Net change theorem: $\displaystyle\int_a^b F'(t)\,dt = F(b) - F(a)$. For velocity $v(t)$: displacement $= \displaystyle\int_a^b v(t)\,dt$, but total distance $= \displaystyle\int_a^b \lvert v(t) \rvert\,dt$. To compute the second, split the interval where $v$ changes sign.
💡 Por qué funciona
A rate times a short time is a small change: $v(t)\,\Delta t$ is how far you move in time $\Delta t$. Adding those small changes and taking the limit gives the total change. When $v < 0$ you move backward, and the integral subtracts that movement, which is right for displacement (where you end up) but wrong for distance (how far the odometer turns). Using $\lvert v \rvert$ counts every bit of motion as positive.
Velocity $v(t) = t^2 - 4t + 3$ on top. The accumulated area below it is the position change: it rises, falls while $v < 0$ on $(1, 3)$, then rises again.
✏️ Ejemplo resuelto: Displacement and distance
A particle moves with $v(t) = t^2 - 4t + 3$ m/s for $0 \le t \le 4$. Find its displacement and total distance.
Population: if $P'(t)$ is a growth rate in people per year, $\int_a^b P'(t)\,dt$ is the change in population.
Cost: integrating the marginal cost from 100 to 200 items gives the extra cost of those 100 items.
Water: integrating a flow rate in liters per minute gives liters added (negative rates count as water removed).
The units always work out: (units per time) times time = units.
⚠️ Error común
Reporting displacement when total distance is asked: answering $\frac{4}{3}$ m in the first example. The particle went forward, came back, and went forward again; the odometer counts all of it. Check: if the velocity ever changes sign on the interval, distance and displacement are different.
Práctica
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