Difference between revisions of "Integration by Parts"
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::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{f(x)g(x)} & = & \displaystyle{\int f'(x)g(x)+f(x)g'(x)~dx}\\ | + | \displaystyle{f(x)g(x)} & = & \displaystyle{\int (f(x)g(x))'~dx}\\ |
| + | &&\\ | ||
| + | & = & \displaystyle{\int f'(x)g(x)+f(x)g'(x)~dx}\\ | ||
&&\\ | &&\\ | ||
& = & \displaystyle{\int f'(x)g(x)~dx+\int f(x)g'(x)~dx.} | & = & \displaystyle{\int f'(x)g(x)~dx+\int f(x)g'(x)~dx.} | ||
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Evaluate the following integrals. | Evaluate the following integrals. | ||
| − | '''1)''' <math style="vertical-align: - | + | '''1)''' <math style="vertical-align: -13px">\int xe^x~dx</math> |
{| class = "mw-collapsible mw-collapsed" style = "text-align:left;" | {| class = "mw-collapsible mw-collapsed" style = "text-align:left;" | ||
!Solution: | !Solution: | ||
|- | |- | ||
| − | | | + | |We have two options when doing integration by parts. |
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
|- | |- | ||
| − | | | + | |We can let <math style="vertical-align: 0px">u=x</math> or <math style="vertical-align: 0px">u=e^x.</math> |
| − | |||
|- | |- | ||
| + | |In this case, we let <math style="vertical-align: 0px">u</math> be the polynomial. | ||
|- | |- | ||
| − | |<u> | + | |So, we let <math style="vertical-align: 0px">u=x</math> and <math style="vertical-align: 0px">dv=e^x~dx.</math> |
|- | |- | ||
| − | | | + | |Then, <math style="vertical-align: 0px">du=dx</math> and <math style="vertical-align: 0px">v=e^x.</math> |
|- | |- | ||
| − | | | + | |Hence, by integration by parts, we get |
|- | |- | ||
| | | | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int xe^x~dx} & = & \displaystyle{xe^x-\int e^x~dx}\\ |
| − | |||
| − | & = & \displaystyle{ | ||
| − | |||
| − | |||
&&\\ | &&\\ | ||
| − | & = & \displaystyle{x^ | + | & = & \displaystyle{xe^x-e^x+C.} |
\end{array}</math> | \end{array}</math> | ||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
|} | |} | ||
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!Final Answer: | !Final Answer: | ||
|- | |- | ||
| − | | <math> | + | | <math>xe^x-e^x+C</math> |
| − | |||
| − | |||
| − | |||
| − | |||
|} | |} | ||
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|- | |- | ||
| | | | ||
| − | + | We have a choice to make. | |
|- | |- | ||
| − | | | + | |We can let <math style="vertical-align: 0px">u=x</math> or <math style="vertical-align: -5px">u=\cos(2x).</math> |
| − | + | |- | |
| + | |In this case, we let <math style="vertical-align: 0px">u</math> be the polynomial. | ||
|- | |- | ||
| − | | | + | |So, we let <math style="vertical-align: 0px">u=x</math> and <math style="vertical-align: -5px">dv=\cos(2x)~dx.</math> |
|- | |- | ||
| − | | | + | |Then, <math style="vertical-align: 0px">du=dx.</math> |
| − | |||
|- | |- | ||
| − | |< | + | |To find <math style="vertical-align: -4px">v,</math> we need to use <math style="vertical-align: 0px">u-</math>substitution. So, |
|- | |- | ||
| − | | | + | | |
| + | ::<math style="vertical-align: -13px">v=\int \cos(2x)~dx=\frac{1}{2} \sin(2x).</math> | ||
|- | |- | ||
| − | | | + | |Hence, by integration by parts, we get |
|- | |- | ||
| | | | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int x\cos(2x)~dx} & = & \displaystyle{\frac{1}{2}x\sin(2x)-\int \frac{1}{2}\sin(2x)~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{ | + | & = & \displaystyle{\frac{1}{2}x\sin(2x)+\frac{1}{4}\cos(2x)+C,} |
| − | |||
| − | |||
\end{array}</math> | \end{array}</math> | ||
|- | |- | ||
| − | | | + | |where we use <math style="vertical-align: 0px">u-</math> substitution to evaluate the last integral. |
| − | |||
| − | |||
| − | : | ||
|} | |} | ||
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!Final Answer: | !Final Answer: | ||
|- | |- | ||
| − | + | | <math>\frac{1}{2}x\sin(2x)+\frac{1}{4}\cos(2x)+C</math> | |
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
|} | |} | ||
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!Solution: | !Solution: | ||
|- | |- | ||
| − | | | + | |We have a choice to make. |
| + | |- | ||
| + | |We can let <math style="vertical-align: -1px">u=\ln x</math> or <math style="vertical-align: -1px">dv=\ln x~dx.</math> | ||
| + | |- | ||
| + | |In this case, we don't want to let <math style="vertical-align: -1px">dv=\ln x~dx</math> since we don't know how to integrate <math style="vertical-align: -1px">\ln x</math> yet. | ||
| + | |- | ||
| + | |So, we let <math style="vertical-align: -1px">u=\ln x</math> and <math style="vertical-align: -1px">dv=1~dx.</math> | ||
| + | |- | ||
| + | |Then, <math style="vertical-align: -13px">du=\frac{1}{x}~dx</math> and <math style="vertical-align: 0px">v=x.</math> | ||
| + | |- | ||
| + | |Hence, by integration by parts, we get | ||
|- | |- | ||
| | | | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int \ln x~dx} & = & \displaystyle{x\ln (x) -\int x \bigg(\frac{1}{x}\bigg)~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\ | + | & = & \displaystyle{x\ln (x)-\int 1~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{ | + | & = & \displaystyle{x\ln (x)-x+C.} |
| − | |||
| − | |||
| − | |||
| − | |||
\end{array}</math> | \end{array}</math> | ||
|- | |- | ||
| − | | | + | |<u>Note:</u> The domain of the function <math style="vertical-align: -1px">\ln x</math> is <math style="vertical-align: -5px">(0,\infty).</math> |
|- | |- | ||
| − | | | + | |So, this integral is defined for <math style="vertical-align: 0px">x>0.</math> |
| − | |||
| − | |||
| − | |||
|} | |} | ||
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!Final Answer: | !Final Answer: | ||
|- | |- | ||
| − | | <math> | + | | <math>x\ln (x)-x+C</math> |
|- | |- | ||
|} | |} | ||
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== Exercise 1 == | == Exercise 1 == | ||
| − | Evaluate <math style="vertical-align: -13px">\int x^ | + | Evaluate <math style="vertical-align: -13px">\int x \sec^2 x~dx.</math> |
| + | |||
| + | Since we know the antiderivative of <math style="vertical-align: -3px">\sec^2 x,</math> | ||
| − | + | we let <math style="vertical-align: 0px">u=x</math> and <math style="vertical-align: 0px">dv=\sec^2 x~dx.</math> | |
| − | : | + | Then, <math style="vertical-align: 0px">du=dx</math> and <math style="vertical-align: -1px">v=\tan x.</math> |
| − | + | Using integration by parts, we get | |
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{\ | + | \displaystyle{\int x \sec^2 x~dx} & = & \displaystyle{x\tan x -\int \tan x~dx}\\ |
| − | |||
| − | |||
| − | |||
| − | & = & \displaystyle{ | ||
| − | |||
| − | |||
&&\\ | &&\\ | ||
| − | & = & \displaystyle{-\ | + | & = & \displaystyle{x\tan x -\int \frac{\sin x}{\cos x}~dx.} |
\end{array}</math> | \end{array}</math> | ||
| − | + | For the remaining integral, we use <math style="vertical-align: 0px">u-</math>substitution. | |
| + | |||
| + | Let <math style="vertical-align: 0px">u=\cos x.</math> Then, <math style="vertical-align: -1px">du=-\sin x~dx.</math> | ||
| + | |||
