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Abstract Have you ever wondered why golf balls have a pattern of dimples on their surface? The dimples are important for determining how air flows around the ball when it is in flight. The dimple pattern, combined with the spin imparted to the ball when hit by the club, greatly influence the ball's flight path. For example, backspin generates lift, prolonging flight. When the ball is not hit squarely with the club, varying degrees of sidespin are imparted to the ball. A clockwise sidespin (viewed from the top) will cause the ball to veer right (or slice). A counterclockwise sidespin will cause the ball to veer left (or hook). This project attempts to answer the question, "Can an asymmetric dimple pattern decrease hooks and slices?"Objective The goal of this project is to test whether an asymmetric dimple pattern on golf balls can produce straighter flight. Introduction The dimples on the surface of a golf ball are there for a reason. A golf ball with a smooth surface would only travel about half as far as the dimpled ball. Why is this so? The answer has to do with the flow of air over the ball when it is in flight. When a solid object moves through a gas (or a fluid), the gas pushes back on the solid. In aerodynamics (or fluid mechanics) this resistive force is called drag. The dimples on the surface of the golf ball are there because they reduce the drag force on the ball (Figure 1).
How exactly does this work? In order to understand, we'll need to take a closer look at the pattern of airflow around a ball as it flies through the air. Figure 2 compares the airflow pattern for a smooth ball (top) vs. a dimpled ball (bottom), in horizontal flight (or in a wind tunnel). In the case of a ball with a smooth surface, the airflow in the thin layer right next to the ball (called the boundary layer) is very smooth. This type of flow is called laminar. For a ball with a smooth surface, the boundary layer separates from the ball's surface quite early, creating a wide, turbulent wake pattern behind the ball. The turbulent wake exerts a drag force on the ball. When dimples are added to the surface of the ball, they create turbulence within the boundary layer itself. The turbulent boundary layer has more energy than the laminar boundary layer, so it separates from the surface of the ball much later than the laminar boundary layer flowing over the smooth ball (Figure 2, bottom). Since flow separation occurs later, the turbulent wake behind the ball is narrower, resulting in less drag force.
In the real world, the situation is more complex than shown in Figure 2. First of all, golf balls don't fly horizontally through the air. When the club hits the ball, it launches it at an angle, determined by the golfer's swing and the loft angle of the club. The ball's initial speed and angle will be determined by the speed and orientation of the club face at the moment it strikes the ball, and exactly where on the surface of the ball that contact is made. To make things even more complicated, the club generally imparts a spin to the ball. How does spin affect the flight of the ball? Let's consider the simplest case first. If the club strikes the ball squarely, the spin that is induced is called backspin (because the ball is spinning backwards, from the golfer's viewpoint). To be more precise, backspin is a spin around the horizontal axis, in a clockwise direction if viewed from the left-hand side (as in Figure 2, above). Let's consider the effect that backspin will have on airflow over the ball. Since the surface of the ball is now moving in a clockwise direction, the airflow over the top of the ball will be sped up, and the airflow over the bottom of the ball will be slowed down. This has the effect of decreasing the pressure above the ball, and increasing the pressure below the ball. In other words, a spinning ball acts like an airplane wing and creates lift. Figure 3 shows how backspin affects the airflow over a golf ball in a wind tunnel. The smoke lines in Figure 3 show the airflow pattern. Notice how the flow pattern behind the ball is warped downward. This is the same type of pattern you would see for an airfoil at an angle to the wind tunnel air flow (like an airplane wing at takeoff when the plane starts climbing). The spin rate used in Figure 3 was less than the average spin for a golf ball hit by a club. The lift effect with real-world spin rates would be even greater.
What if you don't hit the ball squarely? For example, say the club face is angled outward (away from the golfer's body) as it strikes the ball. Then the induced spin will have a component about the vertical axis. In this case, the spin would be clockwise, as viewed from above. The spin would result in an aerodynamic force pushing the ball off to the right, away from a straight flight path. In addition, the initial launch angle would be off to the right instead of straight ahead. These two combine to create what golfers call a slice. Instead of sailing straight down the fairway, the ball curves off to the right, perhaps into the rough, or trees, or (in the worst case) off to an adjacent fairway. If the club face is angled inward (toward the golfer's body) as it strikes the ball, then the ball tails off in the opposite direction. Golfers call this a hook. The Polara golf ball has an asymmetric pattern of dimples. There are six rows of deeper dimples on either side of the equator. At each pole, the dimples are shallower. This creates an airflow that tends to correct sidespin, and reorient the ball toward straighter flight. Does it have a significant effect on where the ball ends up? That's what this project is designed to find out. Terms, Concepts, and Questions to Start Background Research To do this project, you should do research that enables you to understand the following terms and concepts:
Questions
Bibliography
Materials and Equipment To do this experiment you will need the following materials and equipment:
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Variations
Credits Andrew Olson, Ph.D., Science Buddies
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