# Physics of Baseball

Topics: Baseball, Baseball rules, Fastball Pages: 9 (3813 words) Published: November 29, 2000
"Baseball's a simple game. You hit the ball. You throw the ball. You catch the ball," said a well-respected baseball manager by the name of Casey Stengel. Mr. Stengel was a baseball man, not a mathematician nor a physicist. Physics and mathematics can be applied to the game of baseball on every pitch, and on every swing of the bat.

To understand the physics of the game, it is first necessary to look at the center of the game, the ball. Section 1.09 of the Official Baseball Rules states that the ball must weigh between 5 ounces and 5 ¼ ounces, and that the circumference of the ball must be between 9 inches and 9 ¼- inches (www.majorleaguebaseball.com/library/rules.sml).

The velocity of the ball plays a large part in its motion. When the ball is traveling at a speed of about 50 miles per hour or less (small velocity), it is said that the air runs "smooth" over the ball, which does not create much movement. For velocities of about 200-mph or more, the air surrounding the ball, and the air trailing the ball, is said to be quite "turbulent" (Adair 6). However, for the most part, the game is played with velocities between these two areas, which creates a gray area where characteristics of both can be observed. When a ball is hurled towards home plate by a pitcher, it can be forced to move in different directions if there is an altered surface on the ball traveling at a small velocity. This can be achieved by illegally placing a foreign material, such as spit or Vaseline, onto the ball. Movement can also be achieved when a ball is changed through use during the game  to prevent such movement, balls are changed constantly throughout the game. The air resistance is, surprisingly, smaller for turbulent air than for smooth air. Despite popular belief the biggest opponent that a hitter faces is not the pitcher it is air resistance. If a ball were hit with a velocity of 110-mph at an angle of 35, it is expected to travel about 700 feet, if it were hit in a vacuum. However, baseball is not played in a vacuum, and a ball with those characteristics would only travel about 400 feet. The force that is placed on the ball depends on the velocity of the ball and the drag coefficient, which varies slowly with the velocity (Adair 6). In the graph below, the drag coefficient for a baseball hit at 110-mph is about 0.2. Because the mass of the ball is constant, and the air density does not vary much for the conditions where baseball is played, the force on the ball is proportional to the velocity squared times the drag coefficient. The rotation of the ball has a small effect on the forces against the ball. If a ball is traveling with a high rotation rate, the drag will increase about one percent of the drag, which does not make a significant difference in the velocity of the ball as it crosses home plate. (http://farside.ph.utexas.edu/teaching/329/lectures/node79.html)

In most major league ballparks, the density of the air is relatively equal. However, in the hitter friendly confines of Coors Field in Denver, Colorado, home of the Colorado Rockies, the air density does play a major role in the distance the ball travels. A ball hit in Shea Stadium in New York by Mets power-hitter Mike Piazza that lands 400 feet from home plate could travel up to 40 feet further in Coors Field. This has caused a lot more homeruns to be hit in Colorado, which excites the fans and hitters, but is hated by the pitchers (Adair 18). Several tests have been performed in order to help further understand the drag on the ball. When a ball is placed in a wind tunnel with an upward wind velocity of 95-mph, the ball appears nearly motionless. This has lead researchers to conclude that for a ball traveling at 95-mph, the drag on the ball is equal to its weight. This is why throwing the ball at a higher initial velocity is beneficial to the pitcher. Not only does the ball reach the plate in a faster time, but also the drag on the...