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If the derivative is the mathematical tool for understanding "instantaneous change," then the integral is the tool for "total accumulation." In the previous units of AP Calculus, we focused on the mechanics of integration—antiderivatives, the Fundamental Theorem of Calculus, and techniques like $u$-substitution and integration by parts. Now, we transition from the how to the why.
Unit 8, Applications of Integration, represents the culmination of integral calculus. It allows us to step out of the abstract world of $x$ and $y$ and into the three-dimensional physical world. How do we calculate the exact volume of a biological cell with an irregular shape? How can an engineer determine the amount of material needed to create a cooling tower for a power plant? How do we find the exact distance an object travels along a curved path?
This chapter bridges the gap between geometry and calculus. We will move beyond simple formulas for the area of a rectangle or the volume of a sphere to find the area and volume of virtually any shape defined by functions. For BC students, we will extend these concepts to the realm of polar coordinates and parametric equations. By the end of this unit, you will see the world not as a collection of static shapes, but as a series of accumulations that can be precisely measured and analyzed.
In discrete math, the average of $n$ numbers is $\frac{1}{n} \sum x_i$. In calculus, a function $f(x)$ has infinitely many values on $[a, b]$. To find the average, we divide the total accumulation (the integral) by the length of the interval.
The Formula:
$$f_{avg} = \frac{1}{b-a} \int_a^b f(x) , dx$$
The Mean Value Theorem for Integrals:
This theorem guarantees that for a continuous function, there is at least one point $x = c$ where the function actually equals its average value.
$$f(c)(b-a) = \int_a^b f(x) , dx$$
Geometrically, this means there is a rectangle with height $f(c)$ and width $(b-a)$ that has the exact same area as the region under the curve.
To find the area between two curves $f(x)$ and $g(x)$, we sum up an infinite number of infinitesimal rectangles.
Integration with respect to $x$:
If $f(x) \ge g(x)$ for all $x$ in $[a, b]$:
$$\text{Area} = \int_a^b [f(x) - g(x)] , dx$$
Tip: Think "Top function minus Bottom function".
Integration with respect to $y$:
Sometimes curves are defined as $x = f(y)$. If $f(y) \ge g(y)$ (meaning $f(y)$ is further to the right):
$$\text{Area} = \int_c^d [f(y) - g(y)] , dy$$
Tip: Think "Right function minus Left function".
If we know the area of a cross-section $A(x)$ perpendicular to the $x$-axis, the volume $V$ is the integral of that area.
The Formula:
$$V = \int_a^b A(x) , dx$$
Common Cross-Section Areas $A(x)$ based on a base length $s$ (where $s = f(x) - g(x)$):
When a region is rotated around an axis, it creates a solid.
Used when the region is adjacent to the axis of rotation. The cross-section is a circle with area $\pi R^2$.
$$V = \pi \int_a^b [R(x)]^2 , dx$$
Where $R(x)$ is the distance from the axis to the function.
Used when there is a "gap" between the region and the axis. The cross-section is a ring (washer) with area $\pi(R_{outer}^2 - R_{inner}^2)$.
$$V = \pi \int_a^b ([R(x)]^2 - [r(x)]^2) , dx$$
Where $R(x)$ is the outer radius and $r(x)$ is the inner radius.
To find the length of a smooth curve $y = f(x)$ from $x=a$ to $x=b$, we use the Pythagorean-based formula:
$$L = \int_a^b \sqrt{1 + [f'(x)]^2} , dx$$
For Parametric Equations $x=x(t), y=y(t)$:
$$L = \int_{t_1}^{t_2} \sqrt{(\frac{dx}{dt})^2 + (\frac{dy}{dt})^2} , dt$$
In polar coordinates, we don't use rectangles; we use circular sectors. The area of a sector is $\frac{1}{2} r^2 \theta$.
The Formula:
$$\text{Area} = \int_\alpha^\beta \frac{1}{2} [r(\theta)]^2 , d\theta$$
For the area between two polar curves $r_{out}$ and $r_{in}$:
$$\text{Area} = \frac{1}{2} \int_\alpha^\beta ([r_{out}(\theta)]^2 - [r_{in}(\theta)]^2) , d\theta$$
Find the average value of $f(x) = x^2$ on the interval $[0, 3]$.
