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Optimization Design of a Wedge Gate Valve Plate Based on RSM

Nov 12, 2025
Teresa
Optimization Design of a Wedge Gate Valve Plate Based on RSM
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Abstract
This study focuses on the wedge gate valve plate and employs Response Surface Methodology (RSM) to optimize its structural parameters. The mass, maximum stress, and maximum deformation of the valve plate under maximum static pressure were selected as response variables. Sensitivity analysis was performed on the structural parameters of the valve plate. After sampling the design variables using the Latin hypercube algorithm, an orthogonal experimental design was conducted. A genetic algorithm was then employed to fit the response surface prediction model. Minimizing the mass, stress, and deformation was defined as the optimization objective. A multi-objective genetic algorithm was then applied to solve the optimization problem based on the prediction model. The results indicate that after optimization, the mass of the valve plate was reduced by 2.53%, the maximum stress by 4.9%, and the maximum deformation by 17%, significantly improving its self-sealing performance. For the structural parameter optimization of a wedge gate valve plate, combining parameter sensitivity analysis with RSM allows for the rapid and effective identification of the optimal design solution. The optimized gate plate demonstrates enhanced operational stability and improved sealing reliability.

 

1. Overview

Wedge gate valves are widely employed in valve systems for oil pipelines, pressurized water pipelines, and gas transmission networks. The sealing performance of the valve directly influences the safety and transport efficiency of the entire pipeline system. Extensive research on valve optimization has been conducted both domestically and internationally. Liu Peng et al. proposed a method combining comprehensive fluid characteristic analysis with sensitivity evaluation to optimize subsea gate valves. They conducted orthogonal experiments on key valve parameters to enhance peak flow velocity and reduce maximum gate deformation. Ali Rezghi et al. performed multi-objective optimization on the closing characteristics of a turbine gate valve and the position of the pressure regulating box in an overpressure water pump, achieving a significant reduction in pump overspeed. Ni Hongjun et al. conducted numerical simulation and warpage analysis of the compression molding process for fluoropolymer-lined valve bushings, optimizing dimensional accuracy and reducing the number of production trials required. Zhang Bo et al. optimized the flow channel structure of electronic water valves for new energy vehicles using CFD simulations, effectively reducing both direct-flow and bypass pressure drops. Yang Xiaobo et al. carried out three-dimensional modeling and finite element simulations of supercritical valves, using statistical analysis methods to optimize their structural parameters. In valve structural optimization, it is common to define specific valve performance characteristics as optimization objectives and to adjust multiple dimensional parameters to achieve an optimal design configuration. However, when the number of design variables is large, the optimization process often incurs high computational demands and extended development cycles. In this study, a static analysis of a wedge gate valve under maximum design pressure in the fully closed state was performed. Sensitivity analysis of the key structural parameters of the gate was first conducted using ANSYS software, and the parameters exhibiting high sensitivity were selected as design variables. An orthogonal experimental design was subsequently conducted using the Latin hypercube sampling method. The response surface prediction model was fitted using a genetic algorithm, and a multi-objective genetic algorithm was then applied to simultaneously minimize mass, stress, and deformation. Finally, simulation verification confirmed the validity of the optimized design scheme. The results demonstrate that combining sensitivity analysis with response surface methodology can accurately identify the key design variables of the gate, effectively reducing computational workload and shortening the optimization process. The optimized design significantly improves the self-sealing performance and operational stability of the wedge gate valve.

 

2. Process Analysis of the Wedge Gate Valve

Figure 1 presents the three-dimensional model of the wedge gate valve, which primarily comprises a handwheel, valve bonnet, valve body, valve stem, and wedge gate plate. The rising valve stem typically adopts a trapezoidal thread. Through the nut at the top of the valve and the guide groove on the valve body, the rotational motion of the handwheel is transformed into linear motion, driving the wedge gate plate to move vertically to open or close the valve. The wedge gate plate is made of HT300 gray cast iron and is designed for a maximum working pressure of 2.2 MPa within an operating temperature range of 10–200 °C. During the sealing performance test, a pressure of 1.1 times the maximum allowable working pressure is applied. The material properties of the gate plate are summarized in Table 1.