| + | So, we get | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int x \sec^2 x~dx} & = & \displaystyle{x\tan x +\int \frac{1}{u}~du}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle | + | & = & \displaystyle{x\tan x + \ln |u|+C}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{ | + | & = & \displaystyle{x\tan x+ \ln |\cos x|+C.} |
\end{array}</math> | \end{array}</math> | ||
So, we have | So, we have | ||
| − | ::<math> | + | ::<math>\int x \sec^2 x~dx=x\tan x+ \ln |\cos x|+C.</math> |
== Exercise 2 == | == Exercise 2 == | ||
| − | Evaluate <math style="vertical-align: - | + | Evaluate <math style="vertical-align: -13px">\int \frac{\ln x}{x^3}~dx.</math> |
| − | + | We start by letting <math style="vertical-align: -1px">u=\ln x</math> and <math style="vertical-align: -13px">dv=\frac{1}{x^3}~dx.</math> | |
| − | + | Then, <math style="vertical-align: -13px">du=\frac{1}{x}~dx</math> and <math style="vertical-align: -13px">v=-\frac{1}{2x^2}.</math> | |
| − | + | So, using integration by parts, we get | |
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int \frac{\ln x}{x^3}~dx} & = & \displaystyle{-\frac{\ln x}{2x^2}-\int -\frac{1}{2x^2}\bigg(\frac{1}{x}\bigg)~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{ | + | & = & \displaystyle{-\frac{\ln x}{2x^2}+\int \frac{1}{2x^3}~dx}\\ |
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | \ | ||
&&\\ | &&\\ | ||
| − | & = & \displaystyle{ | + | & = & \displaystyle{-\frac{\ln x}{2x^2}-\frac{1}{4x^2}+C.} |
\end{array}</math> | \end{array}</math> | ||
So, we have | So, we have | ||
| − | |||
| − | + | ::<math>\int \frac{\ln x}{x^3}~dx=-\frac{\ln x}{2x^2}-\frac{1}{4x^2}+C.</math> | |
| − | + | == Exercise 3 == | |
| − | + | Evaluate <math style="vertical-align: -13px">\int x\sqrt{x+1}~dx.</math> | |
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | + | We start by letting <math style="vertical-align: 0px">u=x</math> and <math style="vertical-align: -3px">dv=\sqrt{x+1}~dx.</math> | |
| − | |||
| − | == | ||
| − | + | Then, <math style="vertical-align: 0px">du=dx.</math> | |
| − | + | To find <math style="vertical-align: -4px">v,</math> we need to use <math style="vertical-align: 0px">u-</math>substitution. So, | |
| − | ::<math> | + | ::<math style="vertical-align: 0px">v=\int \sqrt{x+1}~dx=\frac{2}{3}(x+1)^{\frac{3}{2}}.</math> |
| − | + | Hence, by integration by parts, we get | |
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int x\sqrt{x+1}~dx} & = & \displaystyle{\frac{2}{3}x(x+1)^{\frac{3}{2}}-\int \frac{2}{3}(x+1)^{\frac{3}{2}}~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{ | + | & = & \displaystyle{\frac{2}{3}x(x+1)^{\frac{3}{2}}-\frac{4}{15}(x+1)^{\frac{5}{2}}+C,} |
\end{array}</math> | \end{array}</math> | ||
| − | So, we | + | where we use <math style="vertical-align: 0px">u-</math> substitution to evaluate the last integral. |
| − | ::<math> | + | |
| + | So, we have | ||
| + | |||
| + | ::<math>\int x\sqrt{x+1}~dx=\frac{2}{3}x(x+1)^{\frac{3}{2}}-\frac{4}{15}(x+1)^{\frac{5}{2}}+C.</math> | ||
== Exercise 4 == | == Exercise 4 == | ||
| − | Evaluate <math style="vertical-align: - | + | Evaluate <math style="vertical-align: -13px">\int x^2e^{-2x}~dx.</math> |
| + | |||
| + | We start by letting <math style="vertical-align: 0px">u=x^2</math> and <math style="vertical-align: 0px">dv=e^{-2x}~dx.</math> | ||
| − | + | Then, <math style="vertical-align: 0px">du=2x~dx.</math> | |
| + | |||
| + | To find <math style="vertical-align: -4px">v,</math> we need to use <math style="vertical-align: 0px">u-</math>substitution. So, | ||
| + | |||
