Among all constant acceleration motions that occur in the nature, there are two of particular interest: **free fall** and **vertical launch**. In this section, we will study **free-falling objects**. Both, free fall and vertical launch, are governed by the equations of the uniformly accelerated rectilinear motion (u.a.r.m.) or constant acceleration motion:

## Free fall

In **free fall**, an object falls vertically from a certain *height H* disregarding any kind of friction with the air or any other obstacle. It is a uniformly accelerated rectilinear motion or constant acceleration motion in which *the acceleration is gravity*. On the Earth surface, the acceleration of the gravity can be considered constant, and directed downwards. It is designated by the letter *g* and its value is 9.8 m/s^{2} (sometimes it is approximated to 10 m/s^{2}).

To study **free fall** motion, normally, we will use a system of reference whose origin of coordinates is at the bottom of the y-axis and *we will consider the upward direction as positive*, as can be seen in the figure:

System of Reference in Free Fall

When solving this type of problems, it is customary to use the system of reference in the figure. The body is always on the positive y-axis and its initial position is y_{0}=H, its velocity is 0 m/s (since the body is at rest) and its acceleration is constant and equal to the gravity, but with negative sign because the direction of motion is opposite to that of the y-axis. Keep in mind that the velocity values obtained will also be negative.

So, we get:

**Free fall** is a constant acceleration motion or uniformly accelerated rectilinear motion (u.a.r.m.) in which a body is dropped vertically from a certain height and *does not encounter any obstacle in its way*. The **free fall equations** are:

Where:

*y*: Finalof the body. Its unit in the International System (SI) is the meter (m)*position**v*: Finalof the body. Its unit in the International System (SI) is the meter per second (m/s)*velocity**a*: Theof the body while in motion. Its unit in the International System (SI) is the meter per second squared(m/s**acceleration**^{2})*t*:spent on the motion. Its unit in the International System (SI) is the second (s)**Time***H*:from which the body falls. It is a measurement of**Height***length*and therefore is measured in meters*g*: Value of thewhich**gravitational acceleration***on Earth surface*can be considered equal to 9.8 m/s^{2}

If you understand the formulas that we have seen so far, you may be wondering *Where is mass in these formulas?*. Common sense tells us that a heavy object, such as a hammer, should fall faster than a light object, for example a feather. However, common sense *is wrong* on this occasion. The fact is that if both, the hammer and feather, were in a vacuum, they would fall at the same velocity. If they are not in a vacuum then the air will resist the fall these bodies, its effect more evident on the lighter feather, which will take longer to get to the ground.

If you are not convinced of what we just inferred, watch the following video in which the astronaut David Scott, Commander of the Apollo 15 mission, drops a hammer and a feather on the Moon surface, where there is no air to resist the fall of the objects: