One Motion, Two Different Totals
When an object moves, two natural questions are how far its position changed overall and how much ground it covered along the way. These questions have different answers whenever the object changes direction.
Choose a positive direction along a straight line. Motion in that direction has positive velocity; motion in the opposite direction has negative velocity. A negative velocity contributes a negative change in position, but the distance traveled during that motion is still positive.
For example, if an object moves \(8\) metres forward and then \(3\) metres backward, its position changes by \(8-3=5\) metres in the positive direction. Its total distance traveled is \(8+3=11\) metres. The first quantity preserves direction; the second counts all motion without assigning it a sign.
Interval Changes from Velocity
Suppose a motion is described on consecutive time intervals. Let \(\Delta t_i\) be the duration of interval \(i\), and let \(v_i\) be the velocity on that interval. Durations are positive. If velocity is constant on an interval, its change in position is its velocity multiplied by the interval’s duration.
The sign of \(\Delta x_i\) records direction. A positive value means position increased; a negative value means position decreased. The magnitude \(|\Delta x_i|\) records the length of that interval’s change in position.
The same displacement formula is exact if \(v_i\) is the average velocity over the entire interval. Average velocity is defined as the interval’s displacement divided by its duration, so multiplying that average by the duration recovers the displacement. However, average velocity alone does not in general determine the distance traveled within the interval. We will distinguish these cases carefully.
In formulas, if the interval displacements are \(\Delta x_1,\Delta x_2,\ldots,\Delta x_n\), then
and, when each interval’s displacement magnitude equals the distance traveled on that interval,
These formulas serve different purposes. Adding signed changes allows forward and backward motion to cancel in the net displacement. Adding magnitudes does not allow cancellation, so it measures the accumulated path length under the stated condition.
Worked Example: Constant Velocities in Both Directions
Worked Example: Constant Velocities in Both Directions
An object moves along a straight track. Its velocity is \(4\ \text{m/s}\) for \(2\ \text{s}\), then \(-2\ \text{m/s}\) for \(1\ \text{s}\), then \(1\ \text{m/s}\) for \(3\ \text{s}\). Find its net displacement and total distance.
The velocity is constant on each interval, so each interval’s displacement is velocity multiplied by duration.
First interval:
Second interval:
Third interval:
The net displacement adds the signed changes:
The distance adds their magnitudes. Because velocity is constant on each interval, there is no direction reversal within an interval:
Check: The object ends \(9\ \text{m}\) in the positive direction from where it started. It traveled \(8+2+3=13\ \text{m}\) along the way. The distance exceeds the magnitude of the displacement, as expected when the object reverses direction.
Why Distance Cannot Be Less Than Net Displacement
For any list of interval displacements, the magnitude of their signed sum cannot exceed the sum of their magnitudes. This is the triangle inequality for real numbers. It explains why, when interval magnitudes correctly represent the distances traveled, total distance is at least the magnitude of net displacement.
Here is a justification. For any two real numbers \(a\) and \(b\), both \(|a|+|b|\) and \(|a+b|\) are nonnegative. Also,
The last inequality holds because \(|ab|\geq ab\). Since the two quantities being compared are nonnegative, the inequality between their squares implies \(|a+b|\leq |a|+|b|\). Applying this two-number result repeatedly gives the inequality for any finite list.
If \(a\) and \(b\) have opposite signs and neither is zero, then \(|ab|>ab\), so the two-number inequality is strict. More generally, if a list contains both positive and negative terms, its positive and negative contributions partly cancel in the signed sum. Therefore the magnitude of the net change is strictly smaller than the sum of all magnitudes. If all nonzero changes have the same sign, there is no cancellation and equality holds.
For motion divided into intervals with no reversal inside any interval, this theorem says that total distance equals the magnitude of displacement only when the motion has no net cancellation between intervals—that is, when all nonzero interval displacements have the same sign.
