Physics · Unit 1: Kinematics ·  Activity 1-1-1

Deep Dive: Distance, Displacement, and Speed

🔬 Deep Dive
This is your textbook for this topic. Take your time. Read it more than once.
1.1.1.AConcept

Distance: The Path Length

Distance is the total length of the path an object actually travels. It is a scalar — a number with a unit and nothing else, no direction attached. If you walk 60 meters down a hallway, distance says 60 m. If you then walk back 40 meters, distance doesn't care that you reversed course — it just keeps adding.

distance = sum of all path lengths traveled

Because distance only ever accumulates, it can never be negative and it can never decrease over time. Every step you take — forward, backward, sideways, in circles — adds to it.

🔑Distance answers the question: "How much ground did you cover?" It says nothing about where you ended up.
1.1.1.BMath

Displacement: Where You Ended Up

Displacement only compares your final position to your starting position. It is the straight-line change in position:

Δx = x_f − x_i

Displacement is a vector — it has both size and direction. On a one-dimensional number line, direction shows up as a sign: positive means net motion one way, negative means net motion the other way. (You'll formalize signed direction in Lesson 1-1-3 — for now, just notice that Δx can come out positive, negative, or zero depending on where x_i and x_f fall.)

💡Displacement doesn't care about the route you took, how many times you backtracked, or how long the trip lasted. It cares only about start and end.
ExampleWorked Example — Walking Down the Hall

You start at position x_i = 5 m along a hallway, walk to x = 45 m, then walk back to x_f = 30 m. Find the total distance traveled and the displacement.

1.1.1.CWatch Out

The Round-Trip Case

The single most common error with these two quantities: assuming distance and displacement are always the same number, or assuming that "no displacement" means "no motion happened." Neither is true.

⚠️A runner completes a full lap of a 400 m track and returns to the exact spot she started. Her distance traveled is 400 m. Her displacement is 0 m — x_f and x_i are identical points. She is exhausted and has covered zero net distance, both at once.

Set a start position, a turnaround point, and a final position along a number line (in meters). Watch how distance and displacement respond independently.

x_start (m)0
x_turn (m)60
x_final (m)20
time (s)50
0m60m20m
leg 1 + leg 2
60 m + 40 m
distance
100 m
scalar, always ≥ 0
displacement Δx
+20 m
net rightward
average speed
2.00 m/s
distance / time

Try setting x_final equal to x_start — displacement drops to zero while distance stays large and positive. That's the round-trip case in action.

ExampleGuided Example — Out and Back

A cyclist starts at x_i = 0 m, rides out to x = 60 m, then rides back to x_f = 20 m. Find the distance, the displacement, and identify which one changed.

Step 1Identify the legs of the trip
Leg 1: 0 m → 60 m (60 m of riding). Leg 2: 60 m → 20 m (40 m of riding, in the reverse direction).
1.1.1.DMath

Average Speed

Speed is a rate: how much distance is covered per unit of time. Because it's built from distance (a scalar) and time (always positive), speed is also a scalar — no direction attached.

average speed = total distance / total time

Average speed treats the entire trip as one lump sum. It doesn't matter if you sprinted for part of the trip and crawled for another part — average speed only sees the total distance and the total time elapsed.

🔑Because average speed uses distance, not displacement, a round trip that ends with zero displacement can still have a large, very real average speed. The runner from the misconception above did not average "0 m/s" for her lap.
ExampleWorked Example — Average Speed of a Round Trip

A hiker walks 3.0 km out to a lookout in 40 minutes, then walks back along the same trail in 30 minutes. Find her average speed for the entire hike.

1.1.1.EConcept

Looking Ahead to Velocity

You now have three tools: distance, displacement, and speed. There's a fourth idea waiting just around the corner — velocity, which is to displacement what speed is to distance: a rate, but this time a rate built from a vector. Average velocity = Δx / Δt.

Scalars (today)

distance, average speed — magnitude only, never negative

Vectors (starting 1-1-3)

displacement, velocity — magnitude AND direction, signed numbers

💡In Lesson 1-1-3 you'll formalize direction using positive and negative signs instead of arrows. Everything you just learned about displacement being "final minus initial" carries over directly — you're just about to get much more precise about what the sign means.
← Back to Activity 1-1-1Do the Activity →Next lesson: 1-1-2, Reading Position-Time Graphs.