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x = x 0 + v 0 t + 1 2 a t 2 ( constant a ) .

Calculating displacement of an accelerating object

Dragsters can achieve an average acceleration of 26.0 m/s 2 . Suppose a dragster accelerates from rest at this rate for 5.56 s [link] . How far does it travel in this time?

Picture shows a race car with smoke coming off of its back tires.
U.S. Army Top Fuel pilot Tony “The Sarge” Schumacher begins a race with a controlled burnout. (credit: Lt. Col. William Thurmond. Photo Courtesy of U.S. Army.)

Strategy

First, let’s draw a sketch [link] . We are asked to find displacement, which is x if we take x 0 to be zero. (Think about x 0 as the starting line of a race. It can be anywhere, but we call it zero and measure all other positions relative to it.) We can use the equation x = x 0 + v 0 t + 1 2 a t 2 when we identify v 0 , a , and t from the statement of the problem.

Figure shows race car with acceleration of 26 meters per second squared.
Sketch of an accelerating dragster.

Solution

First, we need to identify the knowns. Starting from rest means that v 0 = 0 , a is given as 26.0 m/s 2 and t is given as 5.56 s.

Second, we substitute the known values into the equation to solve for the unknown:

x = x 0 + v 0 t + 1 2 a t 2 .

Since the initial position and velocity are both zero, this equation simplifies to

x = 1 2 a t 2 .

Substituting the identified values of a and t gives

x = 1 2 ( 26.0 m/s 2 ) ( 5.56 s ) 2 = 402 m .

Significance

If we convert 402 m to miles, we find that the distance covered is very close to one-quarter of a mile, the standard distance for drag racing. So, our answer is reasonable. This is an impressive displacement to cover in only 5.56 s, but top-notch dragsters can do a quarter mile in even less time than this. If the dragster were given an initial velocity, this would add another term to the distance equation. If the same acceleration and time are used in the equation, the distance covered would be much greater.

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What else can we learn by examining the equation x = x 0 + v 0 t + 1 2 a t 2 ? We can see the following relationships:

  • Displacement depends on the square of the elapsed time when acceleration is not zero. In [link] , the dragster covers only one-fourth of the total distance in the first half of the elapsed time.
  • If acceleration is zero, then initial velocity equals average velocity ( v 0 = v ) , and x = x 0 + v 0 t + 1 2 a t 2 becomes x = x 0 + v 0 t .

Solving for final velocity from distance and acceleration

A fourth useful equation can be obtained from another algebraic manipulation of previous equations. If we solve v = v 0 + a t for t , we get

t = v v 0 a .

Substituting this and v = v 0 + v 2 into x = x 0 + v t , we get

v 2 = v 0 2 + 2 a ( x x 0 ) ( constant a ) .

Calculating final velocity

Calculate the final velocity of the dragster in [link] without using information about time.

Strategy

The equation v 2 = v 0 2 + 2 a ( x x 0 ) is ideally suited to this task because it relates velocities, acceleration, and displacement, and no time information is required.

Solution

First, we identify the known values. We know that v 0 = 0, since the dragster starts from rest. We also know that x x 0 = 402 m (this was the answer in [link] ). The average acceleration was given by a = 26.0 m/s 2 .

Second, we substitute the knowns into the equation v 2 = v 0 2 + 2 a ( x x 0 ) and solve for v :

v 2 = 0 + 2 ( 26.0 m/s 2 ) ( 402 m ) .

Thus,

v 2 = 2.09 × 10 4 m 2 /s 2 v = 2.09 × 10 4 m 2 /s 2 = 145 m/s .

Significance

A velocity of 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.

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Practice Key Terms 1

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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