development of new nozzles. Garcera C et al. [19] did a relevant comparative study on the spray droplet deposition of standard cone nozzles and venturi anti-drift nozzles. Bozdogan and the co-authors [20] studied the coverage of the pesticide liquid, the droplet drift, and the liquid residue for pesticide application in strawberry field using three different nozzles: hollow cone nozzle (MI), air-assisted rotating nozzle (M2), and flat fan nozzle (M3). Raquel et al. [21] conducted experimental research on the parameters of the spray performance for the fan-shaped mist nozzle, in terms of the radial droplet distribution and the droplet size. Miller P C H and his co-researchers [22] did experiments on flat fan nozzles and the study results showed that there were many factors affecting the spray process, which had certain influence and guidance on the nozzle design. Burguete et al. [23] studied the spray droplet size and droplet trajectory of the fan-shaped mist nozzle.

From the literatures, it is considered that the situation of few types of nozzles for agro-chemical spray application in China is one of the major gaps between China and developed countries in the field of plant protection nozzles [24] [25] [26]. Therefore, it is especially important to strengthen the nozzle design and optimization of the inner structure of nozzles for promoting the development of agricultural plant protection in China.

For fan nozzles, which are widely used for plant protection in China, the atomization process is that the chemical liquid enters the nozzle under the action of pressure, flowing through the nozzle throat. Due to being squeezed by the wedge surface of the slotted groove of the nozzle orifice, the squeezed liquid spreads into a planar liquid film and then differentiates into pretty small droplets. Finally, these atomized small droplets were uniformly sprayed onto the target vegetation [27] [28] [29] [30]. The main structural parameters of the fan nozzle mainly include the cutting angle of the groove on orifice, the cavity diameter, the length of the nozzle throat, and the relative cutting depth.

Design of spray nozzles involves simulation and test verification of flow field inside the spray nozzles. In recent studies, there have been some similar research methods in different fields. In reference [31], for poor spraying uniformity and short range in low-pressure sprinklers, various special-shaped nozzles were designed based on the principle of identical cross-sectional area. ANASY CFX was applied to simulate three-dimensional internal flow field in these sprinklers. The numerical simulation results were validated by using the measured performance parameters of low-pressure sprinklers, including range, water distribution and drop diameter. In literature [32], commercial software FLUENT was applied to calculate the flow pressure characteristics and internal velocity distribution of full jet nozzle under working conditions. Compared with the experimental results, the simulation results showed that the internal flow field of the full jet nozzle was in good agreement with the experimental results. According to the numerical simulation, the velocity vector diagram of the internal flow field of the full jet nozzle was obtained under direct and wall-attached conditions. Similarly, many studies showed that numerical simulation using FLUENT software can be applied effectively to analyze the flow field features inner the nozzles [26] [33] [34].

In this paper, based on the atomization principle of the nozzle, the entrance part of a fan nozzle was re-designed to be a multi-inlet, single-outlet step-like new structure. And the re-designed nozzle was simulated, focusing on two factors: the cutting angle of the orifice groove and the length of the nozzle throat.

2. Materials and Methods

2.1. Design of New-Type Multi-Entry Fan Nozzle

Based on the ordinary fan nozzle, a change of the nozzle entrance was made for trying to improve the spray characteristics. A kind of multi-inlet and single-outlet nozzle was preliminarily designed, namely, a 5-hole inlet, of which the diameter of each hole was 1 mm and the outlet was a V-shaped groove. The 3-D model of the modified nozzle was drawn using the 3-D drawing software “Solidworks”. For the modified fan nozzle, the 3-D model diagram (a) drawn in “Solidworks”, the overall external view (b), overall internal structure (c), the top view (d), the bottom view (e), the cross-sectional view (f), and the right-side view are separately showed in Figure 1.

Figure 1. Views from different angles of the modified fan nozzle. (a) 3-D model; (b) overall external view; (c) overall internal structure; (d) top view; (e) bottom view; (f) cross-sectional view; (g) right-side view.

2.2. Simulation of the Internal Flow Field of the 5-Hole-Inlet Nozzle

2.2.1. Meshing

It is assumed that the fluid inside the nozzle is steady-state and incompressible, then a solid-liquid non-slip boundary is adopted. The model of the modified nozzle was imported into ANSYS for meshing. Set the five small-end faces at the bottom of the grid to be the entrance of the flow field. The two faces of the V-shaped groove orifice was the exit of the flow field. The mesh plot is shown in Figure 2.