Solution:
$$f_{avg} = \frac{1}{3-0} \int_0^3 x^2 , dx = \frac{1}{3} \left[ \frac{x^3}{3} \right]_0^3 = \frac{1}{3} (\frac{27}{3} - 0) = 3$$
Find the value of $c$ guaranteed by the MVT for Integrals for $f(x) = \sqrt{x}$ on $[0, 4]$.
Solution:
First, find the average value:
$$f_{avg} = \frac{1}{4-0} \int_0^4 x^{1/2} , dx = \frac{1}{4} \left[ \frac{2}{3}x^{3/2} \right]_0^4 = \frac{1}{4} (\frac{2}{3} \cdot 8) = \frac{4}{3}$$
Set $f(c) = \frac{4}{3}$:
$$\sqrt{c} = \frac{4}{3} \implies c = \frac{16}{9}$$
Since $16/9 \approx 1.77$ is in $[0, 4]$, $c = 16/9$.
Find the area of the region bounded by $f(x) = x^2$ and $g(x) = x + 2$.
Solution:
Find intersections: $x^2 = x + 2 \implies x^2 - x - 2 = 0 \implies (x-2)(x+1)=0$. Intersects at $x = -1, 2$.
On $[-1, 2]$, $x+2 \ge x^2$.
$$\text{Area} = \int_{-1}^2 (x + 2 - x^2) , dx = \left[ \frac{x^2}{2} + 2x - \frac{x^3}{3} \right]_{-1}^2$$
$$= (2 + 4 - \frac{8}{3}) - (\frac{1}{2} - 2 + \frac{1}{3}) = \frac{10}{3} - (-\frac{7}{6}) = \frac{20+7}{6} = \frac{27}{6} = 4.5$$
Find the area bounded by $y^2 = x$ and $y = x - 2$.
Solution:
Rewrite as $x = y^2$ and $x = y + 2$.
Intersections: $y^2 = y + 2 \implies y^2 - y - 2 = 0 \implies y = 2, -1$.
Right function: $x = y + 2$. Left function: $x = y^2$.
$$\text{Area} = \int_{-1}^2 (y + 2 - y^2) , dy = \left[ \frac{y^2}{2} + 2y - \frac{y^3}{3} \right]_{-1}^2 = 4.5$$
The base of a solid is the circle $x^2 + y^2 = 1$. Cross sections perpendicular to the $x$-axis are squares. Find the volume.
Solution:
The circle is $y = \pm \sqrt{1-x^2}$. The side length $s$ of the square is the distance between top and bottom:
$s = \sqrt{1-x^2} - (-\sqrt{1-x^2}) = 2\sqrt{1-x^2}$.
$A(x) = s^2 = (2\sqrt{1-x^2})^2 = 4(1-x^2)$.
$$V = \int_{-1}^1 4(1-x^2) , dx = 4 [x - \frac{x^3}{3}]_{-1}^1 = 4[(1 - 1/3) - (-1 + 1/3)] = 4[2/3 + 2/3] = \frac{16}{3}$$
Find the volume of the solid generated by rotating $y = \sqrt{x}$ from $x=0$ to $x=4$ about the $x$-axis.
Solution:
$R(x) = \sqrt{x}$.
$$V = \pi \int_0^4 (\sqrt{x})^2 , dx = \pi \int_0^4 x , dx = \pi [\frac{x^2}{2}]_0^4 = 8\pi$$
Find the volume rotating the region bounded by $y = x^2$ and $y = \sqrt{x}$ about the $x$-axis.
Solution:
Intersections at $x=0, 1$. $R_{out} = \sqrt{x}$, $r_{in} = x^2$.
$$V = \pi \int_0^1 ((\sqrt{x})^2 - (x^2)^2) , dx = \pi \int_0^1 (x - x^4) , dx = \pi [\frac{x^2}{2} - \frac{x^5}{5}]_0^1 = \pi (1/2 - 1/5) = \frac{3\pi}{10}$$
Rotate $y = x^3$, $y = 8$, and $x = 0$ about the $y$-axis.
Solution:
Rewrite as $x = y^{1/3}$. Bounds for $y$ are $0$ to $8$.
$$V = \pi \int_0^8 (y^{1/3})^2 , dy = \pi \int_0^8 y^{2/3} , dy = \pi [\frac{3}{5}y^{5/3}]_0^8 = \pi \cdot \frac{3}{5} \cdot 32 = \frac{96\pi}{5}$$
Rotate the region bounded by $y = x^2$ and $y = 4$ about the line $y = 5$.
Solution:
Intersections at $x = -2, 2$.
$R_{out} = \text{distance from } y=5 \text{ to } y=x^2 \implies 5 - x^2$.
$r_{in} = \text{distance from } y=5 \text{ to } y=4 \implies 5 - 4 = 1$.
$$V = \pi \int_{-2}^2 ((5-x^2)^2 - 1^2) , dx = \pi \int_{-2}^2 (25 - 10x^2 + x^4 - 1) , dx$$
$$= \pi \int_{-2}^2 (24 - 10x^2 + x^4) , dx = \pi [24x - \frac{10x^3}{3} + \frac{x^5}{5}]_{-2}^2 = \frac{832\pi}{15}$$
Find the arc length of $f(x) = \frac{2}{3}x^{3/2}$ from $x=0$ to $x=3$.
Solution:
$f'(x) = x^{1/2}$.
$$L = \int_0^3 \sqrt{1 + (x^{1/2})^2} , dx = \int_0^3 \sqrt{1 + x} , dx$$
Let $u = 1+x, du=dx$.
$$L = \int_1^4 u^{1/2} , du = [\frac{2}{3}u^{3/2}]_1^4 = \frac{2}{3}(8 - 1) = \frac{14}{3}$$
Find the length of the path $x = \cos t, y = \sin t$ for $0 \le t \le \pi$.
Solution:
$\frac{dx}{dt} = -\sin t, \frac{dy}{dt} = \cos t$.
$$L = \int_0^\pi \sqrt{(-\sin t)^2 + (\cos t)^2} , dt = \int_0^\pi \sqrt{1} , dt = [t]_0^\pi = \pi$$
(This makes sense as it is half the circumference of a unit circle).
Find the area of $r = 3 \sin \theta$.
Solution:
This is a circle of diameter 3. It is traced once from $0$ to $\pi$.
$$\text{Area} = \frac{1}{2} \int_0^\pi (3 \sin \theta)^2 , d\theta = \frac{9}{2} \int_0^\pi \sin^2 \theta , d\theta$$
Using $\sin^2 \theta = \frac{1-\cos 2\theta}{2}$:
$$\text{Area} = \frac{9}{4} \int_0^\pi (1 - \cos 2\theta) , d\theta = \frac{9}{4} [\theta - \frac{1}{2}\sin 2\theta]_0^\pi = \frac{9\pi}{4}$$
Find the area inside $r = 1 + \cos \theta$.
Solution:
Integrated from $0$ to $2\pi$.
$$\text{Area} = \frac{1}{2} \int_0^{2\pi} (1 + \cos \theta)^2 , d\theta = \frac{1}{2} \int_0^{2\pi} (1 + 2\cos \theta + \cos^2 \theta) , d\theta$$
$$= \frac{1}{2} \int_0^{2\pi} (1 + 2\cos \theta + \frac{1 + \cos 2\theta}{2}) , d\theta = \frac{1}{2} \int_0^{2\pi} (1.5 + 2\cos \theta + 0.5\cos 2\theta) , d\theta$$
$$= \frac{1}{2} [1.5\theta + 2\sin \theta + 0.25\sin 2\theta]_0^{2\pi} = \frac{1}{2} (3\pi) = \frac{3\pi}{2}$$
Water flows into a tank at a rate $R(t) = 20e^{-0.1t}$ liters/min. How much water enters from $t=0$ to $t=10$?
