# Summer Physics as Taught by Albert

Energy is such a natural part of life that its contribution to the fabric of our lives can often go unnoticed. Sometimes, however, its impact cannot be ignored. Nowhere is this more true than in the ultimate sports act, hitting a home run.

The batter above is Albert Pujols, first baseman for the Saint Louis Cardinals. You see him in the act of hitting one out of the park. Imagine you were in his shoes a moment earlier, your muscles tensed with anticipation, holding a 42 inch wooden bat while you wait for the precise instant to swing at a 3 inch, 5 ounce cowhide-wrapped ball hurtling toward you at over 90 miles per hour.

At this speed, it will take about four-tenths of a second for the ball to travel the 60 feet, 6 inches from the pitcher’s mound to home plate.

In that brief interval, if you decide to swing the bat, and have the good fortune to hit the ball, you will be carrying out a physics experiment on the transformation of energy. As you can imagine, there is a lot of energy invested in a baseball travelling 90 miles per hour. This energy of motion is called kinetic energy by scientists, and it’s easy to appreciate its raw power. Not so evident is the latent power in the muscles of the batter awaiting the pitch. Like coiled springs, their energy is ready to be put into action. This stored energy is called potential energy by scientists, energy ready to be put to work swinging the bat. The more potential energy the batter’s muscles release, the faster the speed of the bat through the swing.

Obviously there is a lot of energy at play here. The batter has converted a considerable amount of potential energy from his arm and shoulder muscles to the kinetic energy of the swinging bat. Similarly, the pitcher has converted potential energy from his throwing arm to the kinetic energy of the speeding baseball. What happens in the instant when the ball hits the bat is the difference between a home run and a fly ball, and a lot of scientists’ time has been devoted to understanding that brief 1/1,000th of a second, the measured duration of the collision of a pitched baseball on a swinging bat.

The Sports Biomechanics Laboratory at the Davis campus of the University of California has for decades carried out detailed examinations of the scientific principles governing baseball. Many of the researchers in the Lab are graduate and undergraduate students in biomedical engineering. The student researchers have learned a lot about what it takes to hit a home run. The on-the-field mechanics of baseball  how pitchers throw, how batters swing  are examined through equations that attempt to simulate what happens when bat meets ball. When a simulation seems to take the laws of physics into account properly, it is then checked by direct measurements to see how well the simulation predicts what actually happens.

First lets look at how the ball is thrown. Three variables turn out to be of particular importance:

Ball velocity. Not surprisingly, balls that are pitched faster travel off the bat further. Much of the kinetic energy of the ball is returned to it by the bat, as kinetic energy of motion in the opposite direction.

Spin. However, even more important is the spin of the pitched ball. Conventional wisdom says a hitter can drive a fastball farther than a curveball  the fastball travels some 42 meters per second, the curve ball only 35 meters per second, so the fastball has much more kinetic energy to contribute to the ball’s flight, they say. Not so, it turns out. A curveball is thrown with topspin, so the top of the ball rotates in the direction of the pitch. Being hit by the bat throws the ball into reverse, giving it backspin and thus lift to carry it further. A fastball is thrown with backspin; it spins the other way when hit, and so has less lift and sinks sooner.

Ball elasticity. When the ball is deformed by its collision with the bat, it tends to bounce back. The more elastic the ball, the more of its kinetic energy is returned by the bat. The cork core of a baseball is wound tightly with yarn to make it bouncy. If the yarn is wound tighter, a more “lively” ball results, one that travels further off the bat.

Now consider how the ball is hit. Again, three variables have been found to be of prime importance:

Bat speed. More than any other variable, the speed with which the hitter swings the bat determines how far the hit ball will travel. As a general rule, increasing the bat velocity of an average home run swing (30 meters per second) by one meter per second increases the distance of the hit five meters.

Bat position on ball. For optimal range, the bat should not contact the ball squarely, but rather 2.65 cm below center. This undercut imparts backspin, creating lift that causes the ball to travel further.

Ball position on bat. The impact of the ball causes the 42 inch wooden bat to vibrate, like plucking a tightly drawn string. This is important, because every vibration of the bat draws energy away from the ball, reducing its speed as it leaves the bat. Each bat vibrates at several low and high frequencies at once, like the harmonics of a violin string. Striking the bat at “nodes” where a frequency produces no vibrations avoids this loss of energy. The optimal position is about 6 inches from the tip. Interestingly, the shape of the shaft and handle makes no difference whatever  by the time the vibration reaches there, the ball has already left the bat.

Because of the enormous kinetic energy invested in the baseball when a big league pitcher throws a 90 mph fast ball, to hit a home run Albert Pujols must act very fast, and very precisely. He has less than a quarter second to see the pitch, judge its speed and location, decide what to do, and then start to swing. The bat must meet the ball within an eighth of an inch of dead center to avoid a foul ball, at precisely the right millisecond to generate the correct arc to send it out of the park. A home run by Albert is all about precision in the application of energy. See? Summer school physics doesn’t have to be boring…