Η παραγοντική ολοκλήρωση είναι σημαντική μέθοδος για τον υπολογισμό σύνθετων περιπτώσεων ολοκληρωμάτων
![Rendered by QuickLaTeX.com \[ \begin{tabular}{r l r r r c r} $ 1.)\dint_{\frac{\pi}{6}}^{\frac{\pi}{2}}\dfrac{x}{\hm^{2} x}\, dx.$ & & & 2.)$\dint_{0}^{\frac{\pi}{3}}\dfrac{x-\hm x}{\syn^{2}x}dx$ & & & \\\\ & & & & & & \\\\ 3.)$\dint_{1}^{4}\dfrac{\ln x}{\sqrt{x}}\, dx$ & & & 4.)$ \dint_{\frac{1}{e}}^{1}\dfrac{\ln x}{x^{2}}dx.$ & & & \\ \end{tabular}\\ \]](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-9dd3eaeeb35bf3c1c7b5f1bc0da226c6_l3.png)
Παράδειγμα.1.
Να υπολογίσετε το ολοκλήρωμα: ![]()
Λύση
![Rendered by QuickLaTeX.com \begin{align*} &\int_{\frac{\pi}{6}}^{\frac{\pi}{2}}\dfrac{x}{\hm^{2} x}\, dx=\\\\ &\int_{\frac{\pi}{6}}^{\frac{\pi}{2}}x\cdot \dfrac{1}{\hm^{2} x} \, dx=\\\\ &\int_{\frac{\pi}{6}}^{\frac{\pi}{2}}x\cdot \Big(-\snf x\Big)'\, dx=\\\\ &\Big[ x\cdot \big(-\snf x\big)\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}-\int_{\frac{\pi}{6}}^{\frac{\pi}{2}}(x)'\cdot \big(-\snf x\big)\, dx=\\\\ &\Big[ x\cdot \big(-\snf x\big)\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}-\int_{\frac{\pi}{6}}^{\frac{\pi}{2}} -\snf x \, dx=\\\\ &\Big[ x\cdot \big(-\snf x\big)\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}+\int_{\frac{\pi}{6}}^{\frac{\pi}{2}}\dfrac{\syn x}{\hm x} \, dx=\\\\ &\Big[ x\cdot \big(-\snf x\big)\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}-\int_{\frac{\pi}{6}}^{\frac{\pi}{2}} \dfrac{(\hm x)'}{\hm x} \, dx=\\\\ &\Big[ x\cdot \big(-\snf x\big)\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}-\int_{\frac{\pi}{6}}^{\frac{\pi}{2}} \big(\ln|\hm x|\big)' \, dx=\\\\ &\Big[ x\cdot \big(-\snf x\big)\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}-\Big[ \ln|\hm x|\Big]_{\frac{\pi}{6}}^{\frac{\pi}{2}}= \end{align*}](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-aa3a3b41e8ee935f80d8ec3f88eee8aa_l3.png)
![Rendered by QuickLaTeX.com \Bigg\{ \bigg[\frac{\pi}{2}\cdot \big(-\snf \dfrac{\pi}{2}\big)\bigg]-\bigg[\frac{\pi}{6}\cdot \big(-\snf \dfrac{\pi}{6}\big) \bigg] \Bigg\} -\Big(\ln|\hm \dfrac{\pi}{2}| -\ln|\hm \dfrac{\pi}{6}|\Big)=](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-52b2130ef8581fc85f07f595d19bf2e2_l3.png)
![]()
![]()
![]()
![]()
Παράδειγμα.2.
Να υπολογίσετε το ολοκλήρωμα: ![]()
Λύση
![Rendered by QuickLaTeX.com \begin{align*} &\int_{0}^{\frac{\pi}{3}}\dfrac{x-\hm x}{\syn^{2}x}dx = \\\\ & \int_{0}^{\frac{\pi}{3}}(x-\hm x)\cdot \dfrac{1}{\syn^{2}x}dx =\\\\ &\int_{0}^{\frac{\pi}{3}}(x-\hm x)\cdot(\ef x)' dx =\\\\ &\Big[ (x-\hm x)\cdot \ef x\Big]_{0}^{\frac{\pi}{3}} -\int_{0}^{\frac{\pi}{2}}(x-\hm x)'\cdot \ef x dx=\\\\ \end{align*}](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-00f94d92a4d99b4bfb03aa01e7bc2d52_l3.png)
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
Παράδειγμα.3.
