গণিতে **নির্দিষ্ট সমাকল**

{\displaystyle \int \_{a}^{b}f(x)\,dx}
xy-সমতলের গ্রাফ f, x-অক্ষ, তথা x = a ও x = b রেখা দ্বারা সীমাবদ্ধ ক্ষেত্রের ক্ষেত্রফলের সমান হয়। (x-অক্ষের উপরের ক্ষেত্রফল ধনাত্মক নেওয়া হয় যেখানে x-অক্ষের নীচের ক্ষেত্র ঋনাত্মক)

মূলদ বা অমূলদ অপেক্ষক সমন্বিত নির্দিষ্ট সমাকল
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{\displaystyle \int \_{0}^{\infty }{\frac {dx}{x^{2}+a^{2}}}={\frac {\pi }{2a}}}
{\displaystyle \int \_{0}^{a}{\frac {x^{m}dx}{x^{n}+a^{n}}}={\frac {\pi a^{m-n+1}}{n\sin[(m+1)\pi /n)]}}}
{\displaystyle \int \_{0}^{\infty }{\frac {x^{p-1}dx}{1+x}}={\frac {\pi }{\sin p\pi }}\ \,0<p<1}
{\displaystyle \int \_{0}^{\infty }{\frac {x^{m}dx}{1+2x\cos \beta +x^{2}}}={\frac {\pi }{\sin(m\pi )}}{\frac {\sin(m\beta )}{\sin \beta }}}
{\displaystyle \int \_{0}^{\infty }{\frac {dx}{\sqrt {a^{2}-x^{2}}}}={\frac {\pi }{2}}}
{\displaystyle \int \_{0}^{a}{\sqrt {a^{2}-x^{2}}}\,dx={\frac {\pi a^{2}}{4}}}
{\displaystyle \int \_{0}^{a}x^{m}(a^{n}-x^{n})^{p}\,dx={\frac {a^{m+1+np}\Gamma [(m+1)/n]\Gamma (p+1)}{n\Gamma [((m+1)/n)+p+1]}}}
{\displaystyle \int \_{0}^{\infty }{\frac {x^{m}\,dx}{({x^{n}+a^{n})}^{r}}}={\frac {(-1)^{r-1}\pi a^{m+1-nr}\Gamma [(m+1)/n]}{n\sin[(m+1)\pi /n](r-1)!\Gamma [(m+1)/n-r+1]}}\ \,0<m+1<nr}

ত্রিকোণমিতিক অপেক্ষক সমন্বিত নির্দিষ্ট সমাকল
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{\displaystyle \int \_{0}^{\pi }\sin mx\sin nx\,dx={\begin{cases}0&{\text{if }}m\neq n\\\pi /2&{\text{if }}m=n\end{cases}}\ \ m,n{\text{ integers}}}
{\displaystyle \int \_{0}^{\pi }\cos mx\cos nxdx={\begin{cases}0&{\text{if }}m\neq n\\\pi /2&{\text{if }}m=n\end{cases}}\ \ m,n{\text{ integers}}}
{\displaystyle \int \_{0}^{\pi }\sin mx\cos nx\,dx={\begin{cases}0&{\text{if }}m+n{\text{ even}}\\{\frac {2m}{m^{2}-n^{2}}}&{\text{if }}m+n{\text{ odd}}\end{cases}}\ \ m,n{\text{ integers}}.}
{\displaystyle \int \_{0}^{\pi /2}\sin ^{2}x\,dx=\int \_{0}^{\pi /2}\cos ^{2}x\,dx=\pi /4}
{\displaystyle \int \_{0}^{\pi /2}\sin ^{2m}x\,dx=\int \_{0}^{\pi /2}\cos ^{2m}x\,dx={\frac {1\times 3\times 5\times \cdots \times (2m-1)}{2\times 4\times 6\times \cdots \times 2m}}{\frac {\pi }{2}}\ \ m=1,2,3,\ldots }
{\displaystyle \int \_{0}^{\pi /2}\sin ^{2m+1}x\,dx=\int \_{0}^{\pi /2}\cos ^{2m+1}x\,dx={\frac {2\times 4\times 6\times \cdots \times 2m}{1\times 3\times 5\times \cdots \times (2m-1)}}\ \ m=1,2,3,\ldots }
{\displaystyle \int \_{0}^{\pi /2}\sin ^{2p-1}\cos ^{2q-1}x\,dx={\frac {\Gamma (p)\Gamma (q)}{2\Gamma (p+q)}}}
{\displaystyle \int \_{0}^{\infty }{\frac {\sin px}{x}}\,dx={\begin{cases}\pi /2&{\text{if }}p>0\\0&{\text{if }}p=0\\-\pi /2&{\text{if }}p<0\end{cases}}}
{\displaystyle \int \_{0}^{\infty }{\frac {\sin px\cos qx}{x}}\ dx={\begin{cases}0&{\text{ if }}p>q>0\\\pi /2&{\text{ if }}0<p<q\\\pi /4&{\text{ if }}p=q>0\end{cases}}}