Solution:
$$\text{Net Change} = \int_0^{10} 20e^{-0.1t} , dt = 20 [\frac{e^{-0.1t}}{-0.1}]_0^{10} = -200 [e^{-1} - e^0] = 200(1 - \frac{1}{e}) \approx 126.42 \text{ liters.}$$
Base is bounded by $y = e^x, y=0, x=0, x=ln(3)$. Cross sections perpendicular to the $x$-axis are semicircles.
Solution:
$s = e^x$. Area $A(x) = \frac{\pi}{8}s^2 = \frac{\pi}{8}e^{2x}$.
$$V = \frac{\pi}{8} \int_0^{\ln 3} e^{2x} , dx = \frac{\pi}{8} [\frac{1}{2}e^{2x}]_0^{\ln 3} = \frac{\pi}{16} (e^{2\ln 3} - e^0) = \frac{\pi}{16} (9 - 1) = \frac{\pi}{2}$$
Rotate the region bounded by $x = y^2$ and $x = 1$ about the line $x = 1$.
Solution:
Since the axis is vertical ($x=1$), we integrate with respect to $y$.
Intersections: $y^2 = 1 \implies y = \pm 1$.
The radius is the distance from $x=1$ to $x=y^2$: $R(y) = 1 - y^2$.
$$V = \pi \int_{-1}^1 (1-y^2)^2 , dy = \pi \int_{-1}^1 (1 - 2y^2 + y^4) , dy = \pi [y - \frac{2y^3}{3} + \frac{y^5}{5}]_{-1}^1$$
$$= \pi [(1 - 2/3 + 1/5) - (-1 + 2/3 - 1/5)] = \pi [8/15 + 8/15] = \frac{16\pi}{15}$$
A particle's velocity is $v(t) = t^2 - 4$. Find the displacement from $t=0$ to $t=3$.
Solution:
$$\text{Displacement} = \int_0^3 (t^2 - 4) , dt = [\frac{t^3}{3} - 4t]_0^3 = (9 - 12) - 0 = -3$$
Using $v(t) = t^2 - 4$ from Example 17, find total distance on $[0, 3]$.
Solution:
$\text{Distance} = \int_0^3 |t^2 - 4| , dt$.
$t^2 - 4 = 0$ at $t=2$. On $[0, 2]$, $v(t) \le 0$. On $[2, 3]$, $v(t) \ge 0$.
$$\text{Dist} = \int_0^2 -(t^2 - 4) , dt + \int_2^3 (t^2 - 4) , dt$$
$$= [-t^3/3 + 4t]_0^2 + [t^3/3 - 4t]_2^3 = (-8/3 + 8) + [(9-12) - (8/3 - 8)] = \frac{16}{3} + [-3 + 16/3] = \frac{16+7}{3} = \frac{23}{3}$$
Find the area inside $r = 3 \sin \theta$ and outside $r = 2 - \sin \theta$.
Solution:
Find intersections: $3 \sin \theta = 2 - \sin \theta \implies 4 \sin \theta = 2 \implies \sin \theta = 1/2$.
$\theta = \pi/6, 5\pi/6$.
$$\text{Area} = \frac{1}{2} \int_{\pi/6}^{5\pi/6} [(3 \sin \theta)^2 - (2 - \sin \theta)^2] , d\theta$$
$$= \frac{1}{2} \int_{\pi/6}^{5\pi/6} [9 \sin^2 \theta - (4 - 4 \sin \theta + \sin^2 \theta)] , d\theta$$
$$= \frac{1}{2} \int_{\pi/6}^{5\pi/6} [8 \sin^2 \theta + 4 \sin \theta - 4] , d\theta$$
Using $8 \sin^2 \theta = 4(1 - \cos 2\theta)$:
$$= \frac{1}{2} \int_{\pi/6}^{5\pi/6} [4 - 4\cos 2\theta + 4\sin \theta - 4] , d\theta = \frac{1}{2} \int_{\pi/6}^{5\pi/6} (4\sin \theta - 4\cos 2\theta) , d\theta$$
$$= \frac{1}{2} [-4\cos \theta - 2\sin 2\theta]{\pi/6}^{5\pi/6} = 2 [-\cos \theta - \frac{1}{2}\sin 2\theta]{\pi/6}^{5\pi/6}$$
$$= 2 [(\frac{\sqrt{3}}{2} - \frac{1}{2}(-\frac{\sqrt{3}}{2})) - (-\frac{\sqrt{3}}{2} - \frac{1}{2}(\frac{\sqrt{3}}{2}))] = 3\sqrt{3}$$
A cable weighing 2 lbs/ft is used to lift a 100 lb bucket from a 50 ft well. Find the work done.
