Magnus effect on a rotating soccer ball

Flight of the famous free kick taken by Roberto Carlos in the 1997 Soccer Photograph: Tony Marshall/Empics Sport, Image source Comsol and www.theguardian.com

Author: Midhun Murali Mohan

Introduction 
The flight of a ball is vital across various sports, including soccer, golf, baseball, cricket, tennis, and volleyball. Research into the aerodynamics of sports balls traces back to 1672 when Newton observed deviations in tennis ball flight. Important fluid mechanics principles encompass boundary layer flow, turbulence, rough surface effects, the Magnus Effect, and wake characteristics. Mastery of these concepts’ benefits equipment designers, players, coaches, and governing bodies. 

In soccer, knowing how the ball moves through the air helps us understand its range, trajectories, and deflections, with or without spin. The Magnus Effect, which makes spinning balls curve, is greatly influenced by the ball’s surface texture. Thanks to advancements in computational power, Computational Fluid Dynamics (CFD) has become an essential tool for analysing the aerodynamics of sports balls. CFD technology allows us to better understand and compare airflow around various sports balls, influencing how sports equipment is designed and performs. 

The Magnus Effect 
During matches, spinning sports balls alter their trajectory. Side spin induces lateral movement, top spin causes downward trajectory, and backspin results in upward lift. When spinning, factors like lift coefficient (FL) and side force coefficient (FS) alongside drag coefficient (FD) are relevant due to the Magnus Effect. This effect is depicted in Fig. 1 for a ball with side spin moving from right to left (as seen from above). In the absence of spin, streamlines would symmetrically flow around the ball. However, spinning rotates the air around it, increasing velocity at point A and decreasing it at point B. This asymmetry leads to delayed separation at the top and early separation at the bottom, creating an uneven wake. The pressure difference between points A and B generates a sideways Magnus Force (FM) acting on the ball. 

Fig. 1 The Magnus Effect for a ball moving from right to left with sidespin (top view) (S. Barber et al [1]) 

Rotating soccer ball Experimental Investigations 
The Magnus effect exhibited on a prototype soccer ball, rotating perpendicular to the flow direction across various Reynolds number ranges, can be explored through aerodynamic force measurements and a survey of the flow field. Experiments were conducted by Thorsten Kray et al [2] using a rear sting support system, wherein the soccer ball was divided into two halves, each powered by an internal motor. Even when stationary, the force coefficients varied within the range observed in real soccer balls alongside boundary layer separation points. As depicted in Fig. 2, the prototype soccer ball, having a diameter of 226 mm, was affixed to an ‘L’-shaped sting featuring a NACA 0015 wing vertical section. Propelled by an internal DC motor, the ball halves could rotate at speeds of up to 540 rpm. This aluminium alloy ball, resembling the design of the 2006 World Cup Teamgeist ball, was adorned with 14 textured panels featuring triangle-based pyramidal peaks and valleys. 

Fig. 2 (a) Installation photograph of the ball-halves set-up with the textured 14-panel model; (b) spinning mechanism including constructional details (Thorsten Kray et al [2]) 

Forces were measured using a six-component wind tunnel balance, recording drag force FD, side force FS, and Magnus force FM as lift in the z-direction, with positive force corresponding to negative z-direction lift.  

Fig. 3 Aerosol visualizations of the flow around the soccer ball-halves (Thorsten Kray et al [2]) 

Numerical study of the erratic motion of soccer balls 
Using CFD analysis, researchers S. Barber et al [3]. effectively compared the aerodynamics of different soccer balls. By examining various scanned and modified soccer balls, they discovered that the drag coefficient (FD) remained consistent across different designs. However, the lift coefficient (FL) and side force coefficient (FS) varied significantly depending on the ball’s orientation and type. This variation was attributed to the asymmetrical geometry affecting the separation around seams. When these variations were approximated and inputted into trajectory simulation programs, the balls displayed distinct behaviours and erratic trajectories at spin rates below 2 revolutions per second. The study concluded that the surface geometry of a soccer ball significantly impacts its trajectory, with consistently performing balls achieving an optimal combination of amplitude and frequency of varying force coefficients relative to the applied spin. 

Fig. 4 (a) Example of CFD flow visualisation, (b) example of wind tunnel tests, (c) example of trajectory measurements S. Barber et al [3] 

The famous free kick by Roberto Carlos in the 1997 Soccer Confederations Cup was scientifically explained by Asai et al [4]. The sideways deviation of the ball, rotating around an axis perpendicular to its flight direction from its initial straight path, is attributed to the ordinary Magnus effect. Additionally, the negative Magnus effect, which involves the reversal of the side force within a specific range of Reynolds numbers and spin parameters, also plays a role.