Να υπολογίσετε το ολοκλήρωμα: ![]()
Λύση
![Rendered by QuickLaTeX.com \begin{align*} &\int_{1}^{4}\dfrac{\ln x}{\sqrt{x}}\, dx =\\\\ &\int_{1}^{4} \dfrac{1}{\sqrt{x}}\cdot \ln x\, dx=\\\\ &\int_{1}^{4} \dfrac{1}{2\sqrt{x}}\cdot 2 \cdot \ln x\, dx=\\\\ &\int_{1}^{4} \big( \sqrt{x}\big)'\cdot 2 \cdot \ln x\, dx =\\\\ &\Big[ 2 \cdot\sqrt{x}\cdot\ln x\Big]_{1}^{4} - \int_{1}^{4} \sqrt{x}\cdot \big(2 \cdot \ln x\big)'\, dx =\\\\ &\Big[ \big(2 \cdot\sqrt{4}\cdot\ln 4\big)-\big(2 \cdot\sqrt{1}\cdot\ln 1\big)\Big] - \int_{1}^{4} \sqrt{x}\cdot \dfrac{2}{x}\, dx =\\\\ &\Big[ \big(2 \cdot2\cdot\ln 4\big)-\big(2 \cdot\sqrt{1}\cdot 0 \big)\Big] - \int_{1}^{4} \sqrt{x}\cdot \dfrac{2}{x}\, dx =\\\\ &\Big[ \big(4\ln 4\big)-\big( 0 \big)\Big] - \int_{1}^{4} \sqrt{x}\cdot \dfrac{2}{\sqrt{x}^{2}}\, dx \end{align*}](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-4d329c0857f65833ca8466f546c94c0d_l3.png)
Συνεπώς
![Rendered by QuickLaTeX.com \begin{align*} &4\ln 4 - \int_{1}^{4} \dfrac{2}{\sqrt{x}}\, dx =\\\\ &4\ln 4 - \int_{1}^{4} \dfrac{4}{2\cdot\sqrt{x}}\, dx =\\\\ &4\ln 4 - 4\cdot\int_{1}^{4} \dfrac{1}{2\cdot\sqrt{x}}\, dx =\\\\ &4\ln 4 - 4\cdot\int_{1}^{4} \big(\sqrt{x}\big)' =\\\\ &4\ln 4 - 4\cdot\Big[\sqrt{x}\Big]_{1}^{4} =\\\\ &4\ln 4 - 4\cdot\big (\sqrt{4}-\sqrt{1} \big) = 4\ln 4 -4. \end{align*}](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-6f39e1c1d9f779187963c488aca54231_l3.png)
Παράδειγμα.4.
Να υπολογισθεί το ολοκλήρωμα
![]()
Λύση
Έχουμε:
![]()
![Rendered by QuickLaTeX.com \begin{align*} &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}- \int_{\frac{1}{e}}^{1}\big(-\dfrac{1}{x}\big)\cdot \Big(\ln x \Big)'dx =\\\\ &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}- \int_{\frac{1}{e}}^{1}\big(-\dfrac{1}{x}\big)\cdot \dfrac{1}{x}\,dx =\\\\ &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}+ \int_{\frac{1}{e}}^{1}\dfrac{1}{x}\cdot \dfrac{1}{x}\,dx =\\\\ &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}+ \int_{\frac{1}{e}}^{1}\dfrac{1}{x^{2}}\,dx =\\\\ &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}+ \int_{\frac{1}{e}}^{1}\Big(-\dfrac{1}{x}\Big)'dx =\\\\ &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}- \int_{\frac{1}{e}}^{1}\Big(\dfrac{1}{x}\Big)'dx =\\\\ &\Big[-\dfrac{1}{x} \cdot \ln x \Big]_{\frac{1}{e}}^{1}- \Big[\dfrac{1}{x}\Big]_{\frac{1}{e}}^{1} =\\\\ &\Big[\big(-\dfrac{1}{1} \cdot \ln 1\big)-\big(-\dfrac{1}{\frac{1}{e}} \cdot \ln \frac{1}{e}\big) \Big]- \Big[\dfrac{1}{1}-\dfrac{1}{\frac{1}{e}}\Big]=\\\\ &\Big[\big(0)-\big(-e\cdot \ln \frac{1}{e}\big) \Big]- \Big[1-e\Big]=\\\\ \end{align*}](https://study4maths.gr/wp-content/ql-cache/quicklatex.com-3297a99b4e079b58cae9fbaa7f6a1d5f_l3.png)

Βιβλιογραφία: Μπάρλας εκδόσεις Ελληνοεκδοτική. Παπαδάκης εκδόσεις Σαββάλα.

Αυτή η εργασία χορηγείται με άδεια Creative Commons Αναφορά Δημιουργού – Μη Εμπορική Χρήση – Παρόμοια Διανομή 4.0 Διεθνές .