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Proceeding Paper

One-Way Fluid Structure Interaction of a Go-Kart Spoiler Using CFD Analysis †

by
Mohammad AL-Rawi
1,* and
Abderrahmane Oumssount
2
1
Centre of Engineering and Industrial Design, Waikato Institute of Technology, Hamilton 3240, New Zealand
2
JP Marshall Engineering, Hamilton 3200, New Zealand
*
Author to whom correspondence should be addressed.
Presented at the 13th Conference of the International Sports Engineering Association, Online, 22–26 June 2020.
Proceedings 2020, 49(1), 51; https://doi.org/10.3390/proceedings2020049051
Published: 15 June 2020

Abstract

:
The spoiler on a go-kart is required to prevent the vehicle becoming airborne at speeds of 80 km/h or more. An optimal spoiler design balances this safety aspect with speed and fuel economy. This paper reports the results of a project to improve the aerodynamic aspects of a go-kart spoiler design using CFD Analysis. We investigated the design of a rear spoiler with three proposed angles ( θ 1 = 9.5 ° ,   θ 2 = 19.5 ° ,   θ 3 = 29.5 ° ). The drag force produced by each of the three designs is compared. Different computational results are discussed such as the air flow velocity, pressure and the applied forces in terms of CFD analysis using one-way fluid structure interaction (one-way FSI) to determine the spoiler stress, strain and drag coefficient. The findings of this paper have implications for the leisure and tourism industries, and may be applicable to other recreational vehicles’ spoilers.

1. Introduction

Go-karts are very popular recreational vehicles suitable for a wide variety of ages [1]. The vehicles must be safe, fuel efficient, but able to obtain sufficient speed to be entertaining to the user. The focus of current sports engineering research is to improve the efficiency of the aerodynamic shape of the vehicle and minimize accidents. Given that the kart speed varies from 45–90 km/h, a strong chassis and rear spoiler prevent the kart from flying at top speed [1]. However, many improvements will impact on the performance of the kart at the desired speed ranges [2,3,4]. A rear spoiler acts like plane wings but in a reversed way: where the plane wings provide lift forces, the spoiler provides down forces. These down forces allow the vehicles to travel faster and turn corners more safely by increasing the vertical loads on the tires, thereby increasing the grip. Without a spoiler, the bodyweight of the cart would have to be increased to prevent it flying off the track, which decreases fuel consumption efficiency. Rear spoilers also compensate for the adverse effects of the body shape in competitive sports vehicles, where other elements of the vehicle design are dedicated to enhancing the existing favorable properties of the vehicle [5,6]. Spoilers also reduce drag forces that may cause vehicle instability and poor handling [5,6]. Much of the literature is devoted to improving the aerodynamic efficiency of spoilers in cars [1,2,3,5,6]. This paper focuses on aerodynamic efficiency of spoilers applied to go-karts.
The main objective of this study is to investigate the drag coefficient produced by the spoiler tilted to one of three different angles: θ 1 = 9.5 ° ,   θ 2 = 19.5 ° ,   and θ 3 = 29.5 ° with respect to the supports on the kart (Figure 1). This paper generates and discusses different results for the air flow, pressure and applied forces obtained by the CFD modeling and the spoiler stress and the drag coefficient obtained from the FE analysis using the one-way FSI method.

2. Materials and Methods

2.1. CFD Setup and Analysis

In this project, CFD analysis is performed using SolidWorks flow simulation tools. This provides results for fluid flow velocity, forces and pressure that closely approximate real life events. The proposed spoiler is constructed in SolidWorks to fit on our go-kart project as shown in Figure 1. The drawing dimensions for the SolidWorks file are shown in Figure 2, which demonstrates the general assembly of the 3D model. Three spoiler designs are investigated, each having a different angles of 9.5°, 19.5° and 29.5°, as shown in Figure 3. The designs are compared in terms of drag coefficient to avoid flying accidents while speeding.
The computational simulation is set to an external flow (Air), and includes gravity in the y-direction with a value of −9.81 m/s2, and air flow velocity of 80 km/h in the z-direction. The boundary conditions are set to the following computational domain; x = 1.1933, y = 0.458 and z = 1.0337 m. Additionally, we set the following goals to monitor and capture the simulation results: average velocity, forces in x, y and z direction and the drag coefficient, C d , equation into SolidWorks.
C d = F ρ A v 2 2
where, force (F) is in N, fluid density ( ρ ) is in kg/m3, average velocity   ( v ) is in m/s and the reference area (A) is in m2. The mesh is set using the global setting with uniform mesh and value of 0.169 m for the minimum gap size with a 3 ratio factor and the level of initial mesh set to 5. The CFD simulation generates the air flow results as force impacting on the front face of the spoiler which will be exported into the FE analysis as a one-way FSI to present the pure mapping of the physical air flow properties.