| + | ::<math style="vertical-align: 0px">v=\int e^{-2x}~dx=\frac{e^{-2x}}{-2}.</math> | ||
| + | |||
| + | Hence, by integration by parts, we get | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int x^2 e^{-2x}~dx} & = & \displaystyle{\frac{x^2e^{-2x}}{-2}-\int 2x\bigg(\frac{e^{-2x}}{-2}\bigg)~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{x^ | + | & = & \displaystyle{\frac{x^2e^{-2x}}{-2}+\int xe^{-2x}~dx.} |
\end{array}</math> | \end{array}</math> | ||
| − | Now, we need to use | + | Now, we need to use integration by parts a second time. |
| + | |||
| + | Let <math style="vertical-align: 0px">u=x</math> and <math style="vertical-align: 0px">dv=e^{-2x}~dx.</math> | ||
| + | |||
| + | Then, <math style="vertical-align: 0px">du=dx</math> and <math style="vertical-align: -13px">v=\frac{e^{-2x}}{-2}.</math> | ||
| + | |||
| + | Therefore, using integration by parts again, we get | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int x^2 e^{-2x}~dx} & = & \displaystyle{\frac{x^2 e^{-2x} }{-2}+\frac{x e^{-2x} }{-2}-\int \frac{e^{-2x}}{-2}~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{x^2\ | + | & = & \displaystyle{\frac{x^2e^{-2x}}{-2}+\frac{xe^{-2x}}{-2}+\frac{e^{-2x}}{-4}+C.} |
\end{array}</math> | \end{array}</math> | ||
So, we have | So, we have | ||
| − | ::<math> | + | ::<math>\int x^2e^{-2x}~dx=\frac{x^2e^{-2x}}{-2}+\frac{xe^{-2x}}{-2}+\frac{e^{-2x}}{-4}+C.</math> |
== Exercise 5 == | == Exercise 5 == | ||
| − | Evaluate <math style="vertical-align: - | + | Evaluate <math style="vertical-align: -13px">\int e^{3x}\sin(2x)~dx.</math> |
| − | + | We begin by letting <math style="vertical-align: -6px">u=\sin(2x)</math> and <math style="vertical-align: 0px">dv=e^{3x}~dx.</math> | |
| + | |||
| + | Then, <math style="vertical-align: -5px">du=2\cos (2x)~dx.</math> | ||
| + | |||
| + | To find <math style="vertical-align: -4px">v,</math> we need to use <math style="vertical-align: 0px">u-</math>substitution. So, | ||
| + | |||
| + | ::<math style="vertical-align: 0px">v=\int e^{3x}~dx=\frac{e^{3x}}{3}.</math> | ||
| + | |||
| + | Hence, by integration by parts, we have | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int e^{3x} \sin(2x)~dx} & = & \displaystyle{\frac{e^{3x}\sin(2x)}{3}-\int \frac{2}{3}\cos(2x)e^{3x}~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{ | + | & = & \displaystyle{\frac{e^{3x}\sin(2x)}{3}-\frac{2}{3} \int \cos(2x)e^{3x}~dx.} |
\end{array}</math> | \end{array}</math> | ||
| − | Now, we need to use | + | Now, we need to use integration by parts a second time. |
| + | |||
| + | Let <math style="vertical-align: -5px">u=\cos (2x)</math> and <math style="vertical-align: 0px">dv=e^{3x}~dx.</math> | ||
| + | |||
| + | Then, <math style="vertical-align: -5px">du=-2\sin(2x)~dx</math> and <math style="vertical-align: -13px">v=\frac{e^{3x}}{3}.</math> | ||
| + | |||
| + | Therefore, using integration by parts again, we get | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int e^{3x} \sin(2x)~dx} & = & \displaystyle{\frac{e^{3x}\sin(2x)}{3}-\frac{2}{3} \bigg[ \frac{\cos(2x)e^{3x}}{3}+\int \frac{2}{3}\sin(2x)e^{3x}~dx\bigg]}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{ | + | & = & \displaystyle{\frac{e^{3x}\sin(2x)}{3}-\frac{2\cos(2x)e^{3x}}{9}-\frac{4}{9}\int e^{3x}\sin(2x)~dx.} |
\end{array}</math> | \end{array}</math> | ||
| − | So, we | + | Now, we have the exact same integral that we had at the beginning of the problem. |
| − | ::<math> | + | |
| + | So, we add this integral to the other side of the equation. | ||
| + | |||
| + | When we do this, we get | ||