2.2.2. Numerical Simulation

In the study, a pressure-based steady-state algorithm was used. The boundary conditions were selected as pressure inlet and pressure outlet. The inlet pressure was 3 Mpa and the outlet pressure is atmospheric pressure. The medium was single-phase liquid water. The SIMPLE solution method belonging to the finite volume method was adopted to be the numerical simulation method which currently is the most widely used in flow field calculations in engineering practices. The governing equation was the standard k-ε turbulence model, in which the equations of turbulent kinetic energy k and turbulent dissipation rate ε are as follows [35] [36] [37] [38]:

$\frac{\partial }{\partial t}\left(\rho k\right)+\frac{\partial }{\partial x_i}\left(\rho k{u}_i\right)=\frac{\partial }{\partial x_j}\left[\left(\mu +\frac{{\mu }_t}{{\sigma }_k}\right)\frac{\partial k}{\partial x_j}\right]+G_k+G_b-\rho \epsilon -Y_M+S_k$ (1)

$\frac{\partial }{\partial t}\left(\rho \epsilon \right)+\frac{\partial }{\partial x_i}\left(\rho k{u}_i\right)=\frac{\partial }{\partial x_j}\left[\left(\mu +\frac{{\mu }_t}{{\sigma }_{\epsilon }}\right)\frac{\partial \epsilon }{\partial x_j}\right]+C_{1\epsilon }\frac{\epsilon }{k}\left(G_k+G_{3\epsilon }{G}_b\right)-C_{2\epsilon }\rho \frac{{\epsilon }^2}{k}+S_k$ (2)

Figure 2. Meshing.

where, ρ is the continuous phase density, kg/m³; ε is the turbulent dissipation rate, m²/s³; k is the turbulent kinetic energy, m²/s²; μ is the dynamic viscosity, pa·s; σ_k is the Prandtl number of turbulent kinetic energy; σ_s is the Prandtl number of dissipation rate of turbulent kinetic energy; G_k the turbulent kinetic energy caused by laminar velocity gradient, pa/s; Y_M is the kinetic energy generated due to the transitional diffusion in the compressible turbulent flow, pa/s; C_1e, C_2e, C_3e is the empirical constant.

2.3. Application Software

ANSYS software is a kind of large-scale general finite element analysis software developed by American ANSYS Inc., which can match with many design software to realize data sharing and exchange, such as Creo, NASTRAN, Alogor, AutoCAD. FLUENT Inc., which is a commercial CFD (Computer Fluid Dynamics) software commonly used in the international market and a leader in fluid simulation, was taken over by ANSYS Inc. in 2006 to integrate FLUENT into its ANSYS software. It has rich physical models, advanced numerical calculation methods, and powerful post-processing functions. The version of the ANSYS used in the study was ANSYS 15.0.

3. Results

3.1. The Simulating Result

After setting the relevant parameters, 200 times of iteration calculation were performed on the nozzle model and the residual curve appeared converged. The plots of pressure contours and velocity contours for the nozzle inlet and outlet are respectively shown in Figure 3 and Figure 4.

It can be seen from Figure 3 and Figure 4 that the pressure on the same cross section was the same for both the inlet and the outlet, while the velocity on the

Figure 3. Plots of the pressure and velocity contour of the nozzle inlet.

Figure 4. Plots of the pressure and velocity contour of the nozzle outlet.

same cross section was varying. The more, the pressures on same cross section of the five holes at the inlet were the same and higher than the other areas along the nozzle throat. The pressure at the outlet gradually decreased layer by layer as a rippled shape from the center to the edge.

3.2. Effect of the Throat Length on the Internal Flow Field of the Nozzle

In the case of a cavity diameter of 2 mm and a grooving degree of 30˚, the nozzle model was simulated on three conditions of 2.5 mm, 3.0 mm, and 4.0 mm nozzle throat lengths, as listed in Table 1. As the simulation result, the pressure and velocity contour plots of the internal flow field for the nozzles with three different throat lengths are separately shown in Figure 5.

Figure 5(a), Figure 5(c), and Figure 5(e) are the pressure contour plots with nozzle throat length of 2.5 mm, 3.0 mm, and 4.0 mm, respectively. The results showed that the pressure inside the nozzle significantly changed when there were abrupt places on the in wall of nozzle throats. Moreover, from the inlet to the outlet, the pressure first increased to a certain value and then decreased.

Table 1. Internal structural parameters of nozzles with different throat lengths.

Figure 5. The pressure and velocity contour plots for nozzle throat lengths of 2.5 mm, 3.0 mm, and 4.0 mm.

With the increasing throat length, there is no significant change in the pressure of the internal flow field of the nozzle. Figure 5(b), Figure 5(d), and Figure 5(f) are the velocity contour plots at the nozzle length of 2.5 mm, 3.0 mm, and 4.0 mm. The flow velocity inside the nozzle significantly changed when there was an abrupt place for the internal cross section of the nozzle. Moreover, from the inlet to the outlet, the flow velocity first decreased and then increased. The velocity at the orifice portion was the largest.

Since the plots of the pressure and the velocity contours at each part of the flow field inside the nozzle exist in separate graphs, it is unable to make an intuitive and clear comparison. Therefore, the pressure and the velocity data on the center line of the internal flow field of the three nozzles were separately extracted in the FLUENT software and then respectively plotted in the same table for the purpose of conducting a comparative analysis and further contrasting with the conclusions obtained from the contour plots. The resulting plots were shown in Figure 6 and Figure 7. Figure 6 is the pressure profile on the center line of each nozzle with different nozzle throat lengths and Figure 7 is the velocity profile on the center line of each nozzle with different nozzle throat lengths.

