Indefinite integrals and net change

The Fundamental Theorem of Calculus connects integrals with antiderivatives. So we use the integral sign for antiderivatives too. In this section, we introduce this notation. Then we see what an integral of a rate of change means.

Indefinite integrals

The indefinite integral of $f$ is its general antiderivative:

$\displaystyle\int f(x)\,dx=F(x)+C$

means that $F'(x)=f(x)$.

For example,

$\displaystyle\int x^2\,dx=\dfrac{x^3}{3}+C$,

because the derivative of $\dfrac{x^3}{3}$ is $x^2$.

Notice the difference:

They are connected by the Fundamental Theorem: to find a definite integral, find the indefinite integral, then subtract its values at the two ends.

A table of indefinite integrals

These come from the antiderivative formulas. Each can be checked by differentiating the right side.

Also, constants move out, and sums can be integrated one term at a time:

$\displaystyle\int c\,f(x)\,dx=c\int f(x)\,dx$

$\begin{align*}&\int[f(x)\pm g(x)]\,dx\\&=\int f(x)\,dx\pm\int g(x)\,dx\end{align*}$

Example 1: Find

$\displaystyle\int(10x^4-2\sec^2 x)\,dx$.

Solution:

$\begin{align*}&\int(10x^4-2\sec^2 x)\,dx\\&=10\cdot\dfrac{x^5}{5}-2\tan x+C\\&=2x^5-2\tan x+C\end{align*}$

Check: The derivative of $2x^5-2\tan x$ is $10x^4-2\sec^2 x$.

Example 2: Find

$\displaystyle\int\dfrac{x^2+1}{\sqrt{x}}\,dx$.

Solution:

There is no quotient rule for integrals. So simplify first. Divide each term by $x^{1/2}$ (that is, $\sqrt{x}$):

$\dfrac{x^2+1}{\sqrt{x}}=x^{3/2}+x^{-1/2}$

Now integrate one term at a time:

$\begin{align*}&\int(x^{3/2}+x^{-1/2})\,dx\\&=\dfrac{x^{5/2}}{5/2}+\dfrac{x^{1/2}}{1/2}+C\\&=\dfrac{2}{5}x^{5/2}+2x^{1/2}+C\end{align*}$

Example 3: Find

$\displaystyle\int\dfrac{\sin\theta}{\cos^2\theta}\,d\theta$.

Solution:

This is not in the table. But split the fraction:

$\dfrac{\sin\theta}{\cos^2\theta}=\dfrac{1}{\cos\theta}\cdot\dfrac{\sin\theta}{\cos\theta}=\sec\theta\tan\theta$

So

$\displaystyle\int\dfrac{\sin\theta}{\cos^2\theta}\,d\theta=\sec\theta+C$.

Example 4: Find

$\displaystyle\int_1^9\dfrac{2t^2+t^{5/2}-1}{t^2}\,dt$.

Solution:

Divide each term by $t^2$ first:

$\dfrac{2t^2+t^{5/2}-1}{t^2}=2+t^{1/2}-t^{-2}$

An antiderivative is $2t+\dfrac{2}{3}t^{3/2}+\dfrac{1}{t}$. Now use the Fundamental Theorem:

$\begin{align*}&\left[2t+\dfrac{2}{3}t^{3/2}+\dfrac{1}{t}\right]_1^9\\&=\left(18+18+\dfrac{1}{9}\right)-\left(2+\dfrac{2}{3}+1\right)\\&=\dfrac{325}{9}-\dfrac{33}{9}\\&=\dfrac{292}{9}\approx 32.44\end{align*}$

Here $9^{3/2}=(\sqrt{9})^3=27$.

So $\dfrac{2}{3}\cdot 27=18$.

The net change theorem

If $F'$ is the rate of change of $F$, then the Fundamental Theorem says

$\displaystyle\int_a^b F'(x)\,dx=F(b)-F(a)$.

The right side is the change in $F$ from $a$ to $b$. This gives the net change theorem:

The integral of a rate of change is the net change.

Here are some examples:

Example 5: Water flows into a tank at a rate of

$r(t)=200-4t$ liters per minute,

for $0\le t\le 50$. How much water flows in during the first $10$ minutes?

Solution:

By the net change theorem, the amount is the integral of the rate:

$\begin{align*}&\int_0^{10}(200-4t)\,dt\\&=\Big[200t-2t^2\Big]_0^{10}\\&=(2000-200)-0\\&=1800\end{align*}$

So $1800$ liters flow in.

Displacement and distance

For an object moving on a line with velocity $v(t)$:

To find the total distance, split the time interval where $v$ changes sign. Integrate each piece, and add the sizes (absolute values) of the results.

Example 6: A particle moves on a line with velocity

$v(t)=t^2-t-6$ m/s.

(a) Find its displacement for $1\le t\le 4$.

(b) Find the total distance it travels in that time.

143−+tv
The velocity $v(t)=t^2-t-6$. The particle moves backward while $v$ is negative (red), and forward while $v$ is positive (teal).

Solution:

An antiderivative of $v$ is

$F(t)=\dfrac{t^3}{3}-\dfrac{t^2}{2}-6t$.

Its values: $F(1)=-\dfrac{37}{6}$, $F(3)=-\dfrac{27}{2}$, and $F(4)=-\dfrac{32}{3}$.

(a) The displacement:

$\begin{align*}&\int_1^4 v(t)\,dt\\&=F(4)-F(1)\\&=-\dfrac{32}{3}+\dfrac{37}{6}\\&=-\dfrac{9}{2}\end{align*}$

The particle ends $4.5$ m behind where it started.

(b) Factor the velocity:

$v(t)=(t-3)(t+2)$

  • On $(1,3)$: $v(t)<0$.
  • On $(3,4)$: $v(t)>0$.

Integrate each piece:

$\begin{align*}&\int_1^3 v(t)\,dt\\&=F(3)-F(1)\\&=-\dfrac{27}{2}+\dfrac{37}{6}\\&=-\dfrac{22}{3}\end{align*}$

$\begin{align*}&\int_3^4 v(t)\,dt\\&=F(4)-F(3)\\&=-\dfrac{32}{3}+\dfrac{27}{2}\\&=\dfrac{17}{6}\end{align*}$

Add the sizes:

$\dfrac{22}{3}+\dfrac{17}{6}=\dfrac{61}{6}\approx 10.17$ m

The particle moved $\dfrac{22}{3}$ m backward and then $\dfrac{17}{6}$ m forward. Its total distance is about $10.17$ m, but its displacement is only $-4.5$ m.

Summary