← MATH 161 MathScape 0 MATH161

Applications of Net Change

4 min read

Jump to a section
Reference: Stewart §4.4

Textbook Reference

Primary source OpenStax Calculus Volume 2, Section 1.4: “Integration Formulas and the Net Change Theorem”
Direct link https://openstax.org/books/calculus-volume-2/pages/1-4-integration-formulas-and-the-net-change-theorem
Textbook used in class Stewart, Calculus, Section 4.4: “Indefinite Integrals and the Net Change Theorem”

Opening Scenario

FTC Part 2 says that $\displaystyle\int_a^b F'(x)\,dx = F(b) - F(a)$. Written in words: the integral of a rate of change over an interval equals the net change in the quantity over that interval. This statement -- the Net Change Theorem -- is the same as FTC Part 2, but stated in a way that makes applied problems immediate.

Velocity is the rate of change of position. Marginal cost is the rate of change of total cost. Birth rate minus death rate is the rate of change of population. In each case, integrating the rate over a time interval gives the net change in the quantity.


Quick Reference

Net Change Theorem. If $F'(x) = f(x)$, then $$\int_a^b f(x)\,dx = F(b) - F(a) = \text{net change in } F \text{ from } a \text{ to } b.$$

Key applications:

Rate of change $f(t)$ Net change $\displaystyle\int_a^b f(t)\,dt$
Velocity $v(t)$ Displacement (net change in position)
Speed $|v(t)|$ Total distance traveled
Acceleration $a(t)$ Change in velocity
Marginal cost $C'(x)$ Change in total cost from $x = a$ to $x = b$ units
Population growth rate $P'(t)$ Change in population

Key Concepts

1. Displacement vs. Distance Traveled

When a particle moves with velocity $v(t)$ on $[t_1, t_2]$:

These agree only when $v(t)$ does not change sign on $[t_1, t_2]$. When $v$ changes sign (the particle reverses direction), the integral of $v$ cancels some motion, but the integral of $|v|$ does not.

How to compute total distance when $v$ changes sign:

  1. Find the zeros of $v(t)$ on $[t_1, t_2]$. These are the reversal times.
  2. Split the integral at each reversal.
  3. Add the absolute values of each piece.

2. The Net Change Perspective Unifies Many Fields

The same formula $\int_a^b f(x)\,dx = F(b) - F(a)$ applies in many contexts:

The specific field determines what $f$ and $F$ represent. The mathematics is identical.

3. Reading the Integral as Accumulation

An alternative reading of $\displaystyle\int_a^b f(x)\,dx$: it accumulates (adds up) infinitely many infinitesimal amounts $f(x)\,dx$ over $[a, b]$. Each $f(x)\,dx$ is the contribution to the total during the infinitesimal interval $[x, x + dx]$.

Common misconception

“Displacement and distance are always the same for a moving particle.” They are the same only when the particle moves in one direction throughout the interval. If the particle reverses direction, displacement can be zero even though the particle has traveled a positive total distance.


Worked Example

A particle moves along a line with velocity $v(t) = t^2 - 4t + 3$ m/s for $0 \leq t \leq 4$.

(a) Find the displacement over $[0, 4]$.

$\displaystyle\int_0^4 (t^2 - 4t + 3)\,dt = \left[\frac{t^3}{3} - 2t^2 + 3t\right]_0^4 = \left(\frac{64}{3} - 32 + 12\right) - 0 = \frac{64}{3} - 20 = \frac{4}{3}$ m.

(b) Find the total distance traveled over $[0, 4]$.

First find zeros: $t^2 - 4t + 3 = (t-1)(t-3) = 0$, so $t = 1$ and $t = 3$.

Check signs: $v(0) = 3 > 0$, $v(2) = -1 < 0$, $v(4) = 3 > 0$.

Split at the reversal times and add absolute values:

$$\text{Distance} = \left|\int_0^1 v\,dt\right| + \left|\int_1^3 v\,dt\right| + \left|\int_3^4 v\,dt\right|.$$

$\displaystyle\int_0^1(t^2-4t+3)\,dt = \left[\frac{t^3}{3}-2t^2+3t\right]_0^1 = \frac{1}{3} - 2 + 3 = \frac{4}{3}$.

$\displaystyle\int_1^3(t^2-4t+3)\,dt = \left[\frac{t^3}{3}-2t^2+3t\right]_1^3 = (9-18+9) - \frac{4}{3} = 0 - \frac{4}{3} = -\frac{4}{3}$.

$\displaystyle\int_3^4(t^2-4t+3)\,dt = \left[\frac{t^3}{3}-2t^2+3t\right]_3^4 = \frac{4}{3} - 0 = \frac{4}{3}$.

$$\text{Distance} = \frac{4}{3} + \frac{4}{3} + \frac{4}{3} = 4 \text{ m}.$$

Boxed answers: Displacement $= \dfrac{4}{3}$ m; total distance $= 4$ m.


Common Errors Summary

Error Example Correction
Confusing displacement and distance Reporting $\int_0^4 v\,dt$ as total distance when $v$ changes sign When $v$ changes sign, compute $\int |v|\,dt$ by splitting at zeros
Forgetting to split the integral Computing $\int_{t_1}^{t_2} v\,dt$ directly when $v < 0$ partway Find zeros of $v$, split the integral, then sum absolute values
Misidentifying which quantity is the rate Integrating position instead of velocity The integrand must be a rate; position is $F$, velocity $v = F'$ is the rate

Leveled Practice

Level 1 -- Direct Application

Problem 1. A particle’s velocity is $v(t) = 3t^2 - 6t$ for $0 \leq t \leq 3$. Find the displacement.

Show answer

$\displaystyle\int_0^3(3t^2 - 6t)\,dt = \left[t^3 - 3t^2\right]_0^3 = (27 - 27) - 0 = 0$ m.

The particle returns to its starting position.


Level 2 -- Distance with Direction Change

Problem 2. For the same $v(t) = 3t^2 - 6t$ on $[0, 3]$, find the total distance traveled.

Show answer

Zero at $t = 2$ (factor: $3t(t-2) = 0$). $v < 0$ on $(0, 2)$, $v > 0$ on $(2, 3)$.

$\displaystyle\int_0^2(3t^2-6t)\,dt = [t^3-3t^2]_0^2 = (8-12) = -4$. $|\text{\ }| = 4$.

$\displaystyle\int_2^3(3t^2-6t)\,dt = [t^3-3t^2]_2^3 = (27-27)-(8-12) = 0-(-4) = 4$.

Total distance $= 4 + 4 = 8$ m.


Mastery Checklist


Mental Model

Think of $f(x)$ as a water faucet that controls flow rate. When $f > 0$, water enters a tank; when $f < 0$, water drains. $\displaystyle\int_a^b f(x)\,dx$ is the net change in the water level -- inflow minus outflow. $\displaystyle\int_a^b |f(x)|\,dx$ is the total water that passed through the faucet in either direction. The distinction matters any time the sign of $f$ changes.


Connections

Looking back

Looking ahead


Back to Integration Foundations | Next: The Substitution Rule