Skip to main content
Contents
Embed
Dark Mode Prev Up Next
\(\require{physics}\require{upgreek}\everymath{\displaystyle}
\newcommand{\N}{\mathbb N}
\newcommand{\Z}{\mathbb Z}
\newcommand{\Q}{\mathbb Q}
\newcommand{\R}{\mathbb R}
\newcommand{\inv}{^{-1}}
\newcommand{\DS}{\displaystyle}
\newcommand{\eps}{\varepsilon}
\newcommand{\tsub}[1]{_{\mathrm{#1}}}
\newcommand{\ee}{\mathrm{e}}
\newcommand{\ii}{\mathrm{i}}
\newcommand{\limit}[1]{\lim\limits_{#1}}
\newcommand{\resid}[1]{\underset{#1}{\Res}}
\DeclareMathOperator{\sinc}{sinc}
\DeclareMathOperator{\sgn}{sgn}
\newcommand{\pii}{\pi}
\DeclareMathOperator{\Prob}{P}
\DeclareMathOperator{\EV}{E}
\DeclareMathOperator{\Var}{Var}
\newcommand{\bv}[1]{\boldsymbol{#1}}
\newcommand{\uv}[1]{\hat{\bv{#1}}}
\newcommand{\cl}[1]{\mathcal{#1}}
\newcommand{\bb}[1]{\mathbb{#1}}
\DeclareMathOperator{\Cis}{cis}
\DeclareMathOperator{\RE}{Re}
\DeclareMathOperator{\IM}{Im}
\newcommand{\xd}{\mathbf{d}}
\newcommand{\seq}[3]{{#1}_{#2},\cdots,{#1}_{#3}}
\newcommand{\psup}[1]{^{(#1)}}
\newcommand{\hypext}{{}^*}
\DeclareMathOperator{\st}{st}
\newcommand{\set}[1]{\left\{#1\right\}}
\DeclareMathOperator{\Sin}{Sin}
\DeclareMathOperator{\Cos}{Cos}
\DeclareMathOperator{\Tan}{Tan}
\DeclareMathOperator{\Sec}{Sec}
\DeclareMathOperator{\Csc}{Csc}
\DeclareMathOperator{\Cot}{Cot}
\DeclareMathOperator{\Log}{Log}
\DeclareMathOperator{\Arg}{Arg}
\DeclareMathOperator{\Ln}{Ln}
\DeclareMathOperator{\Grad}{grad}
\DeclareMathOperator{\Div}{div}
\DeclareMathOperator{\Curl}{curl}
\newcommand{\rd}{\textstyle\mathop{}\!\mathrm{d}^{\!\!\!-}\hspace{-0.0555 em}}
\newcommand{\rpd}{\textstyle\mathop{}\!\partial^{\hspace{-0.5 em}-}\hspace{-0.1666 em}}
\newcommand{\rdv}[2]{\frac{\rd{#1}}{\rd{#2}}}
\newcommand{\rpdv}[2]{\frac{\rpd{#1}}{\rpd{#2}}}
\newcommand{\lt}{<}
\newcommand{\gt}{>}
\newcommand{\amp}{&}
\definecolor{fillinmathshade}{gray}{0.9}
\newcommand{\fillinmath}[1]{\mathchoice{\colorbox{fillinmathshade}{$\displaystyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\textstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptscriptstyle\phantom{\,#1\,}$}}}
\)
Section 15.2 Double integrals over general regions
Objectives
Handle irregular regions by extending the integrand to a surrounding rectangle.
Set up iterated integrals by describing the region with inequalities bounding one variable in terms of the other.
Reverse the order of integration to simplify difficult integrals.
Can use a ‘bounding box’ approach to take double integrals over regions with more general regions. If \(D\) is a region over which \(f\) is defined, let \(R\) be a rectangle containing \(D\text{,}\) and let
\begin{equation*}
F(x,y)=\begin{cases}f(x,y) \amp \text{if }(x,y)\in D\\ 0 \amp \text{if }(x,y)\in R\setminus D\end{cases}
\end{equation*}
Then \(\DS\iint_{D} f(x,y)\dd{A}=\iint_{R} F(x,y)\dd{A}\text{.}\)
If \(D\) is bounded below by \(y=g(x)\) and above by \(y=h(x)\text{:}\)
\begin{equation*}
\iint_{D} f(x,y)\dd{A}=\int_{x=a}^{x=b}\int_{y=g(x)}^{y=h(x)}f(x,y)\dd{y}\dd{x}
\end{equation*}
If \(D\) is bounded on the left by \(x=g(y)\) and the right by \(x=h(y)\text{:}\)
\begin{equation*}
\iint_{D} f(x,y)\dd{A}=\int_{y=c}^{y=d}\int_{x=g(y)}^{x=h(y)}f(x,y)\dd{x}\dd{y}
\end{equation*}
Changing order of integration:
\begin{equation*}
\int_{x=0}^{x=1}\int_{y=x}^{y=1}\sin(y^{2})\dd{y}\dd{x}=\int_{y=0}^{y=1}\int_{x=0}^{x=y}\sin(y^{2})\dd{x}\dd{y}
\end{equation*}