Motion Revisited: Accumulating Velocity
- Recover displacement by integrating velocity over an interval
- Compute total distance traveled by integrating the speed |v(t)|
- Find position from velocity and an initial condition
Integration reverses the motion derivatives
In Unit 4 you differentiated position to get velocity; integration runs it backward. The displacement over [a, b] is the accumulated velocity, ∫[a to b] v(t) dt = s(b) − s(a) (the Net Change Theorem). Likewise integrating acceleration recovers velocity. Integration is how you rebuild position and velocity from the rates that describe the motion.
Displacement vs. total distance — with integrals
Integrating velocity directly gives displacement, where motion in opposite directions cancels. To get total distance traveled you integrate the speed, ∫[a to b] |v(t)| dt, so every bit of motion counts as positive. In practice you find where v changes sign, split the interval there, and add the absolute values of the pieces — the integral version of the Unit 4 idea.
Position from velocity and a starting point
To find the actual position at a time, you need an initial condition. Since s(t) = s(a) + ∫[a to t] v(τ) dτ, the position at time t is the starting position plus the accumulated displacement since a. Without the initial position you can find only the change in position, not where the particle actually is.
A particle has velocity v(t) = t − 3 (m/s) for 0 ≤ t ≤ 5. Find its displacement and its total distance traveled.
- 1.Displacement is ∫[0 to 5] (t − 3) dt = [t²/2 − 3t] from 0 to 5 = (25/2 − 15) − 0 = −2.5 m.
- 2.For total distance, find where v = 0: t − 3 = 0 at t = 3, where velocity changes sign.
- 3.On [0, 3], v < 0: ∫[0 to 3] (t − 3) dt = (9/2 − 9) = −4.5, absolute value 4.5.
- 4.On [3, 5], v > 0: ∫[3 to 5] (t − 3) dt = (25/2 − 15) − (9/2 − 9) = (−2.5) − (−4.5) = 2. Add absolute values: 4.5 + 2.
To get total distance you must integrate |v(t)|, not v(t). Split the interval at every time velocity changes sign and add the absolute values — integrating v directly gives only the net displacement, where opposite motions cancel.
The displacement of a particle over [a, b] is given by:
A particle starts at position s(0) = 4 with velocity v(t). What is its position at t = 3?
Watch the wording: "displacement" or "position change" means ∫v dt, while "total distance traveled" means ∫|v| dt with the interval split at sign changes. And "where is the particle" always needs the initial position added to the integral.
Answer the 2 checkpoints as you read.
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