2.2. FE Analysis

Finite element analysis (FEA) is the part of the SolidWorks suite of simulation tools that deals with solid objects. FEA is used to measure the stress and strain on the spoiler due to the air flow resulting from the CFD analysis. This air flow is imported as an inlet force facing the spoiler using flow effects option. This will generate fluid shear stress in the x, y and z directions.
The spoiler material is set to ABS, considered the most realistic material for modelling applying the cost effectiveness criterion. The material could be modeled as manufactured from fiber glass or carbon fiber, but these are more expensive materials so unlikely to be applied in most leisure-operator settings. ABS spoilers are mechanically strong, resistant to cracking or deforming due to the wind flow forces. Figure 3 shows how the constructed spoiler is modeled fixed at the base support at the three angles described in Section 2.1 above.
The FE mesh is set to fine standard type mesh with parameter values: global size (5.25 mm) and tolerance (0.262 mm) as shown in Figure 4.

3. Results and Discussion

The CFD results for pressure and velocity for the three proposed designs ( θ 1 = 9.5 ° ,   θ 2 = 19.5 ° ,   and θ 3 = 29.5 ° ) are shown in Figure 5. This figure demonstrates the pressure impacting on both sides of the spoiler (front and back) and shows the flow streamline passing the spoiler to calculate the drag coefficient.
The drag coefficient (Cd) of the same spoiler at three different angles—9.5 ° , 19.5 ° and 29.5 ° —is investigated and the results of the air flow are exported to the FE Analysis. The air flow is then set up as an external force impacting on the spoiler using the one-way FSI method. Figure 6 shows the von Mises stresses (the maximum distortion energy) which indicates the yielding point for the ductile material for the 9.5 ° design. This design produces the least drag of the three designs with a Cd of 0.65. Additionally, after passing the spoiler, the air flow kept straight and did not show turbulent behavior, as shown in Figure 5.
The von Mises stress result is assessed to the maximum yield strength for the ABS material which should not exceed 30 MPa. From Figure 6, the 9.5 ° von Mises stress analysis shows that the maximum is 1.386 MPa, which occurred in the support due to the 4.5 N wind force in the z-direction and 17 N downward force in the y-direction. The center of the spoiler recorded a 0.36 MPa von Mises stress, which still did not impact on its structure. For the strain, the highest deflection, 0.48 mm, was recorded in the center of the spoiler. The supports’ reaction forces to stabilize the spoiler reached 15.654 N, which is safe as it is greater than the body weight.
The 19.5 ° spoiler produced the second highest drag between all the designs with a Cd value of 0.89. Figure 5 indicates that the air flow after passing the spoiler had a higher pressure drop from an atmospheric pressure to 101.19 KPa, and which would create greater turbulence compared to the 9.5 ° design.
The center of the spoiler recorded a 0.4 MPa von Mises stress, which still did not impact its structure. For the strain, the center of the spoiler recorded the highest deflection, of 0.45 mm. The supports’ reaction forces to stabilize the spoiler reached 16.8 N, which is safe as it exceeds the body weight.
Finally, the 29.5 ° spoiler produced the highest drag between all the designs with a Cd value of 1.26. As with the 19.5 ° spoiler, the pressure dropped from an atmospheric pressure to 101.19 kPa. Figure 5 shows the air flow simulation, including where it contains a higher dead zone with a higher turbulence than the other designs.