| + | |||
| + | ::<math>\frac{13}{9} \int e^{3x}\sin(2x)~dx = \frac{e^{3x}\sin(2x)}{3}-\frac{2\cos(2x)e^{3x}}{9}.</math> | ||
| + | |||
| + | Therefore, we get | ||
| + | |||
| + | ::<math> \int e^{3x}\sin(2x)~dx = \frac{9}{13}\bigg(\frac{e^{3x}\sin(2x)}{3}-\frac{2\cos(2x)e^{3x}}{9}\bigg)+C.</math> | ||
== Exercise 6 == | == Exercise 6 == | ||
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Evaluate <math style="vertical-align: -14px">\int \sin(2x)\cos(3x)~dx.</math> | Evaluate <math style="vertical-align: -14px">\int \sin(2x)\cos(3x)~dx.</math> | ||
| − | + | For this problem, we use a similar process as Exercise 5. | |
| + | |||
| + | We use integration by parts twice, which produces the same integral given to us in the problem. | ||
| + | |||
| + | Then, we solve for our integral. | ||
| + | |||
| + | We begin by letting <math style="vertical-align: -5px">u=\sin(2x)</math> and <math style="vertical-align: -5px">dv=\cos(3x)~dx.</math> | ||
| + | |||
| + | Then, <math style="vertical-align: -5px">du=2\cos (2x)~dx.</math> | ||
| + | |||
| + | To find <math style="vertical-align: -4px">v,</math> we need to use <math style="vertical-align: 0px">u-</math>substitution. So, | ||
| + | |||
| + | ::<math style="vertical-align: 0px">v=\int \cos(3x)~dx=\frac{1}{3}\sin(3x).</math> | ||
| + | |||
| + | Hence, by integration by parts, we have | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int \sin(2x)\cos(3x)~dx} & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)-\int \frac{2}{3}\cos(2x)\sin(3x)~dx}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{ | + | & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)-\frac{2}{3} \int \cos(2x)\sin(3x)~dx.} |
\end{array}</math> | \end{array}</math> | ||
| − | Now, we need to use | + | Now, we need to use integration by parts a second time. |
| + | |||
| + | Let <math style="vertical-align: -5px">u=\cos (2x)</math> and <math style="vertical-align: -5px">dv=\sin(3x)~dx.</math> | ||
| + | |||
| + | Then, <math style="vertical-align: -5px">du=-2\sin(2x)~dx</math> and <math style="vertical-align: -13px">v=\frac{-\cos(3x)}{3}.</math> | ||
| + | |||
| + | Therefore, using integration by parts again, we get | ||
::<math>\begin{array}{rcl} | ::<math>\begin{array}{rcl} | ||
| − | \displaystyle{ | + | \displaystyle{\int \sin(2x)\cos(3x)~dx} & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)-\frac{2}{3} \bigg[ \frac{-\cos(2x)\cos(3x)}{3}-\int \frac{2}{3}\sin(2x)\cos(3x)~dx\bigg]}\\ |
&&\\ | &&\\ | ||
| − | & = & \displaystyle{\frac{ | + | & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)+ \frac{2\cos(2x)\cos(3x)}{9}+\frac{4}{9}\int \sin(2x)\cos(3x)~dx.} |
\end{array}</math> | \end{array}</math> | ||
| − | So, we | + | Now, we have the exact same integral that we had at the beginning of the problem. |
| − | ::<math> | + | |
| + | So, we subtract this integral to the other side of the equation. | ||
| + | |||
| + | When we do this, we get | ||
| + | |||
| + | ::<math>\frac{5}{9} \int \sin(2x)\cos(3x)~dx = \frac{1}{3}\sin(2x)\sin(3x)+ \frac{2\cos(2x)\cos(3x)}{9}.</math> | ||
| + | |||
| + | Therefore, we get | ||
| + | |||
| + | ::<math> \int e^{3x}\sin(2x)~dx = \frac{9}{5}\bigg(\frac{1}{3}\sin(2x)\sin(3x)+ \frac{2\cos(2x)\cos(3x)}{9}\bigg)+C.</math> | ||
Latest revision as of 12:17, 30 October 2017
Introduction
Let's say we want to integrate
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int x^{2}e^{x^{3}}~dx.}
Here, we can compute this antiderivative by using Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u-} substitution.
While Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u-} substitution is an important integration technique, it will not help us evaluate all integrals.
For example, consider the integral
There is no substitution that will allow us to integrate this integral.
We need another integration technique called integration by parts.
The formula for integration by parts comes from the product rule for derivatives.
Recall from the product rule,
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle (f(x)g(x))'=f'(x)g(x)+f(x)g'(x).}
Then, we have
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {f(x)g(x)}&=&\displaystyle {\int (f(x)g(x))'~dx}\\&&\\&=&\displaystyle {\int f'(x)g(x)+f(x)g'(x)~dx}\\&&\\&=&\displaystyle {\int f'(x)g(x)~dx+\int f(x)g'(x)~dx.}\end{array}}}
If we solve the last equation for the second integral, we obtain
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int f(x)g'(x)~dx=f(x)g(x)-\int f'(x)g(x)~dx.}
This formula is the formula for integration by parts.
But, as it is currently stated, it is long and hard to remember.
So, we make a substitution to obtain a nicer formula.
Let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=f(x)} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=g'(x)~dx.}
Then, and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=g(x).}
Plugging these into our formula, we obtain
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int u~dv=uv-\int v~du.}
Warm-Up
Evaluate the following integrals.
1) Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int xe^{x}~dx}
| Solution: |
|---|
| We have two options when doing integration by parts. |
| We can let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=x} or Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=e^{x}.} |
| In this case, we let be the polynomial. |
| So, we let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=x} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=e^{x}~dx.} |
| Then, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle du=dx} and |
| Hence, by integration by parts, we get |
|
| Final Answer: |
|---|
| Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle xe^{x}-e^{x}+C} |
2) Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int x\cos(2x)~dx}
| Solution: |
|---|
|
We have a choice to make. |
| We can let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=x} or Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=\cos(2x).} |
| In this case, we let be the polynomial. |
| So, we let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=x} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=\cos(2x)~dx.} |
| Then, |
| To find Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v,} we need to use substitution. So, |
|
| Hence, by integration by parts, we get |
|
| where we use substitution to evaluate the last integral. |
| Final Answer: |
|---|
| Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\frac {1}{2}}x\sin(2x)+{\frac {1}{4}}\cos(2x)+C} |
3) Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int \ln x~dx}
| Solution: |
|---|
| We have a choice to make. |
| We can let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=\ln x} or Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=\ln x~dx.} |
| In this case, we don't want to let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=\ln x~dx} since we don't know how to integrate yet. |
| So, we let and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=1~dx.} |
| Then, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle du={\frac {1}{x}}~dx} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=x.} |
| Hence, by integration by parts, we get |
|
| Note: The domain of the function is Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle (0,\infty ).} |
| So, this integral is defined for |
| Final Answer: |
|---|
| Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle x\ln(x)-x+C} |
Exercise 1
Evaluate Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int x\sec ^{2}x~dx.}
Since we know the antiderivative of Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \sec ^{2}x,}
we let and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=\sec ^{2}x~dx.}
Then, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle du=dx} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=\tan x.}
Using integration by parts, we get
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {\int x\sec ^{2}x~dx}&=&\displaystyle {x\tan x-\int \tan x~dx}\\&&\\&=&\displaystyle {x\tan x-\int {\frac {\sin x}{\cos x}}~dx.}\end{array}}}
For the remaining integral, we use substitution.
