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2019 International Conference on Information Technology, Electrical and Electronic Engineering (ITEEE 2019) ISBN: 978-1-60595-606-0

Research on Spray Trajectory Atomization

Based on Mathematical Analysis

Jian DU

1,*

, Gui-ling JU

1

, Li-juan DU

2

and Hui-zhen LI

1

1

Department of Fundamental, Army Academy of Armored Force, Beijing, China

2

School of Education, Minzu University of China, Beijing, China

*Corresponding author

Keywords: Trajectory automation, Thickness distribution model, Pattem search.

Abstract. The most important part of the spraying process is the paint film thickness uniform and how to plan the spray path. The paper is optimize the trajectory of spray gun by establishing mathematical model. Based on the analysis of the factors affecting the thickness distribution of paint film, establishing the thickness of single-trajectory spraying model, and analysis the relationship and surface geometry invariant to simplified the model, getting the optimal solution by using overlapping thickness model based on the movable surface, useing MATLAB to establish model of the curve surface. Then using projection to establish the thickness distribution model of any curve surface. Then use cloud sectioning to optimize the curve surface and establish the thickness of paint film in double trajectory.

Introduction

Glaze spraying process sprays glaze into the mist under compressed air with the glaze spray gun or glaze spray machine, so that the glaze adheres onto the clay body. It is a process easily realizing automation in the ceramic production process. As the uneven glaze will crack in the firing process, causing workpiece scrapping, so the thickness of the sprayed glaze in the spraying process is required to be uniform as far as possible.[1]

In actual air spraying, compressed air is usually arranged on both sides of the spray gun mouth, the mist cone is squashed into an elliptical cone, the region on the plane covered by the spray cone formed by the paint mist is an ellipse, the thickness of paint film meets elliptic double β distribution model in the elliptic distribution region. Atomization pressure1, diaphragm pump pressure and spray distance h are the main factors affecting the above parameters, and they accord with model of the spray gun spraying at a single point.The thickness of paint film in the middle of the spraying areais is bigger than other areas.When moving the spray gun, the mist cone will overlap in the adjacent paths.

The Cumulative Deposition Model of Single Channel Spraying

Based on the proposed ellipse bibeta model, the thickness of any point S in the spray area is the accumulation of the coating thickness during the spray gun moving above the spraying model at the speed of v when it comes to reality.[2]

[image:1.595.247.363.697.775.2]

As shown in Fig 1, we establish coordinates on the spray path, put the long axis of the elliptic region as X-axis, and the direction of the trajectory as Y-axis, which is in the same direction of elliptic spraying region.

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We assume that the increase of coating thickness of each point in the ellipse is proportional to time t, when the spray gun doesn’t move, the time required for the point S to pass through the elliptical spray area with a straight trajectory can be shown as follow:

[image:2.595.193.416.163.281.2]

According to the parameters obtained from the title a, b, beta 1, and beta 2, we use matlab to analyze the model, the analysis result is shown in Fig2.

Figure 2. The elliptical spray area.

Where: d -the width of twice overlapping thickness of paint film; d1 -Spray distance;

The overlapping film thickness of the workpiece surface point s is represented as Z(S)=Z(S1)+Z(S2) ; Z(S1)、Z(S2)-the cumulative thickness of the surface point S during the two spray trips.[3]

Because the height h is fixed,the key to get uniformity film thickness is to plan the reasonable v and the overlap width d. In response to this problem, we set up the optimization of function to attach the minimum sum of variance between the actual film thickness of S point Zs and ideal film thickness Zmax:

[image:2.595.229.383.477.568.2]

By summarizing actual spraying experience, we can determine the range of the unknown values. According to the above data,we can get the most optimal d and v by using MATLAB to calculate the least squares,and then get the width of spraying path according to the overlap width d.The effect of spraying trajectory on the plane is shown as Fig3.

Figure 3. Spraying ingtrajectory planning on fla.

The trajectory planning and optimization simulation of the plane are carried out on the basis of thickness distribution of paint film on the plane model.[4]The distribution model of the film thickness profile of the two-channel spraying process is shown in Fig 4.