Worked Example: Net Change Can Be Small After Long Travel
Worked Example: Net Change Can Be Small After Long Travel
A cyclist travels at \(-3\ \text{km/h}\) for \(0.5\ \text{h}\), remains at rest for \(1.5\ \text{h}\), and then travels at \(2\ \text{km/h}\) for \(2\ \text{h}\). Find the net displacement and total distance.
For the first interval:
For the second interval, the velocity is zero:
For the third interval:
The net displacement is
Each velocity is constant on its interval, so add the magnitudes to get the distance:
Check: The cyclist first travels \(1.5\ \text{km}\) in the negative direction, then \(4\ \text{km}\) in the positive direction. The final position is \(4-1.5=2.5\ \text{km}\) in the positive direction from the start, while the total traveled is \(1.5+4=5.5\ \text{km}\). The rest interval adds neither displacement nor distance.
Average Velocity Does Not Always Give Distance
It is important not to confuse average velocity with a guarantee about motion throughout an interval. Average velocity gives the exact displacement over the whole interval. If direction changes within that interval, the distance can be greater than the magnitude of that displacement.
Worked Example: Zero Average Velocity but Positive Distance
An object moves at \(2\ \text{m/s}\) in the positive direction for the first \(2\ \text{s}\) of a \(4\ \text{s}\) interval, then at \(-2\ \text{m/s}\) for the remaining \(2\ \text{s}\). Find its displacement, average velocity, and distance over the full interval.
During the first half, its displacement is
During the second half, its displacement is
The displacement over the full interval is therefore
The average velocity for the full \(4\ \text{s}\) is displacement divided by elapsed time:
But the direction reverses halfway through, so the distance is the sum of the two traveled lengths:
Check: The object finishes at its starting position, which confirms zero displacement and zero average velocity. It moved \(4\ \text{m}\) out and \(4\ \text{m}\) back, for a total distance of \(8\ \text{m}\).
A Common Mistake: Taking the Magnitude of an Average
A tempting but incorrect calculation in the preceding example is to multiply the magnitude of the average velocity by the full duration and call the result distance:
This result is not the distance traveled. It is the magnitude of the net displacement, which is zero. The forward and backward motions have canceled in the average velocity. To determine distance, we need information that separates the motion into portions with no reversal, as the two \(2\ \text{s}\) intervals did in the example.
Thus, if a listed velocity is an average over a whole interval, multiplying it by the duration gives exact displacement. Summing the magnitudes of those average-velocity-based displacements gives exact distance only when direction does not reverse within each interval. If a reversal may occur, the average value alone is insufficient to determine distance.
Keeping the Two Calculations Straight
When working from interval velocities, first determine what the velocity information represents. If the velocity is constant on each interval, calculate the interval displacement and use its sign to record direction. If it is an average over the whole interval, the same product gives the exact displacement, but do not infer the distance without knowing whether direction reversed within that interval.
Keep the time and velocity units visible so their product has units of distance.
Use velocity times duration when velocity is constant, or when the listed value is the interval’s average velocity.
Positive and negative changes may cancel because the result records final position relative to initial position.
This is valid when motion does not reverse within each interval; otherwise, more detailed information about the motion is needed.
These quantities answer different questions, and both can be useful. Net displacement tells how much the final position differs from the starting position and in which direction. Total distance tells how much motion occurred along the path, regardless of direction. Their units are the same, but their meanings are not interchangeable.
Check Your Understanding
Use signed interval changes where appropriate, and state any condition needed to interpret magnitudes as distance.
- An object moves at \(3\ \text{m/s}\) for \(2\ \text{s}\), then at \(-1\ \text{m/s}\) for \(4\ \text{s}\). If velocity is constant on each interval, what are its net displacement and total distance?
- What does the sign of an interval displacement tell you, and what does its magnitude tell you?
- An object’s average velocity over a \(5\ \text{s}\) interval is \(2\ \text{m/s}\). What displacement does this determine? Does it determine the distance traveled? Explain.
- Under what condition do total distance and the magnitude of net displacement agree for a sequence of straight-line interval changes?
- Why can the sum of the magnitudes of average-velocity-based interval displacements fail to give the actual distance?