 

Table 1 Material parameters of the wedge gate valve plate

Parameter

Elastic Modulus E (GPa)

Density (kg/m³)

Poisson’s Ratio

Value

130

7300

0.25

Structural schematic of the wedge gate valve

Figure 1 Structural schematic of the wedge gate valve

 

3. Static Simulation Analysis of the Base Structure

The static analysis of the wedge gate plate was carried out using ANSYS. The model was discretized into a mesh consisting of 160,809 elements and 252,201 nodes. As illustrated in Figure 2(a), frictional constraints with a coefficient of 1.3 were applied to the contact edges of the gate plate. As shown in Figure 2(b), a pressure of 2.4 MPa was applied to the opposite surface to simulate the self-sealing test water pressure. The simulation results are presented in Figures 2(c) and 2(d). The maximum deformation occurs at the center of the gate plate, measuring 0.347 mm. The maximum equivalent stress occurs at the root of the central flange, reaching 162.33 MPa. The total mass of the wedge gate plate is 13.836 kg.

Static analysis of the base structure of the wedge gate valve

(a) Schematic of constraint application (b) Schematic of pressure loading
(c) Stress distribution cloud diagram (d) Displacement distribution cloud diagram

Figure 2 Static analysis of the base structure of the wedge gate valve

 

4. Sensitivity Analysis of Valve Plate Structural Parameters

The key structural parameters of the wedge gate plate are illustrated in Figure 3. Sensitivity analysis of these parameters was performed using ANSYS Workbench in combination with SolidWorks. The corresponding sensitivity values for each structural parameter are presented in Figure 4. Direct optimization of the full model would result in a high computational load and prolonged optimization time. Therefore, parameters exhibiting low sensitivity in the mass, stress, and deformation responses were excluded. Only parameters with higher sensitivity values were selected for orthogonal experiments, effectively reducing the computational scale while retaining the most influential factors. Based on the sensitivity diagram, the key structural parameters D1, D2, D4, D5, D6, and D7 were identified and selected as the design variables for the subsequent orthogonal experimental design.

Structural parameter definitions of the wedge gate valve plate

Figure 3. Structural parameter definitions of the wedge gate valve plate

Sensitivity diagram of design parameters
Figure 4. Sensitivity diagram of design parameters

 

5. Latin Hypercube Experimental Design and Results

The Design Exploration module in ANSYS was employed for the Design of Experiments (DOE) study, and the Latin hypercube sampling algorithm was used to generate sample points for each design variable. This algorithm efficiently captures the true characteristics of the model using fewer sample points, significantly reducing computational effort while maintaining accuracy. A portion of the DOE experimental data and the corresponding results are presented in Table 2.

Table 2. DOE experimental scheme and results

No.

D1 (mm)

D7 (mm)

D6 (mm)

D5 (mm)

D4 (mm)

D2 (mm)

Mass (kg)

Deformation (mm)

Stress (MPa)

1

13.627

153.013

4.956

208.533

9.720

30.533

13.806

0.111

161.180

2

14.187

159.724

5.444

221.822

8.280

30.933

12.925

0.132

160.730

3

12.631

151.671

4.822

231.022

8.960

32.400

13.300

0.127

170.582

4

13.876

139.591

4.778

222.844

8.200

29.067

14.405

0.105

160.632

5

12.756

136.236

4.867

238.178

9.760

28.667

14.219

0.112

162.868

44

13.067

137.578

5.333

237.156

8.240

27.467

14.087

0.338

160.910

45

14.560

163.751

5.222

215.689

9.280

32.267

12.792

0.401

191.189

 

6. Response Surface Fitting

The Genetic Aggregation Algorithm was employed to fit the response surfaces of mass, maximum deformation, and maximum stress based on the DOE experimental data. As shown in Figure 5(a), under the optimized mass conditions, when D7 is at a high level, the mass increases as D2 decreases; conversely, when D2 is at a high level, the mass also increases with increasing D7. In Figure 5(b), when D5 is at a high level, an increase in D7 has a relatively minor effect on the mass. However, when D5 is at a low level, an increase in D7 has a more pronounced effect, indicating a strong positive correlation between these two parameters and the mass. Under the optimized maximum deformation conditions, as shown in Figure 6(a), when D2 is at a low level and D7 increases within the range of 140–155 mm, the effect on maximum deformation is minimal. However, when D7 increases within the range of 155–165 mm, its effect on deformation becomes more pronounced. In Figure 6(b), when D6 is at a low level and D5 increases from 210 to 235 mm, the maximum deformation rises sharply. As D5 continues to increase beyond 235 mm, the rate of deformation growth slows, indicating a nonlinear relationship between these two parameters. As shown in Figure 7(a), under the optimized maximum stress conditions, D5 is positively correlated with the maximum stress value. As D5 increases, the maximum stress also rises. When D2 varies gradually, the maximum stress initially decreases and then increases, exhibiting a U-shaped trend. In Figure 7(b), as D5 increases, the maximum stress again exhibits a trend of initially decreasing and then increasing. In contrast, as D6 decreases, the maximum stress first rises and then falls, indicating complex interactive effects between these parameters.