[image:2.595.204.418.643.770.2]
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[image:3.595.157.452.171.262.2]

Put the parameters into the formula. In the MATLAB programming environment, we can get the most optimal solution by using least squares method to iteratively calculate the fitness function.[5]According to the ideal average thickness of paint film Zmax ,we find the thickness of paint film is in average when v=414.392mm/s, d=98.856mm. The optimized overlap interval of the spray gun trajectory is d1=146.134mm, and the thickness distribution of the paint film of double travel is shown as Fig5.

Figure 5. Simulation of spraying trajectory optimization of double travel.

The Spray Model of Spray Gun of One Point on Curve Surface

[image:3.595.233.367.352.465.2]

The spray gun of one point on curve surface is shown as follow:

Figure 6. The spraying trajectory optimization of double trave.

The thickness of paint film on tangent plane I,normal plane II and plane.III of point F. Plane III -the plane of the spray gun thickness model expressed in problem 1.γ-the angle of the normal vector n at point B and line GB. GE=h,GB=l, At point P, we establish the movable orthogonal frame {p;x,z,Z}.Z-axis:the normal direction of point P on the curve surface, also the short axis direction of the elliptic spray area; X-axis:the direction of ellipse long axis.[6]The model of paint film thickness on plane is shown in problem one,and the sedimentary thickness at point B is shown in the equation above. Now we need to compute the spray area on the curve surface, the spraying angle θ at point B and angle αof normal vector n and line GB. It is shown as Fig7.

Figure 7. The spray area on the curve surface.

[image:3.595.262.346.615.708.2]
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Combined with the superposition formula in problem one, taking any overlapping point P in the spray plane, and the thickness of film at point P is:

[image:4.595.223.384.151.278.2]

Take the equation above as fitness function to optimize d and v, and we can get the best d, we can get the optimal d by using MATLAB and least squares method, then get the width of spraying trajectory d1= 2a-d =160.34mm. It is shown as Fig 8.

Figure 8. Optimized spraying trajectory.

The Model of Thickness Distribution of Paint

[image:4.595.226.388.366.484.2]

First of all, we use MATLAB to creat the model of curved surface ,which is shown as shown Fig 9.

Figure 9. The thickness distribution of paint film.

Then we establish model of thickness distribution of paint film for any little curvature surface. Establish the XOY coordinate system with origin point O on the surface ,draw tangent plane M1 across point O, draw plane M2 paralleled with M1 across point P which is on the curved surface.(θp- spray angle of point P; hp’- spraying distance and stay fixed when spraying; hp-the distance from the spray gun to the plane M2; n-the normal vector of O2 on the ellipse surface; αp-angel of normal vector n and the line across point P and spray gun; lp-the distance of spray gun to point P).

It can creat a differential surface O3 ,the normal vector of which is consistent with the spraying direction, and O3 is in the same spraying area with differential surface O2. (Where:θp-the angle between O3 and point P in the direction of the long axis;β-the angle of the normal vector of surface O3 and the normal vector n of the surface O4,P,P’,P”differential surface O2 ,O3 ,O4.). I t is shown as Fig10.

[image:4.595.231.362.673.774.2]
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According to the relationship between the differential Combined with cloud section-cutting, we select parallel planes as slice plane and optimize the film thickness d and speed of spraying v aimed at getting the uniform thickness of film.

[image:5.595.229.372.145.266.2]

Firstly, we establish the model of film thickness distribution in double-trajectory spraying is shown as below: I t is shown as Fig11.

Figure 11. The film thickness distribution in double-trajectory spraying.

where:α-angle of the line across spraying boundary and spray gun; θp-spraying angel of spraying point; θp’-angle of the second spraying.