It can be seen from Figure 6 that the pressure profiles on the center lines of Nozzle 1, 2, and 3 which had different throat lengths were almost the same, which indicated that the structural parameter of the nozzle throat length had similar effect on the pressure changing trend of the internal flow field of the nozzle. The internal flow field pressure significantly changed along the center of the nozzle throat for each of the three nozzles. Within a certain range, the flow field pressure first decreased and then increased from the inlet to the outlet of the nozzle.

It can be seen from Figure 6 that the velocity profiles on the center lines of Nozzle 1, 2, and 3 with different throat lengths were different, which showed that to some extent the velocity of the internal flow field of the nozzle was influenced by the structure parameter of the nozzle throat length and gradually decreased as the nozzle throat length increased. The more, the velocity profiles were relatively unchanged after the distance from the inlet surface was 3.0 mm. for each one of the three nozzles, within a certain range the internal flow field velocity was gradually reduced from the inlet to the outlet of the nozzle.

3.3. Effect of the Grooving Degree on the Internal Flow Field of the Nozzle

As the case of a cavity diameter of 2 mm and a nozzle throat length of 3.5 mm, three different nozzles with grooving degree of 15˚, 30˚, and 45˚ were shown in Table 2. The simulated results of the pressure and velocity contour plots of internal flow field of the nozzles listed in Table 2 were shown in Figure 8.

It can be seen from the simulation results in Figure 8 that for the orifice grooving degrees of respectively 15˚, 30˚, and 45˚, the pressure and velocity inside the nozzle significantly changed when there were abrupt places for the in wall of nozzle throats. From the inlet to the outlet, the flow field pressure first

Figure 6. The pressure profile on the center line of each nozzle with different nozzle throat lengths.

Figure 7. The velocity profile on the center line of each nozzle with different nozzle throat lengths.

Table 2. Internal structural parameters of nozzles with different grooving degrees.

increased and then decreased. As the grooving degree increased, the internal flow field pressure of the nozzle gradually decreased. From the inlet to the outlet, the internal flow field velocity first decreased and then increased.

In order to compare the pressure and the velocity of the internal flow field of nozzles with different orifice grooving degrees, the data of the pressure and the velocity on the center line of nozzles with different grooving degrees were separately abstracted from the simulating results in FLUENT software and the profiles of the pressure and the velocity along the center lines of the nozzles were respectively plotted in the same diagram, as shown in Figure 9 and Figure 10. Figure 9 is the pressure profile on the center line of each nozzle with different orifice grooving degrees and Figure 10 is the velocity profile on the center line of each nozzle with different orifice grooving degrees.

Figure 8. The pressure and velocity contour plots for orifice grooving degrees of 15˚, 30˚, and 45˚.

It can be seen from Figure 9 that the flow field pressure inside the nozzle was significantly influenced by the orifice grooving degree and gradually decreased with the increase of the orifice groove degree within a certain range. From the inlet to the outlet inside the same nozzle, after the pressure of the internal flow field gradually increased to a certain value, then begun to gradually decrease.

Figure 9. The pressure profile on the center line of each nozzle with different orifice grooving degrees.

Figure 10. The velocity profile on the center line of each nozzle with different orifice grooving degrees.

It can be seen from Figure 10 that the velocity profiles on the center lines of Nozzle 4, 5, and 6 almost overlapped, which indicated that the orifice grooving degree had a negligible effect on the internal flow field velocity of the nozzle. For each velocity profile, namely for each nozzle with different orifice grooving degrees, the velocity of the internal flow field gradually decreased from the inlet to the outlet of the nozzle.

4. Conclusion

In consideration of the increasing velocity of the flow field, when the hydraulic pressure remains unchanged and the flow path becomes narrow, a re-designed nozzle with a multi-inlet and single-outlet step-like new structure was simulated for its internal flow field using ANSYS software. The results showed that the orifice grooving degree had a significant influence on the flow field pressure and velocity inside the nozzle, while the nozzle throat length had trivial effect on the internal flow field. The velocity of the inner flow field gradually increased and then decreased to a certain value, finally with a tendency of slightly increasing. From the results of simulation analysis, the optimal combination of the structure parameters of fan nozzle was that set Cavity diameter (D) as 2 mm, orifice grooving degree as 30˚, and the nozzle throat length (L) as 3 mm. In addition, the pressure and the velocity of the inner flow field of the nozzle appeared significant change at the abrupt changing point of the internal structure of the nozzle in wall. This research just provided an alternative for trying to change the spray pressure and velocity in order to adapt to different kinds of agro-chemical application for different crops.

Acknowledgements

This research was financially supported by the National Key Research and Development Project of China (No.2017YFD0701004), the National Natural Science Foundation of China (31601228), the Youth Science Fund of the Beijing Natural Science Foundation (6164032). The authors acknowledge the National Experimental Station of Precision Agriculture of China.

Conflicts of Interest

The authors declare no conflicts of interest regarding the publication of this paper.

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