Displacement and velocity
A particle moves along a straight line. Its displacement s is its position measured from a fixed origin on the line, positive on one side and negative on the other, as a function of the time t.
Its velocity is the rate of change of displacement, : the gradient of the graph of s against t. If meters after t seconds, then v = 2t meters per second. At t = 3 the particle is at s = 9 m and moving at 6 meters per second, and the tangent to the graph there has gradient 6.
Acceleration, and being at rest
Acceleration is the rate of change of velocity, , the second derivative of s. For v = 2t it is a = 2 meters per second per second: the velocity grows by 2 meters per second every second.
A particle is momentarily at rest when v = 0. That says nothing about a. A ball thrown up with has v = 20 − 10t and a = −10. At t = 2, v = 0 and the ball is at its highest point, 40 − 20 = 20 meters up; its acceleration is still −10, which is why it does not stay there.
v = 20 − 10t > 0: the ball is rising, and a = −10 is pulling its speed down
Set t to where the velocity crosses zero
The ball on one clock: its height, its velocity 20 − 10t and its acceleration −10. Drag the time to t = 2: the velocity graph crosses 0 at the top of the flight, and the acceleration is −10 throughout.
Velocity has a sign; speed does not
Velocity carries a sign for direction. Positive v means s is increasing, so the particle moves in the positive direction; negative v means it moves the other way. The ball has v = 10 at t = 1, rising at 10 meters per second, and v = −10 at t = 3, falling at 10 meters per second.
Speed is the size of the velocity, speed = |v|, and is never negative. At t = 1 and t = 3 the ball has the same speed, 10 meters per second, and opposite velocities.
A particle that turns back
A particle starts at the origin, and after t seconds its displacement is meters, for . Then meters per second, and meters per second per second.
At t = 0 the particle is moving at 9 meters per second, with a = −12. It is at rest when 3(t − 1)(t − 3) = 0, at t = 1 and at t = 3. At t = 1 it is at s = 1 − 6 + 9 = 4 m, and at t = 3 at s = 27 − 54 + 27 = 0 m, back at the origin.
Between those times the velocity has one sign on each interval. For , v is positive (3.75 at t = 0.5): the particle moves forward. For 1 < t < 3, v is negative (−3 at t = 2): it moves back. For t > 3, v is positive again (3.75 at t = 3.5): forward once more.
The gold curve . Its gradient, the velocity, is 0 at (1, 4) and at (3, 0), where the particle turns; between them the graph falls and the particle moves back toward the origin.
Speeding up and slowing down
A particle speeds up when its velocity and acceleration have the same sign, and slows down when they have opposite signs. Negative acceleration alone does not mean slowing down: it pushes in the negative direction, which slows a particle moving forward and speeds up one moving back.
Here a = 6t − 12 is negative for t < 2 and positive for t > 2. So for 0 < t < 1, v is positive and a negative: slowing down, from 9 meters per second to rest. For 1 < t < 2, both are negative: speeding up, backwards. For 2 < t < 3, v is negative and a positive: slowing down, to rest at the origin. For t > 3, both are positive: speeding up.
At t = 2, a = 0 and v = 12 − 24 + 9 = −3. The backward speed stops growing there, so 3 meters per second is the fastest the particle moves backwards.
The gold curve is the velocity , below the axis between t = 1 and t = 3, lowest at (2, −3). The dashed curve is the speed |v|, folded above the axis.
Distance and displacement
Over the first 4 seconds the displacement is s(4) − s(0) = (64 − 96 + 36) − 0 = 4 m: the particle ends 4 m from where it began.
The distance traveled is more, because the particle turned back twice. Split the time where v changes sign. From t = 0 to t = 1 it goes from 0 to 4, which is 4 m. From t = 1 to t = 3 it goes from 4 back to 0, another 4 m. From t = 3 to t = 4 it goes from 0 to 4, another 4 m. The distance is 4 + 4 + 4 = 12 m.
The ball is the same. From t = 0 to t = 4 it rises 20 m and falls 20 m, a distance of 40 m, while its displacement is 80 − 80 = 0.
The usual mistakes
Differentiating as 3t, or as . The power comes down and drops by one: v = 6t.
Giving v as the acceleration. For v = 4t the acceleration is the gradient of that line, 4.
Reading v = 0 as a = 0. The ball at its top has v = 0 and a = −10.
Taking negative acceleration to mean slowing down. Between t = 1 and t = 2 the particle has a < 0 and is speeding up, because it is moving backwards.
Giving the displacement as the distance traveled when the particle turns back: 4 m against 12 m over the first 4 seconds.
Two average-speed cameras
In the application below, a van's distance past a camera is a function of time. Its derivative is the van's speed at each instant, and setting that derivative equal to the average speed between two cameras finds the moment the van was traveling at exactly the average.
Worked example: Two Average-Speed Cameras on a Motorway: the Instant a Van Was Doing Exactly the Average
Question Two cameras stand 12 km apart on a motorway. A van passes the first and reaches the second 8 minutes later. Its distance past the first camera is s = m + 0.0625m2 km, where m is the number of minutes since it passed. (a) Find the van's average speed between the cameras, in kilometers per hour. (b) The mean value theorem says that at some instant between the cameras the van was traveling at exactly that speed. Find that instant.
1.Check the two ends. At m = 0 the van is at the first camera, s = 0; at m = 8, s = 8 + 0.0625 × 64 = 8 + 4 = 12 km, the second camera.
The van is at the first camera when m = 0 and at the second when m = 8, where s = 8 + 4 = 12 km. 2.(a) The average speed is the distance divided by the time: 128 = 1.5 km a minute. In an hour that is 1.5 × 60 = 90, so the average speed is 90 km/h.
(a) The chord joining the two cameras has gradient 128 = 1.5 km a minute, which is 90 km/h. 3.The distance is a smooth function of the time, so the mean value theorem applies: somewhere strictly between the cameras the derivative equals the gradient of the chord, and that gradient is the average of 1.5 km a minute.
The distance is smooth, so the mean value theorem promises an instant where the tangent is parallel to that chord. 4.Differentiate for the speed at any instant: dsdm = 1 + 0.125m km a minute.
The speed at any instant is dsdm = 1 + 0.125m km a minute. 5.Set that equal to the average: 1 + 0.125m = 1.5, so 0.125m = 0.5 and m = 4.
Setting that equal to the average, 1 + 0.125m = 1.5, gives m = 4, and the tangent there is drawn parallel to the chord. 6.(b) Four minutes after the first camera the van was traveling at exactly 1.5 km a minute, which is 90 km/h. Check: it passed the first camera at 1 km a minute (60 km/h) and the second at 2 km a minute (120 km/h), so it went through 1.5 on the way.
(b) After 4 minutes the van was traveling at exactly 90 km/h: 60 km/h at the first camera, 120 at the second.
Answer: (a) 90 km/h, which is 1.5 km a minute; (b) 4 minutes after the first camera
Common mistakes
- Dividing 12 by 8 and calling the answer 1.5 km/h. The time is in minutes, so 1.5 is kilometers a minute; it must be multiplied by 60 to give the 90 km/h the two cameras report.
- Reading the theorem as saying the van held that speed all the way. It names one instant only: this van was traveling at 60 km/h as it passed the first camera and 120 km/h at the second, and matched 90 km/h exactly once, after 4 minutes.