The simplest model that makes any sense at all for the golf swing is a double pendulum. The two members of the pendulum are:
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This
is a very simple model, having only two moving elements hinged
together. To see just how simple, let's re-draw it the way an engineer
would: as a collection of free, hinged bodies. Now we can see why the
model is a double pendulum; it is a black pendulum (the club) hanging
from the end of a green pendulum (representing the triangle). While the
diagram looks different from the golfer above, it works exactly the
same when it comes to physics.Given the simplicity of the model, it's pretty amazing how close it can get to the actual measured performance of a golfer's swing. True, there are a lot of nuances of the swing that it doesn't capture. But experience has shown it is rich enough to explain where the clubhead speed comes from in a good swing. |
![]() Let's look at the next question about using the model. We have two hinges, and we can apply a torque at each of those hinges. Those two torques -- plus gravity -- are the only forces in this model that will cause the golfer to swing the club. So the engineering model has to say what kind of torque:
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![]() The answer is centrifugal force.[1] Remember that a body in motion wants to keep moving in a straight line. But the golfer is pulling the club around in a circle. According to Newton, the club wants to fly outward from the circle; the force that is trying to pull it out straight with the arms is centrifugal force. That centrifugal force is generated by pulling the club in a circle around the shoulder hinge, and the force wants to pull the club straight out along a radius from that hinge. How big is that centrifugal force? Let's look again at the formula: m v2The mass m is a property of the golf club, and the radius r is a combination of the extended arms and the wrist-cock angle. The more acute the wrist-cock angle, the closer the club is to the shoulder hinge -- and thus the smaller the radius. As for velocity v, it increases as the body torque accelerates the triangle. So, what does the golfer have to do to get maximum centrifugal force in order to get maximum clubhead speed? His job is to "hold the lag" -- keep the club cocked at a right angle to the arms -- until fairly late in the downswing. This keeps from releasing the club until v is nearly as large as it's going to get, which allows a large F to accelerate the club outward and downward just before impact. This, and not torque applied by the hands, is the way to reliable high clubhead speed. (It is worth noting there is criticism of centrifugal force as the mechanism of the golf swing. More on that here.) |
"But his theory seems to explain a shot I hit at the par-3 fifteenth in the second round at Firestone. The choice of club lay between a two-iron and a three-iron, and I decided to go with an easy two-iron. Coming into the ball I was deliberately 'soft' with my hands. I've never hit a better two-iron in my life! The ball finished over the green."Maybe this explains what happens on those good drives where I have a 'soft' feeling in my hands through the ball... My hands merely went along for the ride."
But the important change he did not have to make was to add any wrist torque to release the club at the bottom of the swing. That is accomplished completely by centrifugal force. In fact, once he had a mathematical model that behaved like the golf swing, he ran some "what if" analyses to see whether application of wrist torque could add to power. He found that there is a critical time about 70-100 milliseconds before impact (where the arms are 60º before the impact position) where torque changes from hurting clubhead speed to helping it. That is, any uncocking wrist torque before the critical time will reduce clubhead speed at impact. You can indeed increase clubhead speed a bit by applying wrist torque, but only if you can do it for just the last 70 milliseconds before impact, and not before. It takes a very well-coordinated athlete to get away with this. (If you are interested in more detail about this, I have worked it to death in another article. In particular, the difficulty of applying torque during those last 70 milliseconds is discussed here.) Interestingly, Jorgensen found that that the same critical time works the other way as well. If you use negative torque (that is, use strength in the wrist to prevent uncocking) early in the swing and then release it 100 milliseconds before impact, you will increase the clubhead speed. In fact, you'll get as much increase in clubhead speed as that well-coordinated athlete would have gotten by a late application of positive torque. And it's much easier to hold off release than to apply a release-aiding torque at exactly the right time. So Jorgensen's study confirms the notion that power in a golf swing -- clubhead speed -- is a product of centrifugal force and not wrist torque. He adds a lot of detail, but nothing that denies that basic truth. |
My
Eureka was because, watching it, I saw an upside-down golf swing. The
principle of a double pendulum driven by centrifugal force was right
there, and history has proven it very effective. For a description of
how a trebuchet works, see the page and the animation I clipped from The Trebuchet Store.
(They sell trebuchet kits and the like, in case you find this stuff
interesting for its own sake, not just what it teaches about the golf
swing.) In short, the inner arm of the pendulum (corresponding to the
triangle) is a rigid, pivoting structure, but the outer arm
(corresponding to the golf club) is literally a string. You couldn't
apply "wrist torque" to it if you wanted to -- it must operate by centrifugal force.
Last modified May 7, 2020