Solution:
Work = $\int F(x) , dx$. Let $x$ be the length of cable already pulled up.
Weight at height $x$ is: (Bucket) + (Remaining Cable) $= 100 + 2(50 - x) = 200 - 2x$.
$$W = \int_0^{50} (200 - 2x) , dx = [200x - x^2]_0^{50} = 10000 - 2500 = 7500 \text{ ft-lb.}$$
Find the area of the region in the first quadrant bounded by $y = \sqrt{x}$, $y = x-2$, and the $y$-axis.
Solution:
This region has two "bottom" functions if integrating $dx$ (from $0$ to $2$, bottom is $y=0$; from $2$ to $4$, bottom is $x-2$). It is easier to use $dy$.
Left curve: $x = 0$. Right curve: $y = \sqrt{x} \implies x = y^2$ (initially) then $y = x-2 \implies x = y+2$.
Actually, the right boundaries are $x = y^2$ and the $y$-axis is the left.
Wait, let's re-sketch. The curves are $y = \sqrt{x}$ (top), $x = 0$ (left), $y=x-2$ (right/bottom).
Intersection: $\sqrt{x} = x-2 \implies x = x^2 - 4x + 4 \implies x^2 - 5x + 4 = 0 \implies x=4, y=2$.
Integrating $dy$ from $y=0$ to $y=2$:
Right curve is $x = y+2$. Left curve is $x = y^2$.
$$\text{Area} = \int_0^2 (y+2 - y^2) , dy = [\frac{y^2}{2} + 2y - \frac{y^3}{3}]_0^2 = 2 + 4 - 8/3 = 10/3$$
Region bounded by $y = e^{-x^2}, y=0, x=0, x=1$. Rotate about $x = -1$.
Solution:
(Note: AP Calculus usually uses Washer/Disk. While Shell is a BC topic in some schools, for AP we stick to Washer by integrating $dy$ or we set up the integral based on the geometry).
Since rotating about a vertical axis $x=-1$, and the function is $y=f(x)$, Shell Method is most efficient:
$V = 2\pi \int_a^b (\text{radius})(\text{height}) , dx$
Radius $= x - (-1) = x+1$. Height $= e^{-x^2}$.
$$V = 2\pi \int_0^1 (x+1)e^{-x^2} , dx = 2\pi \left[ \int_0^1 xe^{-x^2} dx + \int_0^1 e^{-x^2} dx \right]$$
The second part is non-elementary, so this would be a calculator-active question on the AP exam.
Find the length of $x = \frac{1}{3}(y^2 + 2)^{3/2}$ from $y=0$ to $y=1$.
Solution:
$\frac{dx}{dy} = \frac{1}{3} \cdot \frac{3}{2}(y^2 + 2)^{1/2} \cdot 2y = y\sqrt{y^2 + 2}$.
$$L = \int_0^1 \sqrt{1 + (y\sqrt{y^2+2})^2} , dy = \int_0^1 \sqrt{1 + y^2(y^2+2)} , dy$$
$$= \int_0^1 \sqrt{1 + y^4 + 2y^2} , dy = \int_0^1 \sqrt{(y^2+1)^2} , dy = \int_0^1 (y^2+1) , dy$$
$$L = [\frac{y^3}{3} + y]_0^1 = 1/3 + 1 = 4/3$$
Find the area of the inner loop of $r = 1 - 2 \sin \theta$.
