Another way to investigate atmosphere’s effect on airborne objects is their maximum falling velocities. On average, gravity’s force accelerates falling objects at 32 ft/sec2. Folklore contends that if someone drops a penny off New York City’s Empire State Building, when it reaches the sidewalk, it can slice through a pedestrian. This is a gruesome untrue story. The air molecules of New York City's atmosphere will decelerate the maximum falling velocity of a penny far below the velocity required to penetrate pedestrians.
Suppose someone drops a baseball from 10,000 feet high. What is baseball’s final velocity when it contacts the player's glove? The Integrated Final Velocity Formula provides the answer before we factor in atmosphere's effect.
a. Integrated Final Velocity FormulaAt 172.45 miles per hour, nobody could catch these baseballs without risking serious injury. However, baseballs falling in earth’s atmosphere never achieve 172.45 mph. Air molecules decelerate falling baseballs in the same way that they decelerate pitched baseballs. What is baseball’s maximum falling velocity? The drag formula provides the answer.
d. Drag FormulaSubstitute falling object weight (Wt) for drag (DG). Substitute maximum falling velocity (MFV) for relative velocity (RV). Rearrange the substituted formula’s terms to have maximum falling velocity by itself.
1. Drag formula DG = (AD)(SF)(CSA)(RV 2)Baseballs weigh 5.25 ounces or 0.328 pounds. Spheres cross-sectional areas equal the sphere’s circumference squares divided by 3.1416. Baseball’s circumference is 9.25 inches. Baseball’s entire cross-sectional area is 27.24 square inches ((9.25)2 / 3.1416). However, only one-half of falling spheres collide with air molecules. Therefore, divide baseball’s total cross-sectional area by 2 (13.62 square inches). Air density (AD) equals 0.00001. Surface friction (SF) equals 0.7.
1. Wt = 0.328 lbs.Baseball’s maximum falling velocity is 40 miles per hour. All fielders should easily catch 40 mph baseballs dropped from any height from which they can see them. If, with the 32 ft/sec 2 force of gravity continuously accelerating falling baseballs through the air molecules of atmosphere, the maximum velocity baseballs achieve is forty miles per hour, then what influence do air molecules have on pitched baseballs with release velocities of 90 miles per hour and no force continuously accelerating them? In Chapter 2, I demonstrated that my fastball decelerated almost 13 miles per hour from release to the catcher's glove. Air molecules caused that deceleration.