Let Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=\cos x.} Then,
So, we get
So, we have
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int x\sec ^{2}x~dx=x\tan x+\ln |\cos x|+C.}
Exercise 2
Evaluate Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int {\frac {\ln x}{x^{3}}}~dx.}
We start by letting and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv={\frac {1}{x^{3}}}~dx.}
Then, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle du={\frac {1}{x}}~dx} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=-{\frac {1}{2x^{2}}}.}
So, using integration by parts, we get
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {\int {\frac {\ln x}{x^{3}}}~dx}&=&\displaystyle {-{\frac {\ln x}{2x^{2}}}-\int -{\frac {1}{2x^{2}}}{\bigg (}{\frac {1}{x}}{\bigg )}~dx}\\&&\\&=&\displaystyle {-{\frac {\ln x}{2x^{2}}}+\int {\frac {1}{2x^{3}}}~dx}\\&&\\&=&\displaystyle {-{\frac {\ln x}{2x^{2}}}-{\frac {1}{4x^{2}}}+C.}\end{array}}}
So, we have
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int {\frac {\ln x}{x^{3}}}~dx=-{\frac {\ln x}{2x^{2}}}-{\frac {1}{4x^{2}}}+C.}
Exercise 3
Evaluate
We start by letting and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv={\sqrt {x+1}}~dx.}
Then,
To find Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v,} we need to use substitution. So,
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=\int {\sqrt {x+1}}~dx={\frac {2}{3}}(x+1)^{\frac {3}{2}}.}
Hence, by integration by parts, we get
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {\int x{\sqrt {x+1}}~dx}&=&\displaystyle {{\frac {2}{3}}x(x+1)^{\frac {3}{2}}-\int {\frac {2}{3}}(x+1)^{\frac {3}{2}}~dx}\\&&\\&=&\displaystyle {{\frac {2}{3}}x(x+1)^{\frac {3}{2}}-{\frac {4}{15}}(x+1)^{\frac {5}{2}}+C,}\end{array}}}
where we use substitution to evaluate the last integral.
So, we have
Exercise 4
Evaluate Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int x^{2}e^{-2x}~dx.}
We start by letting Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=x^{2}} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=e^{-2x}~dx.}
Then,
To find Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v,} we need to use substitution. So,
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=\int e^{-2x}~dx={\frac {e^{-2x}}{-2}}.}
Hence, by integration by parts, we get
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {\int x^{2}e^{-2x}~dx}&=&\displaystyle {{\frac {x^{2}e^{-2x}}{-2}}-\int 2x{\bigg (}{\frac {e^{-2x}}{-2}}{\bigg )}~dx}\\&&\\&=&\displaystyle {{\frac {x^{2}e^{-2x}}{-2}}+\int xe^{-2x}~dx.}\end{array}}}
Now, we need to use integration by parts a second time.
Let and
Then, Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle du=dx} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v={\frac {e^{-2x}}{-2}}.}
Therefore, using integration by parts again, we get
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {\int x^{2}e^{-2x}~dx}&=&\displaystyle {{\frac {x^{2}e^{-2x}}{-2}}+{\frac {xe^{-2x}}{-2}}-\int {\frac {e^{-2x}}{-2}}~dx}\\&&\\&=&\displaystyle {{\frac {x^{2}e^{-2x}}{-2}}+{\frac {xe^{-2x}}{-2}}+{\frac {e^{-2x}}{-4}}+C.}\end{array}}}
So, we have
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int x^{2}e^{-2x}~dx={\frac {x^{2}e^{-2x}}{-2}}+{\frac {xe^{-2x}}{-2}}+{\frac {e^{-2x}}{-4}}+C.}
Exercise 5
Evaluate Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle \int e^{3x}\sin(2x)~dx.}
We begin by letting Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle u=\sin(2x)} and Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dv=e^{3x}~dx.}
Then,
To find Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v,} we need to use substitution. So,
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle v=\int e^{3x}~dx={\frac {e^{3x}}{3}}.}
Hence, by integration by parts, we have
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\begin{array}{rcl}\displaystyle {\int e^{3x}\sin(2x)~dx}&=&\displaystyle {{\frac {e^{3x}\sin(2x)}{3}}-\int {\frac {2}{3}}\cos(2x)e^{3x}~dx}\\&&\\&=&\displaystyle {{\frac {e^{3x}\sin(2x)}{3}}-{\frac {2}{3}}\int \cos(2x)e^{3x}~dx.}\end{array}}}
Now, we need to use integration by parts a second time.