Solution:
The inner loop exists when $r < 0$. $1 - 2 \sin \theta = 0 \implies \sin \theta = 1/2$.
$\theta = \pi/6$ and $5\pi/6$.
$$\text{Area} = \frac{1}{2} \int_{\pi/6}^{5\pi/6} (1 - 2\sin \theta)^2 , d\theta = \frac{1}{2} \int_{\pi/6}^{5\pi/6} (1 - 4\sin \theta + 4\sin^2 \theta) , d\theta$$
$$= \frac{1}{2} \int_{\pi/6}^{5\pi/6} (1 - 4\sin \theta + 2 - 2\cos 2\theta) , d\theta = \frac{1}{2} \int_{\pi/6}^{5\pi/6} (3 - 4\sin \theta - 2\cos 2\theta) , d\theta$$
$$= \frac{1}{2} [3\theta + 4\cos \theta - \sin 2\theta]_{\pi/6}^{5\pi/6} = \pi - \frac{3\sqrt{3}}{2}$$
Find the average value of $f(x) = \sin^2 x$ on $[0, \pi]$.
Solution:
$$f_{avg} = \frac{1}{\pi} \int_0^\pi \sin^2 x , dx = \frac{1}{\pi} \int_0^\pi \frac{1-\cos 2x}{2} , dx$$
$$= \frac{1}{2\pi} [x - \frac{1}{2}\sin 2x]_0^\pi = \frac{1}{2\pi} (\pi - 0) = 1/2$$
Base is the region between $y=x^2$ and $y=1$. Cross sections perpendicular to the $y$-axis are isosceles right triangles with the hypotenuse in the base.
Solution:
Bounds for $y$: $0$ to $1$. Base length $s$ of the triangle is the width of the region at $y$.
$x = \pm \sqrt{y} \implies s = 2\sqrt{y}$.
Area of isosceles right triangle with hypotenuse $s$: $A(y) = \frac{1}{4}s^2$.
$$A(y) = \frac{1}{4}(2\sqrt{y})^2 = \frac{1}{4}(4y) = y$$
$$V = \int_0^1 y , dy = [\frac{y^2}{2}]_0^1 = 1/2$$
$a(t) = \cos t, v(0) = 5, s(0) = 0$. Find $s(\pi)$.
Solution:
$v(t) = \int a(t) , dt = \sin t + C$. Since $v(0)=5$, $0+C=5 \implies v(t) = \sin t + 5$.
$s(t) = \int v(t) , dt = -\cos t + 5t + C_2$. Since $s(0)=0$, $-1 + 0 + C_2 = 0 \implies C_2 = 1$.
$s(t) = -\cos t + 5t + 1$.
$s(\pi) = -(-1) + 5\pi + 1 = 5\pi + 2$.
Population growth rate is $P'(t) = 400 + 60\sqrt{t}$ people/year. Find the increase in population from year 4 to year 9.
Solution:
$$\Delta P = \int_4^9 (400 + 60t^{1/2}) , dt = [400t + 40t^{3/2}]_4^9$$
$$= (3600 + 40 \cdot 27) - (1600 + 40 \cdot 8) = (3600 + 1080) - (1600 + 320) = 4680 - 1920 = 2760$$
A solid has a base bounded by $f(x)$ and $g(x)$. If the cross-sections are any shape with area $k[s(x)]^n$, show the volume formula.
Solution:
$s(x) = f(x) - g(x)$.
$V = \int_a^b k[f(x) - g(x)]^n , dx$.
For squares, $k=1, n=2$. For semicircles, $k=\pi/8, n=2$. This demonstrates that the geometry of the cross-section is simply a constant multiplier if the area is proportional to the square of the base.
A pipe leaks oil at $R(t) = \frac{10}{t+1}$ gal/hr. How much oil leaks during the first 10 hours?
Solution:
$$\int_0^{10} \frac{10}{t+1} , dt = 10 [\ln|t+1|]_0^{10} = 10(\ln 11 - \ln 1) = 10 \ln 11 \approx 23.98 \text{ gal.}$$
Region bounded by $y = \ln x$, $y=0$, $x=e$. Rotate about the line $x=-2$.
