Air resistance results in a small correction to the result in Eq. (1), as does a headwind or tailwind. The main force on the body is that due to gravity. In addition, the air results in a drag force F=0.5CdAv2 , where A is the cross-sectional area of the body, ρ =1.21 kg m^(-3) is the density of air at 20 °C, v is the speed of the body relative to the air, and Cd is the drag coefficient. The cross-sectional area depends on the orientation of the body, and C_d can be taken to be about 0.7, given that C_d=0.5 for a sphere and C_d=1 for a flat surface. For example, if A=0.1 m2 and v=20 m/s, then F=16.9 N, compared with a gravitational force of 686 N on a 70 kg person. The drag force is negligible in the vertical direction for speeds up to about 30 m/s, but it can reduce the horizontal speed of a 70 kg person from say 5.0 m/s to about 4.7 m/s during a fall time of 3.0 s depending on the orientation and the horizontal component of the drag force. In the vertical orientation, with A=0.1 m^2 and m=70 kg, the terminal velocity would be 127 m/s. However, if A were increased to 0.5 m^2 by falling in a horizontal position, the terminal velocity would decrease to 57 m/s. The relevant equations of motion, including the drag force, are easy to solve numerically.