Let Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u=\cos (2x)} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dv=e^{3x}~dx.}
Then, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle du=-2\sin(2x)~dx} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v=\frac{e^{3x}}{3}.}
Therefore, using integration by parts again, we get
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{array}{rcl} \displaystyle{\int e^{3x} \sin(2x)~dx} & = & \displaystyle{\frac{e^{3x}\sin(2x)}{3}-\frac{2}{3} \bigg[ \frac{\cos(2x)e^{3x}}{3}+\int \frac{2}{3}\sin(2x)e^{3x}~dx\bigg]}\\ &&\\ & = & \displaystyle{\frac{e^{3x}\sin(2x)}{3}-\frac{2\cos(2x)e^{3x}}{9}-\frac{4}{9}\int e^{3x}\sin(2x)~dx.} \end{array}}
Now, we have the exact same integral that we had at the beginning of the problem.
So, we add this integral to the other side of the equation.
When we do this, we get
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{13}{9} \int e^{3x}\sin(2x)~dx = \frac{e^{3x}\sin(2x)}{3}-\frac{2\cos(2x)e^{3x}}{9}.}
Therefore, we get
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int e^{3x}\sin(2x)~dx = \frac{9}{13}\bigg(\frac{e^{3x}\sin(2x)}{3}-\frac{2\cos(2x)e^{3x}}{9}\bigg)+C.}
Exercise 6
Evaluate Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int \sin(2x)\cos(3x)~dx.}
For this problem, we use a similar process as Exercise 5.
We use integration by parts twice, which produces the same integral given to us in the problem.
Then, we solve for our integral.
We begin by letting Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u=\sin(2x)} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dv=\cos(3x)~dx.}
Then, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle du=2\cos (2x)~dx.}
To find Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v,} we need to use Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u-} substitution. So,
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v=\int \cos(3x)~dx=\frac{1}{3}\sin(3x).}
Hence, by integration by parts, we have
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{array}{rcl} \displaystyle{\int \sin(2x)\cos(3x)~dx} & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)-\int \frac{2}{3}\cos(2x)\sin(3x)~dx}\\ &&\\ & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)-\frac{2}{3} \int \cos(2x)\sin(3x)~dx.} \end{array}}
Now, we need to use integration by parts a second time.
Let Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u=\cos (2x)} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dv=\sin(3x)~dx.}
Then, Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle du=-2\sin(2x)~dx} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v=\frac{-\cos(3x)}{3}.}
Therefore, using integration by parts again, we get
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{array}{rcl} \displaystyle{\int \sin(2x)\cos(3x)~dx} & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)-\frac{2}{3} \bigg[ \frac{-\cos(2x)\cos(3x)}{3}-\int \frac{2}{3}\sin(2x)\cos(3x)~dx\bigg]}\\ &&\\ & = & \displaystyle{\frac{1}{3}\sin(2x)\sin(3x)+ \frac{2\cos(2x)\cos(3x)}{9}+\frac{4}{9}\int \sin(2x)\cos(3x)~dx.} \end{array}}
Now, we have the exact same integral that we had at the beginning of the problem.
So, we subtract this integral to the other side of the equation.
When we do this, we get
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{5}{9} \int \sin(2x)\cos(3x)~dx = \frac{1}{3}\sin(2x)\sin(3x)+ \frac{2\cos(2x)\cos(3x)}{9}.}
Therefore, we get
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int e^{3x}\sin(2x)~dx = \frac{9}{5}\bigg(\frac{1}{3}\sin(2x)\sin(3x)+ \frac{2\cos(2x)\cos(3x)}{9}\bigg)+C.}