Fig.5 Flight of the famous free kick taken by Roberto Carlos in the 1997 Soccer (Image source www.thesun.co.uk

Watch the famous free kick !!!

Conclusion 
The aerodynamics of soccer balls is incredibly intriguing, not only because of the variety of kick types and trajectories but also due to recent advancements in manufacturing techniques. These innovations have enabled greater flexibility in designing and structuring the ball’s surface. The most reliable soccer balls strike an ideal balance between maximum force coefficient and frequency relative to the spin applied. Enhancing a ball’s consistency with flow visualizations and computational fluid dynamics (CFD) seems entirely possible. The future of soccer ball design is set to be both thrilling and controversial. 

References:  

  1. S. Barber, and M.J. Carr´e. “Soccer Ball Aerodynamics Book Chapter Computational Fluid Dynamics for Sport Simulation ” Springer-Verlag Berlin Heidelberg 2009. 
  2. Thorsten Kray, Jörg Franke and Wolfram Frank. ” Magnus effect on a rotating soccer ball at high Reynolds numbers.” Retrieved September 30, 2001. 
  3. S. Barber, Chin, S.B, Carré, M.J.” Sports ball aerodynamics: a numerical study of the erratic motion of soccer balls”. Comput. Fluids 38 (6), 1091–1100 2009. 
  4. Asai, T, Seo, K Kobayashi, O, Sakashita, R.” Fundamental aerodynamics of the soccer ball. Sports Engineering 10 (2)”, 101–109 2007. 
  5. Bush, J.W.M., “The aerodynamics of the beautiful game, 2013. In Sports Physics, Ed. C. Clanet, Les Editions de l’Ecole Polytechnique”, pp. 171-192 2013. 


Related Articles

The Marvel of Backspin: How Fast Bowlers Harness Late Swing in Cricket

Swing in cricket fast bowling refers to the lateral movement of the ball in flight, creating a deviation from its original path. This movement can occur in two directions: inswing, where the ball veers towards the batter’s onside, and outswing, where it moves towards the offside. Mastering the art of swing can significantly impact a match by limiting scoring opportunities and increasing the likelihood of dismissals.

At the beginning of an innings, fielding teams are provided with a new ball, characterized by its smooth leather surface and prominent seam, making it ideal for conventional swing. To achieve swing, bowlers must combine skill, precision, and experience. The ball is delivered at high speed with the seam angled slightly upright, and the bowler’s index and middle fingers positioned on either side of the seam. A slight backspin is applied to the ball, creating gyroscopic stability that maintains the seam’s orientation during flight. Without a steady seam position, the ball fails to generate swing, underscoring the importance of this technique.

The Y Plus Concept: Key to Boundary Layer Analysis

When we think about the sleek design of modern aircraft, our focus often turns to their impressive speed, fuel efficiency, and advanced technology. Yet, there exists an unseen force that significantly influences these attributes: the boundary layer, a thin region in which viscous forces are significant and within which the flow is rotational. This thin layer of air adhering to the aircraft’s surface plays a pivotal role in key aerodynamic factors such as drag, lift, and heat transfer.

Computational Fluid Dynamics in Swimming

In the quest for excellence in competitive swimming, athletes and coaches are constantly searching for innovative methods to enhance performance and gain a competitive edge. One of the most significant advancements in sports engineering has been the application of Computational Fluid Dynamics (CFD), which has revolutionized the way swimmers approach training and competition strategies. At its core, swimming is a battle against the resistance of water, and success depends not only on a swimmer’s physical strength and technique but also on how effectively they navigate through the water. By simulating how water flows around a swimmer’s body, CFD provides a detailed analysis of drag, lift, and turbulence, crucial factors impacting performance and speed. For better swimming performance, the hydrodynamic drag force resisting motion should be minimized and the propelling force maximized at the same time. The hydrodynamic drag force on a swimmer can be divided into three components: the friction drag due to the viscosity of water, the form drag due to the complex form of the swimmer’s body and the wave drag due to the interaction of the swimmer with the free surface.

Ernst Mach

Prof. Ludwig Prandtl is known as a physicist who revolutionized fluid dynamics with his notion that the effect of friction is experienced only very near an object moving through a fluid. The modern fluid dynamics and aerodynamics world is based on this great scientist’s idea. His seminal paper which he presented in 1904 at the third international mathematics congress in Heidelberg is regarded as equivalent to that of the seminal paper of Albert Einstein and deserved a Nobel Prize in classical physics.

Responses

Your email address will not be published. Required fields are marked *

error: Content is protected !!
Select your currency