Method 2: Basic Kinematics
We know from kinematics that if y is the vertical position of the object above the ground, and it moves under constant vertical acceleration, then the most general formula for y vs. time is:
[tex]y = y_0 + v_0t + \frac{1}{2}at^2[/tex]
where:
- y0 is the initial vertical position (the position at t = 0)
- v0 is the initial vertical speed (the speed at t = 0)
- a is the vertical acceleration
- t is elapsed time
You just have to accept this for now -- I'm not going to get into a derivation. We also know that for constant acceleration, the expression for the vertical speed v vs. time is:
[tex]v = v_0 + at[/tex]
This just comes from the definition of acceleration -- it is the rate at which speed changes with time. So if you multiply acceleration by time, you get the change in speed. Now, in our case, we know that the acceleration is due to gravity: a = -g, with g = +9.81 m/s2. We also know that v0 = 0 since the object is dropped from rest. We also know that the initial position y0 is just the height h from which the object is dropped. With that in mind, we get for the first equation:
[tex]y = h - \frac{1}{2}gt^2[/tex]
and for the second equation
[tex]v = - gt[/tex]
Using the second equation, solve for t:
[tex]t = -\frac{v}{g}[/tex]
Plug that result for t into the first equation:
[tex]y = h - \frac{1}{2}g\left(-\frac{v}{g}\right)^2[/tex]
Now, we want to know what the speed is when the object reaches the ground, so set the vertical position y = 0 and solve:
[tex]h = \frac{1}{2}g\frac{v^2}{g^2}[/tex]
[tex]2h = \frac{v^2}{g}[/tex]
[tex]2gh = v^2[/tex]
This is exactly the same equation as we derived before using the conservation of energy. You could also have derived it using the work-energy theorem, but that's really not much different from the conservation of energy method.