{\displaystyle \int \_{0}^{\infty }{\frac {\sin px\sin qx}{x^{2}}}\ dx={\begin{cases}\pi p/2&{\text{ if }}0<p\leq q\\\pi q/2&{\text{ if }}0<q\leq p\end{cases}}}

{\displaystyle \int \_{0}^{\infty }{\frac {\sin ^{2}px}{x^{2}}}\ dx={\frac {\pi p}{2}}}

{\displaystyle \int \_{0}^{\infty }{\frac {1-\cos px}{x^{2}}}\ dx={\frac {\pi p}{2}}}

{\displaystyle \int \_{0}^{\infty }{\frac {\cos px-\cos qx}{x}}\ dx=\ln {\frac {q}{p}}}

{\displaystyle \int \_{0}^{\infty }{\frac {\cos px-\cos qx}{x^{2}}}\ dx={\frac {\pi (q-p)}{2}}}

{\displaystyle \int \_{0}^{\infty }{\frac {\cos mx}{x^{2}+a^{2}}}\ dx={\frac {\pi }{2a}}e^{-ma}}

{\displaystyle \int \_{0}^{\infty }{\frac {x\sin mx}{x^{2}+a^{2}}}\ dx={\frac {\pi }{2}}e^{-ma}}
{\displaystyle \int \_{0}^{\infty }{\frac {\sin mx}{x(x^{2}+a^{2})}}\ dx={\frac {\pi }{2a^{2}}}(1-e^{-ma})}
{\displaystyle \int \_{0}^{2\pi }{\frac {dx}{a+b\sin x}}={\frac {2\pi }{\sqrt {a^{2}-b^{2}}}}}
{\displaystyle \int \_{0}^{2\pi }{\frac {dx}{a+b\cos x}}={\frac {2\pi }{\sqrt {a^{2}-b^{2}}}}}
{\displaystyle \int \_{0}^{\frac {\pi }{2}}{\frac {dx}{a+b\cos x}}={\frac {\cos ^{-1}(b/a)}{\sqrt {a^{2}-b^{2}}}}}
{\displaystyle \int \_{0}^{2\pi }{\frac {dx}{(a+b\sin x)^{2}}}=\int \_{0}^{2\pi }{\frac {dx}{(a+b\cos x)^{2}}}={\frac {2\pi a}{(a^{2}-b^{2})^{3/2}}}}
{\displaystyle \int \_{0}^{2\pi }{\frac {dx}{1-2a\cos x+a^{2}}}={\frac {2\pi }{1-a^{2}}}\ \ \,\ 0<a<1}
{\displaystyle \int \_{0}^{\pi }{\frac {x\sin x\ dx}{1-2a\cos x+a^{2}}}={\begin{cases}{\frac {\pi }{a}}\ln(1+a)&{\text{if }}|a|<1\\\pi \ln(1+1/a)&{\text{if }}|a|>1\end{cases}}}
{\displaystyle \int \_{0}^{\pi }{\frac {\cos mx\ dx}{1-2a\cos x+a^{2}}}={\frac {\pi a^{m}}{1-a^{2}}}\quad ,a^{2}<1,\ m=0,1,2,\dots }
{\displaystyle \int \_{0}^{\infty }\sin ax^{2}\ dx=\int \_{0}^{\infty }\cos ax^{2}={\frac {1}{2}}{\sqrt {\frac {\pi }{2a}}}}
{\displaystyle \int \_{0}^{\infty }\sin ax^{n}={\frac {1}{na^{1/n}}}\Gamma (1/n)\sin {\frac {\pi }{2n}}\quad ,n>1}
{\displaystyle \int \_{0}^{\infty }\cos ax^{n}={\frac {1}{na^{1/n}}}\Gamma (1/n)\cos {\frac {\pi }{2n}}\quad ,n>1}
{\displaystyle \int \_{0}^{\infty }{\frac {\sin x}{\sqrt {x}}}\ dx=\int \_{0}^{\infty }{\frac {\cos x}{\sqrt {x}}}\ dx={\sqrt {\frac {\pi }{2}}}}
{\displaystyle \int \_{0}^{\infty }{\frac {\sin x}{x^{p}}}\ dx={\frac {\pi }{2\Gamma (p)\sin(p\pi /2)}},\quad 0<p<1}
{\displaystyle \int \_{0}^{\infty }{\frac {\cos x}{x^{p}}}\ dx={\frac {\pi }{2\Gamma (p)\cos(p\pi /2)}},\quad 0<p<1}
{\displaystyle \int \_{0}^{\infty }\sin ax^{2}\cos 2bx\ dx={\frac {1}{2}}{\sqrt {\frac {\pi }{2a}}}(\cos {\frac {b^{2}}{a}}-\sin {\frac {b^{2}}{a}})}
{\displaystyle \int \_{0}^{\infty }\cos ax^{2}\cos 2bx\ dx={\frac {1}{2}}{\sqrt {\frac {\pi }{2a}}}(\cos {\frac {b^{2}}{a}}+\sin {\frac {b^{2}}{a}})}

