Solving for Final Velocity II
Solving for Final Velocity When Velocity is not Constant (a ≠ 0)
A fourth useful equation can be obtained from another algebraic manipulation of previous equations.
If we solve \(v = v_0 + at\) for \(t,\) we get
\(t = \cfrac{v - v_0}{a}.\)
Substituting this and \(\bar{v} = \frac{v_0 + v}{2}\) into \(x = x_0 + \bar{v} t,\) we get
\(v^2 = v_0^2 + 2a(x \; - \; x_0) \;\; (\text{constant }a).\)
Example on Calculating Final Velocity: Dragsters
Calculate the final velocity of the dragster in the example from the previous lesson without using information about time. Recall that dragsters can achieve average accelerations of 26.0 m/s2. Also, recall that \(x = 402\text{ m}.\)
Strategy
Draw a sketch.
The equation \(v^2 = v_0^2 + 2a(x \; - \; x_0)\) is ideally suited to this task because it relates velocities, acceleration, and displacement, and no time information is required.
Solution
1. Identify the known values. We know that \(v_0 = 0,\) since the dragster starts from rest. Then we note that \(x \; - \; x_0 = 402\text{ m}\) (this was the answer in the example). Finally, the average acceleration was given to be \(a = 26.0\mathrm{\; m/s^2}.\)
2. Plug the knowns into the equation \(v^2 = v_0^2 + 2a(x \; - \; x_0)\) and solve for \(v.\)
\(v^2 = 0 + 2 \left ( 26.0\mathrm{\; m/s^2} \right ) (402\text{ m}).\)
Thus
\(v^2 = 2.09 \times 10^4\mathrm{\; m^2/s^2}.\)
To get \(v,\) we take the square root:
\(v = \sqrt{2.09 \times 10^4\mathrm{\; m^2/s^2}} = 145\text{ m/s}.\)
Discussion
145 m/s is about 522 km/h or about 324 mi/h, but even this breakneck speed is short of the record for the quarter mile. Also, note that a square root has two values; we took the positive value to indicate a velocity in the same direction as the acceleration.
An examination of the equation \(v^2 = v_0^2 + 2a(x \; - \; x_0)\) can produce further insights into the general relationships among physical quantities:
- The final velocity depends on how large the acceleration is and the distance over which it acts
- For a fixed deceleration, a car that is going twice as fast doesn’t simply stop in twice the distance—it takes much further to stop. (This is why we have reduced speed zones near schools.)
This lesson is part of:
One-Dimensional Kinematics