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Applications of the definite integral

  1. The area under a graph Γf{{\Gamma }_{f}}, f:[a,b]→R+,f continu  ⁣ ⁣a˘ ⁣ ⁣f:[a,b]\to {{\mathbb{R}}_{+}}, f\text{ continu }\!\!\breve{\mathrm{a}}\!\!

Γf=∫ab∣f(x)∣dx\displaystyle {{\Gamma }_{f}}=\int\limits_{a}^{b}{\left| f(x) \right|} dx

The area between the graphs of two continuous functions f,g:[a,b]→Rf,g:[a,b]\to \mathbb{R} is:

Γf,g=∑k=1n[f(a+kb−an)−g(a+kb−an)]⋅b−an\displaystyle {{\Gamma }_{f,g}}=\sum\limits_{k=1}^{n}{\left[ f\left( a+k\frac{b-a}{n} \right)-g\left( a+k\frac{b-a}{n} \right) \right]}\cdot \frac{b-a}{n}

Γf,g=∫ab∣f(x)−g(x)∣dx\displaystyle {{\Gamma }_{f,g}}=\int\limits_{a}^{b}{\left| f(x)-g(x) \right|} dx

The region between the two graphs is the set of points:

Γ={(x,y)∈R2∣a≤x≤b i g(x)≤y≤f(x)}\Gamma =\{(x,y)\in {{\mathbb{R}}^{2}}|a\le x\le b\text{ i }g(x)\le y\le f(x)\}

The area of the region lying between the graphs of the functions

f(x)=xf(x)=x and g(x)=x2g(x)={{x}^{2}}

The area of the region lying between the graphs of the functions

f(x)=x2f(x)={{x}^{2}} and g(x)=x3g(x)={{x}^{3}}

|:--:| | sin⁡(x)\sin (x) | | The region enclosed between the graphs of the functions sin⁡(x)\sin (x) and cos⁡(x)co\operatorname{s}(x) |

|:--:|

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| | The region enclosed between the graphs of the functions and x3\sqrt[3]{x} |

  1. Arc length of a graph

Let f:[a,b]→Rf:[a,b]\to \mathbb{R} be a differentiable function with continuous derivative. The length of the graph of ff is:

l=∫ab1+(f′(x))2dx\displaystyle l=\int_{a}^{b}{\sqrt{1+{{({f}'(x))}^{2}}}}dx

  1. Area of a surface of revolution

Let f:[a,b]→Rf:[a,b]\to \mathbb{R} be a continuous function. The set of points in space:

S={(x,y,z)∈R3∣y2+z2=f(x),x∈[a,b]}S=\{(x,y,z)\in {{\mathbb{R}}^{3}}|\sqrt{{{y}^{2}}+{{z}^{2}}}=f(x),x\in [a,b]\}

is called the surface of revolution determined by the function ff about the OxOx axis.

Let f:[a,b]→Rf:[a,b]\to \mathbb{R} be a differentiable function with continuous derivative. The surface of revolution determined by ff has area:

A(f)=2π∫abf(x)⋅1+(f′(x))2dx\displaystyle A(f)=2\pi \int_{a}^{b}{f(x)\cdot \sqrt{1+{{({f}'(x))}^{2}}}}dx

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The surface of revolution of the function x\sqrt{x} on the interval [0,9][0,9]

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The surface of revolution of the function cos(x) on the interval [0,2π][0,2\pi ]

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The surface of revolution of the function sin(x) on the interval [0,2π][0,2\pi ]

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The surface of revolution of the function x⋅sin⁡(x)x\cdot \sin (x) on the interval [0,2π][0,2\pi ]

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The surface of revolution of the function x2{{x}^{2}} on the interval [−2,4][-2,4]

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The surface of revolution of the function x3−x2{{x}^{3}}-{{x}^{2}} on the interval [−1,2][-1,2]

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  1. Volume of a solid of revolution

Let f:[a,b]→Rf:[a,b]\to \mathbb{R} be a continuous function. The set of points in space:

V={(x,y,z)∈R3∣y2+z2≤∣f(x)∣,x∈[a,b]}V=\{(x,y,z)\in {{\mathbb{R}}^{3}}|\sqrt{{{y}^{2}}+{{z}^{2}}}\le \left| f(x) \right|,x\in [a,b]\}

is called the solid of revolution determined by the function ff about the OxOx axis.

Let f:[a,b]→Rf:[a,b]\to \mathbb{R} be a differentiable function with continuous derivative. The solid of revolution determined by ff has volume:

V(f)=π∫abf2(x)dx\displaystyle V(f)=\pi \int_{a}^{b}{{{f}^{2}}(x)}dx

  1. Centre of mass

Let EE be a plane lamina bounded by the continuous functions f,g:[a,b]→R.f,g:[a,b]\to \mathbb{R}. The centre of mass of EE is the point with coordinates:

xG=∫abx(g(x)−f(x))dx∫ab(g(x)−f(x))dx\displaystyle {{x}_{G}}=\tfrac{\int\limits_{a}^{b}{x(g(x)-f(x))dx}}{\int\limits_{a}^{b}{(g(x)-f(x))dx}}, yG=12⋅∫ab(g2(x)−f2(x))dx∫ab(g(x)−f(x))dx\displaystyle {{y}_{G}}=\tfrac{\frac{1}{2}\cdot \int\limits_{a}^{b}{({{g}^{2}}(x)-{{f}^{2}}(x))dx}}{\int\limits_{a}^{b}{(g(x)-f(x))dx}}