Solution:
Since the axis is vertical, integrate $dy$. $y = \ln x \implies x = e^y$.
Bounds for $y$: $0$ to $1$.
$R_{out} = \text{distance from } x=-2 \text{ to } x=e \implies e - (-2) = e+2$.
$r_{in} = \text{distance from } x=-2 \text{ to } x=e^y \implies e^y - (-2) = e^y + 2$.
$$V = \pi \int_0^1 [(e+2)^2 - (e^y+2)^2] , dy = \pi \int_0^1 (e^2 + 4e + 4 - (e^{2y} + 4e^y + 4)) , dy$$
$$= \pi \int_0^1 (e^2 + 4e - e^{2y} - 4e^y) , dy = \pi [ (e^2+4e)y - \frac{1}{2}e^{2y} - 4e^y ]_0^1$$
$$= \pi [(e^2+4e - \frac{1}{2}e^2 - 4e) - (0 - 1/2 - 4)] = \pi [ \frac{1}{2}e^2 + 4.5 ]$$
Find the area of one petal of $r = \cos 3\theta$.
Solution:
One petal is traced as $r$ goes from $0$ to max and back to $0$.
$\cos 3\theta = 0 \implies 3\theta = -\pi/2, \pi/2 \implies \theta = -\pi/6, \pi/6$.
$$\text{Area} = \frac{1}{2} \int_{-\pi/6}^{\pi/6} \cos^2(3\theta) , d\theta = \frac{1}{2} \int_{-\pi/6}^{\pi/6} \frac{1 + \cos 6\theta}{2} , d\theta$$
$$= \frac{1}{4} [\theta + \frac{1}{6}\sin 6\theta]_{-\pi/6}^{\pi/6} = \frac{1}{4} [(\pi/6 + 0) - (-\pi/6 + 0)] = \frac{\pi}{12}$$
Show that the area under $f(x)$ from $a$ to $b$ plus the area under $f^{-1}(x)$ from $f(a)$ to $f(b)$ is $b \cdot f(b) - a \cdot f(a)$.
Solution:
Let $y = f(x)$, so $x = f^{-1}(y)$ and $dy = f'(x)dx$.
Area 2 $= \int_{f(a)}^{f(b)} f^{-1}(y) , dy = \int_a^b x f'(x) , dx$.
Using integration by parts: $u=x, dv=f'(x)dx \implies du=dx, v=f(x)$.
$\int_a^b x f'(x) , dx = [x f(x)]_a^b - \int_a^b f(x) , dx$.
Therefore, $\int_a^b f(x) , dx + \text{Area 2} = b f(b) - a f(a)$.
Find the surface area of the solid generated by rotating $y = x^3$ from $0 \le x \le 1$ about the $x$-axis.
Solution:
Formula: $S = \int 2\pi y , ds = \int_0^1 2\pi x^3 \sqrt{1 + (3x^2)^2} , dx$.
$$S = 2\pi \int_0^1 x^3 \sqrt{1 + 9x^4} , dx$$
Let $u = 1+9x^4, du=36x^3 dx$.
$$S = 2\pi \cdot \frac{1}{36} \int_1^{10} u^{1/2} , du = \frac{\pi}{18} [\frac{2}{3}u^{3/2}]_1^{10} = \frac{\pi}{27}(10\sqrt{10} - 1)$$
Derive the volume of a sphere of radius $R$ using calculus.
Solution:
Rotate the semicircle $y = \sqrt{R^2 - x^2}$ from $x = -R$ to $x = R$ about the $x$-axis.
Using the Disk Method:
$$V = \pi \int_{-R}^R (\sqrt{R^2 - x^2})^2 , dx = \pi \int_{-R}^R (R^2 - x^2) , dx$$
$$V = \pi [R^2x - \frac{x^3}{3}]_{-R}^R = \pi [(R^3 - R^3/3) - (-R^3 + R^3/3)]$$
$$V = \pi [2R^3/3 - (-2R^3/3)] = \frac{4}{3}\pi R^3$$
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