3D response surface plots of mass under different parameter combinations

Figure 5. 3D response surface plots of mass under different parameter combinations
(a) Interaction between D7 and D2 (b) Interaction between D7 and D5

3D response surface plots of maximum deformation under different parameter combinations

Figure 6. 3D response surface plots of maximum deformation under different parameter combinations
(a) Interaction between D7 and D2 (b) Interaction between D5 and D6

3D response surface plots of maximum stress under different parameter combinations

Figure 7. 3D response surface plots of maximum stress under different parameter combinations
(a) Interaction between D5 and D2 (b) Interaction between D5 and D6

 

7. Multi-Objective Genetic Algorithm Optimization

In the structural optimization of the wedge gate plate, the objectives of minimizing mass, maximum deformation, and maximum stress are inherently conflicting, making it challenging to achieve simultaneous optimal performance across all three criteria. To address this challenge, a multi-objective genetic algorithm (MOGA) within the Design Exploration module of the ANSYS platform was employed to optimize the structural parameters of the wedge gate plate. The optimization objectives were defined as follows:

The formula

 

8. Optimization Results and Verification

Using the response surface prediction model, the minimum mass, minimum deformation, and minimum stress were set as the optimization objectives, and iterative solutions were carried out. A sample solution set is presented in Figure 8. When all objective responses simultaneously reached their optimal values, the corresponding input parameters were:

D1 = 15.134 mm, D7 = 146.67 mm, D6 = 4.5462 mm, D5 = 213.85 mm, D4 = 9.8408 mm, D2 = 28.518 mm

The corresponding output responses were:

Mass = 14.258 kg, Maximum Deformation = 0.31545 mm, Maximum Stress = 154.18 MPa

For practical engineering applications, the optimized structural parameters were rounded as follows:

D1 = 15.1 mm, D7 = 146.7 mm, D6 = 4.5 mm, D5 = 213.9 mm, D4 = 9.9 mm, D2 = 28.5 mm

Table 3. Comparison of Wedge Gate Valve Structural Parameters Before and After Optimization

Item

Mass (kg)

Maximum Deformation (mm)

Maximum Stress (MPa)

Original Design

13.836

0.34748

162.33

Response Surface Optimization

10.341

0.28545

154.18

Simulation Verification

10.336

0.28742

154.23

Percentage Reduction

2.53%

17%

4.9%

 

Analysis of the optimized structural parameters indicates that the reduction in mass of the wedge gate valve is mainly attributable to the suboptimal nature of the initial design. The optimization process rationalized the valve geometry, enhancing self-sealing performance, making the structure more compact, and meeting overall performance requirements.

Sample solution set diagram from the multi-objective optimization

Figure 8. Sample solution set diagram from the multi-objective optimization

 

8. Conclusion

This study treated the geometric structural parameters of a wedge gate valve as design variables, with mass, maximum stress, and maximum deformation defined as the optimization objectives. Orthogonal experimental analysis was performed using ANSYS, and response surface prediction models were developed for each objective to characterize the influence of each geometric parameter on valve performance. By combining sensitivity analysis with response surface methodology within the ANSYS Design Exploration module, multi-objective optimization of the wedge gate valve was carried out using a multi-objective genetic algorithm. This approach enabled the rapid and accurate identification of the optimal parameter combination. The optimized design achieved a 2.53% reduction in mass, a 17% reduction in maximum deformation, and a 4.9% decrease in maximum stress, significantly enhancing the self-sealing performance and overall operational reliability of the wedge gate valve.

Teresa
Teresa
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Teresa, a senior editor and technical expert in the field of industrial valves, focuses on writing and analyzing valve technology, market trends, and application cases. She has more than 8 years of experience in industrial valve design and application. Her articles not only provide detailed technical interpretations but also combine industry cases and market trends to offer readers practical reference materials. She has extensive knowledge and practical experience in the field of valves. She has participated in many international projects and provided professional technical support and solutions for industries such as petrochemicals, power, and metallurgy. In her spare time, Teresa enjoys reading scientific and technological literature, attending technical seminars, and exploring emerging technology trends to maintain a keen insight into industry dynamics.
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