4. Conclusions

In conclusion, a spoiler tilted to one of three different angles relative to the supports is investigated. The drag coefficient and mechanical properties were analyzed to identify the most suitable angle to which the spoiler may be tilted on a go-kart operating at a speed of 80 km/h. The most promising design was the 9.5 ° angle, which contains the least drag, with a Cd of 0.62, defined within the air flow forces and the reference area. This design also generates a maximum stress of 1.386 MPa and its minimum strain is 0.45 mm. The supports’ base reaction force was also the lowest with a drag force of 15.64 N.

References

  1. Akash, C.R.; Tushar, S.; Raghvendra, K.M. Design and Development of Foldable Kart Chassis. In Proceedings of the 4th International Conference on Materials Processing and Characterization, Andhra Pradesh, India, 14–15 February 2015; Volume 2, pp. 1707–1713. [Google Scholar]
  2. Estrada, G. Mercedes-AMG GTR: Aerodynamics for the Record. In Progress in Vehicle Aerodynamics and Thermal Management; Wiedemann, J., Ed.; FKFS: Stuttgart, Germany, 2017; Springer: Cham, Switzerland, 2017; pp. 135–144. [Google Scholar]
  3. Wahl, G. 918 Spyder–the impulse source for future sports car concepts. In Munich Chassis Symposium 2014; Springer: Wiesbaden, Germany, 2014; pp. 35–56. [Google Scholar]
  4. Meder, J.; Wiegand, T.; Pfadenhauer, M. Adaptive aerodynamics of the new Porsche 911 Turbo. In ATZ Worldwide 2014; Springer Fachmedien: Wiesbaden, Germany, 2014; Volume 116, pp. 42–45. [Google Scholar]
  5. Gönüldinc, O.; Hölzel, S. Adaptive Aerodynamik–Innovation des Porsche 911 Turbo; Springer: Wiesbaden, Germany, 2014; pp. 159–174. [Google Scholar]
  6. McBeath, S. Competition Car Aerodynamics, 3rd ed.; Veloce Publishing Ltd.: Bondbury, UK, 2015. [Google Scholar]
Figure 1. Go-kart project: (Resource Wintec).
Figure 1. Go-kart project: (Resource Wintec).
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Figure 2. Spoiler dimensions and details.
Figure 2. Spoiler dimensions and details.
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Figure 3. Types of spoilers investigated with three different angles: (a) 9.5 °   Spoiler; (b) 19.5 ° Spoiler; (c) 29.5 ° Spoiler.
Figure 3. Types of spoilers investigated with three different angles: (a) 9.5 °   Spoiler; (b) 19.5 ° Spoiler; (c) 29.5 ° Spoiler.
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Figure 4. Mesh for the 9.5 ° spoiler: (a) side view; (b) isometric view.
Figure 4. Mesh for the 9.5 ° spoiler: (a) side view; (b) isometric view.
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Figure 5. The Air flow simulation around the three designs of spoilers having angles of 9.5 ° , 19.5 ° and 29.5 ° .
Figure 5. The Air flow simulation around the three designs of spoilers having angles of 9.5 ° , 19.5 ° and 29.5 ° .
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Figure 6. von Mises stress analysis of 9.5 ° spoiler.
Figure 6. von Mises stress analysis of 9.5 ° spoiler.
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MDPI and ACS Style

AL-Rawi, M.; Oumssount, A. One-Way Fluid Structure Interaction of a Go-Kart Spoiler Using CFD Analysis. Proceedings 2020, 49, 51. https://doi.org/10.3390/proceedings2020049051

AMA Style

AL-Rawi M, Oumssount A. One-Way Fluid Structure Interaction of a Go-Kart Spoiler Using CFD Analysis. Proceedings. 2020; 49(1):51. https://doi.org/10.3390/proceedings2020049051

Chicago/Turabian Style

AL-Rawi, Mohammad, and Abderrahmane Oumssount. 2020. "One-Way Fluid Structure Interaction of a Go-Kart Spoiler Using CFD Analysis" Proceedings 49, no. 1: 51. https://doi.org/10.3390/proceedings2020049051

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