চলসূচকীয় অপেক্ষক সমন্বিত নির্দিষ্ট সমাকল
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{\displaystyle \int \_{0}^{\infty }e^{-ax}\cos bx\,dx={\frac {a}{a^{2}+b^{2}}}}
{\displaystyle \int \_{0}^{\infty }e^{-ax}\sin bx\,dx={\frac {b}{a^{2}+b^{2}}}}
{\displaystyle \int \_{0}^{\infty }{\frac {{}e^{-ax}\sin bx}{x}}\,dx=\tan ^{-1}{\frac {b}{a}}}
{\displaystyle \int \_{0}^{\infty }{\frac {e^{-ax}-e^{-bx}}{x}}\,dx=\ln {\frac {b}{a}}}
{\displaystyle \int \_{0}^{\infty }{e^{-ax^{2}}}\,dx={\frac {1}{2}}{\sqrt {\frac {\pi }{a}}}}
{\displaystyle \int \_{0}^{\infty }{e^{-ax^{2}}}\cos bx\,dx={\frac {1}{2}}{\sqrt {\frac {\pi }{a}}}e^{-b^{2}/4a}}
{\displaystyle \int \_{0}^{\infty }e^{-(ax^{2}+bx+c)}\,dx={\frac {1}{2}}{\sqrt {\frac {\pi }{a}}}e^{(b^{2}-4ac)/4a}\ \operatorname {erfc} {\frac {b}{2{\sqrt {a}}}},{\text{ where }}\operatorname {erfc} (p)={\frac {2}{\sqrt {\pi }}}\int \_{p}^{\infty }e^{-x^{2}}\,dx}
{\displaystyle \int \_{-\infty }^{+\infty }e^{-(ax^{2}+bx+c)}\ dx={\sqrt {\frac {\pi }{a}}}e^{(b^{2}-4ac)/4a}}
{\displaystyle \int \_{0}^{\infty }x^{n}e^{-ax}\ dx={\frac {\Gamma (n+1)}{a^{n+1}}}}
{\displaystyle \int \_{0}^{\infty }x^{m}e^{-ax^{2}}\ dx={\frac {\Gamma [(m+1)/2]}{2a^{(m+1)/2}}}}
{\displaystyle \int \_{0}^{\infty }e^{-ax^{2}-b/x^{2}}\ dx={\frac {1}{2}}{\sqrt {\frac {\pi }{a}}}e^{-2{\sqrt {ab}}}}
{\displaystyle \int \_{0}^{\infty }{\frac {x}{e^{x}-1}}\ dx=\zeta (2)={\frac {\pi ^{2}}{6}}}
{\displaystyle \int \_{0}^{\infty }{\frac {x^{n-1}}{e^{x}-1}}\ dx=\Gamma (n)\zeta (n)}
{\displaystyle \int \_{0}^{\infty }{\frac {x}{e^{x}+1}}\ dx={\frac {1}{1^{2}}}-{\frac {1}{2^{2}}}+{\frac {1}{3^{2}}}-{\frac {1}{4^{2}}}+\dots ={\frac {\pi ^{2}}{12}}}
{\displaystyle \int \_{0}^{\infty }{\frac {\sin mx}{e^{2\pi x}-1}}\ dx={\frac {1}{4}}\coth {\frac {m}{2}}-{\frac {1}{2m}}}
{\displaystyle \int \_{0}^{\infty }({\frac {1}{1+x}}-e^{-x}){\frac {dx}{x}}=\gamma }
{\displaystyle \int \_{0}^{\infty }{\frac {e^{-x^{2}}-e^{-x}}{x}}\ dx={\frac {\gamma }{2}}}
{\displaystyle \int \_{0}^{\infty }({\frac {1}{e^{x}-1}}-{\frac {e^{-x}}{x}})dx=\gamma }
{\displaystyle \int \_{0}^{\infty }{\frac {e^{-ax}-e^{-bx}}{x\sec px}}\ dx={\frac {1}{2}}\ln {\frac {b^{2}+p^{2}}{a^{2}+p^{2}}}}
{\displaystyle \int \_{0}^{\infty }{\frac {e^{-ax}-e^{-bx}}{x\csc px}}\ dx=\tan ^{-1}{\frac {b}{p}}-\tan ^{-1}{\frac {a}{p}}}
{\displaystyle \int \_{0}^{\infty }{\frac {e^{-ax}(1-\cos x)}{x^{2}}}\ dx=\cot ^{-1}a-{\frac {a}{2}}\ln(a^{2}+1)}
{\displaystyle \int \_{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}}
{\displaystyle \int \_{-\infty }^{\infty }x^{2(n+1)}e^{-x^{2}/2}\,dx={\frac {(2n+1)!}{2^{n}n!}}{\sqrt {2\pi }}\quad n=0,1,2,\ldots }