The distribution function of paint film thickness of P in single -trajectory spraying is:

Based on the equation above, we can get the paint film thickness distribution function of the point P in the two-trajectory spraying. (Zmax-the largest thickness of piant film in single-trajectory spraying) Because of the fixed height, the key to achieve average film thickness is programming logical v and overlapping width d. In response to this problem, we establish the optimization function in order to attain to the least sum of variance between actual film thickness Zs and ideal film thickness Zmax:Take the equation above as fitness function to optimize d and v, and we can get the best d, By summarizing actual spraying experience.

According to the above data, we can get the optimal d and v by using MATLAB and least squares method, then get the width of spraying trajectory d1= 2a-d according to the overlapping width d.After optimizing, we come to the conclusion: d=132.912mm,v=406.33mm/s.

Complicated Surface Segmentation

The height h is fixed, the key to get uniformity film thickness is to plan the reasonable v and the overlap width d.In response to this problem, we set up the optimization of function to attach the minimum sum of variance between the actual film thickness of S point Zs and ideal film thickness Zmax:

Using the above fitness function to optimize d and v, get the optimal solution. It is shown as Fig12.

Figure 12. Optimization of the gun trajectory at the junction

After the surface is sliced, the optimized d value and gun velocity v on each slice should remain unchanged.[7]However, in order to maintain the uniformity of the thickness of the coating at the two junctions, the gun velocity v near the boundary needs to be optimized. The figure below shows the three positional relationships of the gun space path at the junction with the boundary line:

[image:5.595.216.383.592.669.2]
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to the boundary. Suppose the angle between two faces is α, the distance between the path and the boundary line is h. The coating thickness at the junction of two points Z:

The figure above shows the case where the path is vertical-parallel. At this time parallel nozzle gun rate v unchanged, but the vertical spray gun rate needs to be optimized. Use path segmentation to optimize gun velocity on each segment.

The vertical path is divided into 9 ends, which are P1, P2, P3 and P4 ...Each length is d0.P2, P5 and P8 are respectively divided into i +1.The corresponding gun rate is v0,...,vi.P1, P6, P7 are divided into k segments, corresponding rates are vi+1,vi+2, ...vi+k. In the figure, the x axis is established by P3 and P4, and the vertical line connecting the vertical end is the axis of the Y-axis. The formula of coating thickness is obtained from the upper type to get the spray gun along the path 1:Spray gun along path 2 coating thickness equation: The y1 is the distance from S to path 2.The thickness of the point S is: We can get the optimal function by combining the trajectory optimization function of spray gun.

This is an optimization problem of multi-decision variables. The variables are h1, h2, and v0... vi+k and the problem can be solved using the schema search method. This formula can be used to optimize the planning of any surface spray path.

References

[1]Yang Qingchao, Sun Fangxu, Chai Kai, et al. Study on Evolution and Crisis of Chaos Attractor in Strongly Nonlinear System Based on PMUCR Method[J], Journal of Ordnance Equipment Engineering, 2016, (9), pp. 138-141.

[2]Chen Y.H, Dong F.H. Robot machining: recent development and future research issues. International Journal of Advanced Manufacturing Technology, 2013, 66, pp. 1489-1497.

[3]Dong Liying, Jiao Zhigang, Wang Zhijun, et al. Simulation Analysis of Ballistic Trajectory of Projectile Based on Matlab[J].Journal of Ordnance Equipment Engineering, 2017, (12), pp. 98-101.

[4]Andulkar M V, Chiddarwar, S. S. Incremental Approach for Trajectory Generation of Spray Painting Robot. The Industrial Robot. 2015, 42, (3), pp. 228-241.

[5]Zhang Haoran, Yi Wenjun, Guan Jun, et al. Research on Rocket Projectile Ballistic Parameters Measurement Based on MEMS/BD[J].Journal of Ordnance Equipment Engineering, 2017, (9), pp. 41-47.

[6]Denavit, J RS H.A Kinematic Notatton for Lower-Pair Mechanisms[J], 2005.22, (2), pp. 45-46.

Figure

Figure 1. Schematic diagram of spraying trajectory on flat.
Figure 3. Spraying ingtrajectory planning on fla.
Figure 6. The spraying trajectory optimization of double trave.
Figure 8. Optimized spraying trajectory.
+2

References

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