Navigation: Wiki Home > Skills > Displacement vs Total Distance
When a particle moves along a line, there are two natural questions:
These sound similar but have very different answers when the particle changes direction!
graph LR
subgraph "Prerequisites"
A["Net Change<br/>Theorem"]
B["Velocity as<br/>Derivative"]
end
subgraph "This Skill"
C["Displacement vs<br/>Total Distance"]
end
subgraph "Unlocks"
D["Work and<br/>Energy"]
E["Arc Length"]
F["Motion<br/>Applications"]
end
A --> C
B -.-> C
C --> D
C --> E
C --> F
click A "net-change-theorem.html"
click C "displacement-vs-total-distance.html"
click B "../ch2-sec1/instantaneous-velocity.html"
click D "../ch5-sec4/pumping-work.html"
click E "../ch13-sec3/arc-length-vector.html"
From Net Change Theorem:
From Computing Indefinite Integrals:
If these feel unfamiliar, review the prerequisite pages before continuing.
| Property | Value |
|---|---|
| Concept | Indefinite Integrals & Net Change |
| Chapter | Chapter 4, Section 4 |
| Difficulty | Intermediate |
| Time | ~20 minutes |
For a particle with velocity $v(t)$ on the interval $[t_1, t_2]$:
| Quantity | Formula | Meaning |
|---|---|---|
| Displacement | $\displaystyle\int_{t_1}^{t_2} v(t)\, dt$ | Net position change (signed) |
| Total Distance | $\displaystyle\int_{t_1}^{t_2} \vert v(t)\vert \, dt$ | Total ground covered (always ≥ 0) |
Displacement counts movement to the right as positive and movement to the left as negative. They can cancel out.
Total distance counts ALL movement as positive. Nothing cancels.
Visual Example:
Start: ─────● (position 0)
Move right 5: ──────────● (position 5)
Move left 8: ●────────── (position -3)
Displacement: -3 (ended 3 units left of start)
Total distance: 5 + 8 = 13 (traveled 13 units total)
Since $\vert v(t)\vert = v(t)$ when $v(t) \geq 0$ and $\vert v(t)\vert = -v(t)$ when $v(t) < 0$:
Step 1: Find where $v(t) = 0$ (the particle changes direction)
Step 2: Split the integral at these points
Step 3: On intervals where $v(t) > 0$: integrate $v(t)$ On intervals where $v(t) < 0$: integrate $-v(t)$
Step 4: Add all the pieces (all positive)
On a velocity-time graph:
v(t) ↑
│ ╱╲
│ ╱ ╲ A₁ (positive area)
│ ╱ ╲
─────┼─╱──────╲─────────→ t
│ ╲ ╱
│ ╲ ╱ A₂ (negative area)
│ ╲╱
Displacement = A₁ - A₂
Total Distance = A₁ + A₂
A car drives 30 miles east, then 10 miles west.
(a) What is the car's displacement?
(b) What is the total distance traveled?
(c) If this took 1 hour total, could you find the average velocity? Average speed?
A particle moves with velocity $v(t) = 3t^2 - 6t + 5$ m/s for $0 \leq t \leq 2$.
(a) Verify that $v(t) > 0$ for all $t$ in $[0, 2]$.
(b) Find the displacement.
(c) Find the total distance traveled.
A particle moves with velocity $v(t) = t^2 - t - 6$ m/s for $1 \leq t \leq 4$ seconds.
(a) Find the displacement during this time period.
(b) Find the total distance traveled.
A particle has velocity $v(t) = 3t - 5$ m/s for $0 \leq t \leq 3$ seconds.
(a) Find the displacement.
(b) Find the total distance traveled.
(c) Sketch a graph of position $s(t)$ if $s(0) = 2$.
A particle starts from rest and has acceleration $a(t) = t + 4$ m/s² for $0 \leq t \leq 10$ seconds.
(a) Find the velocity function $v(t)$.
(b) Show that $v(t) > 0$ for all $t > 0$, so the particle always moves in the positive direction.
(c) Find the total distance traveled during $0 \leq t \leq 10$.
The Taxi Meter vs GPS
Think of a taxi meter and a GPS:
The integral $\int v(t)\, dt$ is like GPS. The integral $\int \vert v(t)\vert \, dt$ is like the taxi meter.
| Error | Correction |
|---|---|
| Using $\int v(t)\, dt$ for total distance | Must use $\int \vert v(t)\vert \, dt$ when direction changes |
| Forgetting to check for sign changes | Always solve $v(t) = 0$ first |
| Getting wrong sign when $v < 0$ | When $v(t) < 0$, $\vert v(t)\vert = -v(t)$ |
| Adding areas with wrong signs | For total distance, ALL areas are positive |
Looking back:
Looking ahead:
Real-world connections:
| Previous | Up | Next |
|---|---|---|
| Net Change Theorem | Skills Index | u-Substitution |
Last updated: 2026-01-22