লঘুগণকীয় অপেক্ষক সমন্বিত নির্দিষ্ট সমাকল
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{\displaystyle \int \_{0}^{1}x^{m}(\ln x)^{n}\,dx={\frac {(-1)^{n}n!}{(m+1)^{n+1}}}\quad m>-1,n=0,1,2,\ldots }
{\displaystyle \int \_{0}^{1}{\frac {\ln x}{1+x}}\,dx=-{\frac {\pi ^{2}}{12}}}
{\displaystyle \int \_{0}^{1}{\frac {\ln x}{1-x}}\,dx=-{\frac {\pi ^{2}}{6}}}
{\displaystyle \int \_{0}^{1}{\frac {\ln(1+x)}{x}}\,dx={\frac {\pi ^{2}}{12}}}
{\displaystyle \int \_{0}^{1}{\frac {\ln(1-x)}{x}}\,dx=-{\frac {\pi ^{2}}{6}}}

হাইপারবোলিক অপেক্ষক সমন্বিত নির্দিষ্ট সমাকল
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{\displaystyle \int \_{0}^{\infty }{\frac {\sin ax}{\sinh bx}}\ dx={\frac {\pi }{2b}}\tanh {\frac {a\pi }{2b}}}

{\displaystyle \int \_{0}^{\infty }{\frac {\cos ax}{\cosh bx}}\ dx={\frac {\pi }{2b}}{\frac {1}{\cosh {\frac {a\pi }{2b}}}}}

{\displaystyle \int \_{0}^{\infty }{\frac {x}{\sinh ax}}\ dx={\frac {\pi ^{2}}{4a^{2}}}}

বিবিধ
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{\displaystyle \int \_{0}^{\infty }{\frac {f(ax)-f(bx)}{x}}\ dx=[{f(0)-f(\infty )}]\ln {\frac {b}{a}}}

{\displaystyle \int \_{-a}^{a}(a+x)^{m-1}(a-x)^{n-1}\ dx=(2a)^{m+n-1}{\frac {\Gamma (m)\Gamma (n)}{\Gamma (m+n)}}}

আরও দেখুন
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* সমাকলনের তালিকাসমূহ (List of integrals)
* গামা অপেক্ষক (Gamma function)
* সীমার তালিকা (List of limits)

তথ্যসূত্র
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1. Murray R. Spiegel, Seymour Lipschutz, John Liu (২০০৯)। *Mathematical handbook of formulas and tables*বিনামূল্যে নিবন্ধন প্রয়োজন (3rd ed. সংস্করণ)। McGraw-Hill। আইএসবিএন 978-0071548557। উদ্ধৃতি শৈলী রক্ষণাবেক্ষণ: একাধিক নাম: লেখকগণের তালিকা (link) উদ্ধৃতি শৈলী রক্ষণাবেক্ষণ: অতিরিক্ত লেখা (link)
2. Zwillinger, Daniel (২০০৩)। *CRC standard mathematical tables and formulae*বিনামূল্যে নিবন্ধন প্রয়োজন (32nd ed. সংস্করণ)। CRC Press। আইএসবিএন 978-1439835487। উদ্ধৃতি শৈলী রক্ষণাবেক্ষণ: অতিরিক্ত লেখা (link)
3. Abramowitz, Milton; Stegun, Irene A. (১৯৬৫)। *Handbook of mathematical functions with formulas, graphs, and mathematical tables*বিনামূল্যে নিবন্ধন প্রয়োজন (Unabridged and unaltered republ. [der Ausg.] 1964, 5. Dover printing সংস্করণ)। U.S. Govt. Print. Off.। আইএসবিএন 978-0486612720।

বহিঃসংযোগ
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