â¹ïž Skipped - page is already crawled
| Filter | Status | Condition | Details |
|---|---|---|---|
| HTTP status | PASS | download_http_code = 200 | HTTP 200 |
| Age cutoff | PASS | download_stamp > now() - 6 MONTH | 0.2 months ago |
| History drop | PASS | isNull(history_drop_reason) | No drop reason |
| Spam/ban | PASS | fh_dont_index != 1 AND ml_spam_score = 0 | ml_spam_score=0 |
| Canonical | PASS | meta_canonical IS NULL OR = '' OR = src_unparsed | Not set |
| Property | Value |
|---|---|
| URL | https://mathlog.info/articles/eD5JeKj6fR5nUna80ejj |
| Last Crawled | 2026-04-04 20:44:51 (6 days ago) |
| First Indexed | 2023-10-11 01:22:07 (2 years ago) |
| HTTP Status Code | 200 |
| Meta Title | logãããç©åã®è§£æ³ãŸãšã | Mathlog |
| Meta Description | # $\log$ãããç©åã®è§£æ³ã«ã€ã㊠ã©ããããããã§ãã ä»åã¯$\log$ãããç©åã®è§£æ³ã«ã€ããŠãŸãšããŠã¿ãŸããã ããããç¥ã£ãŠã$\log$ãããç©åã¯ããããç¥ãéãã¯5ã€ãã£ãŠãéšåç©å,眮æç©å,çŽæ°å±é,埮å,çæ°å®çã®5ã€ã§ãã ããããæžããŠãããŸãã ## éšåç©å $\displaystyle\frac{d}{dx}\log x=\frac{1}{x}$ãšéšåç©åã䜿ã£ãŠç©åãè§£ããããšããããŸãã $$\int f(x)g(x)dx=f(x)G(x)-\int f'(x)G(x)dx$$ $\log x$ã$f$ã®æ¹ã«ããã°$\log x$ã$\displaystyle\frac{1}{x}$ã«ãªã£ãŠè§£ããããšããããŸãã &&& \begin{align} I&=\int_{0}^{1}x\log x dx \\&=\left[\frac{x^2}{2}\log x\right]^{1}_{0}-\frac{1}{2}\int_{0}^{1}xdx \\&=\frac{1}{2}\lim_{x\to0}x^2\log x-\frac{1}4 \\&=-\frac{1}{4} \end{align} \begin{align} \lim_{x\to0}x^2\log x &=\lim_{x\to0}\frac{\log x}{\frac{1}{x^2}} \\&=\lim_{x\to0}\frac{\frac{1}{x}}{-\frac{2}{x^3 }} \\&=-\frac{1}{2}\lim_{x\to0}x^2 \\&=0 \end{align} &&& ãããªæãã§éšåç©åã§è§£ããããšããã£ããããŸãã æ¥µéã§ã$\log x$ã®åŸ®åã$\displaystyle\frac{1}{x}$ã§ããããšã䜿ã£ãŠãŸããã ## 眮æç©å $\log x=t$ã§çœ®æããããšã§è§£ããããšããããŸãã é颿°ã¯$e^t=x$ã§ãã $dx$ãš$dt$ã®é¢ä¿ã¯$\displaystyle dt=\frac{dx}{x}$ã§ãã ãããã¯$\displaystyle dx=e^t\ dt$ã§ãã &&& \begin{align} I&=\int_{1}^{e}\frac{\log x}{x}dx \\&=\int_{0}^{1}t\ dt\qquad(\log x\mapsto t) \\&=1 \end{align} &&& ãšãããã忝ã«$x$ãããã°$\log x=t$ã§çœ®æããŠãããšæããŸãã ããšã¯$\mathrm{King Property}$ãäœ¿ãæ¹æ³ããã£ããããŸãã [ãã®èšäº](https://mathlog.info/articles/6ogbETh0rF02owJLJzbT)ã§$\mathrm{King Property}$ã䜿ãç©åãè§£ããŠããŸãã ## çŽæ°å±é æžãããã®ã¯ããããã§ãã çŽæ°å±éãããŠç©åãšçŽæ°ã亀æããŠç©åãè§£ããããšããããŸãã ããããç¥ã£ãŠãã$\log$é¢é£ã®çŽæ°å±éããŸãšããŠã¿ãŸãã &&& $$\log(1-x)=-\sum_{n=1}^{\infty}\frac{x^n}{n}\quad(|x|<1)$$ $$\log(1+x)=-\sum_{n=1}^{\infty}\frac{(-1)^n\ x^n}{n}\quad(|x|<1)$$ $$\log\left(2\sin\frac{x}{2}\right)=-\sum_{n=1}^{\infty}\frac{\cos nx}{n}\quad\left(0<x<\frac{\pi}{2}\right)$$ $$\log\left(2\cos\frac{x}{2}\right)=-\sum_{n=1}^{\infty}\frac{(-1)^n\ \cos nx}{n}\quad\left(0<x<\frac{\pi}{2}\right)$$ $$\log\tan\frac{x}{2}=-2\sum_{n=1}^{\infty}\frac{\cos(2n+1)x}{2n+1}\quad\left(0<x<\frac{\pi}{2}\right)$$ &&& çŽæ°å±éã䜿ã£ãŠè§£ããŠèŠãŸãããã &&& \begin{align} I&=\int_{0}^{1}\frac{\log(1+x)}{\sqrt{x}}dx \\&=-\int_{0}^{1}\sum_{n=1}^{\infty}\frac{(-1)^n\ x^n}{n\ \sqrt{x}}dx \\&=-\sum_{n=1}^{\infty}\frac{(-1)^n}{n}\int_{0}^{1}x^{n-\frac{1}{2}}\ dx \\&=-2\sum_{n=1}^{\infty}\frac{(-1)^n}{n(2n+1)} \\&=-2\left(\sum_{n=1}^{\infty}\frac{(-1)^n}{n}-2\sum_{n=1}^{\infty}\frac{(-1)^n}{2n+1}\right) \\&=-2\left(\log2+\frac{\pi}{2}-2\right) \\&=-2\log2-\pi+4 \end{align} &&& æ®éã«éšåç©åã§ãè§£ããŸãã &&& \begin{align} I&=\int_{0}^{\frac{\pi}{2}}\log\left(2\sin\frac{x}{2}\right)\log\left(2\cos\frac{x}{2}\right)dx \\&=\frac{1}{2}\int_{0}^{\pi}\log\left(2\sin\frac{x}{2}\right)\log\left(2\cos\frac{x}{2}\right)dx \\&=\frac{1}{2}\sum_{n,m>0}\frac{(-1)^n}{nm}\int_{0}^{\pi}\cos mx\cos nx dx \\&=\frac{\pi}{4}\sum_{n=1}^{\infty}\frac{(-1)^n}{n^2} \\&=-\frac{\pi^3}{48} \end{align} &&& éã§ããèš±ããŠãã ããã [åã®èšäº](https://mathlog.info/articles/nFkkmCBNuFHtPOyrFUSk)ã§å¥ã®æ¹æ³ã§è§£ããŠãŸãã ## 埮å $\displaystyle\frac{d}{ds}x^s=x^s\log x$ã䜿ã£ãŠç©åãè§£ããããšããããŸãã &&& \begin{align} I&=\int_{0}^{\infty}e^{-x}\log xdx \\&=\left.\frac{d}{ds}\int_{0}^{\infty}x^s e^{-x}dx\right|_{s=1} \\&=\Gamma'(1) \\&=\Gamma(1)\psi(1) \\&=-\gamma \end{align} &&& 埮åãšç©åã®äº€æã䜿ããŸããã &&& $$I=\int_{0}^{1}\frac{x^2-x}{\log x}dx$$ $$f(t)=\int_{0}^{1}\frac{x^t}{\log x}$$ \begin{align} f'(t)&=\int_{0}^{1}x^t \\&=\frac{1}{t+1} \end{align} \begin{align} f(2)-f(1)&=\int_{1}^{2}f'(t)dt \\&=\int_{1}^{2}\frac{1}{t+1}dt \\&=\log\frac{3}{2} \end{align} &&& ãã®è§£æ³ãããªã奜ãã§ãã ## è€çŽ ç©å è€çŽ ç©åã§è§£ããããšããã£ããããã ããããæžããŠãè€çŽ ç©åã®2ã€ã®èšäºã¯ã©ã£ã¡ã$\log$ãããã®ã§ãã¡ããã¿ãŠã»ããã([ãã](https://mathlog.info/articles/dGB4ngusgBuBJM1K6rG6)ãš[ãã](https://mathlog.info/articles/uqiFFCC5kXHH58DYZkks)) 被ç©å颿°ã«$\log x$ã ã£ããããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã§è§£ããŠããããšãå€ãæ°ãããŸãã ããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã¯åã®èšäºã§ãã£ãŠããã &&& $$I=\int_{0}^{\infty}\frac{x\log x}{x^4+1}dx$$ $$f(z)=\frac{z\log z}{z^4+1}$$  $\log0$ãåé¿ããããã«$0$ã¯é¿ããŠããŸãã $\displaystyle C_2,C_4$ã¯è©äŸ¡ããŠæ¥µéãšã°ããš$0$ã«ãªããŸãã 確èªããŠã¿ãŠãã ããã å šäœã®ç©åã$C$ãšããŠãããŸãã ããããèšç®ããŠãããŸãã \begin{align} \int_{C_1}&=\int_{\varepsilon}^{R}f(z)dz \\&=I\qquad(\ip\to0,R\to\infty) \end{align} \begin{align} \int_{C_3}&=\int_{iR}^{i\ip}f(z)dz \\&=-i\int_{\ip}^{R}f(ix)dx \\&=\int_{\ip}^{R}\frac{x\log ix}{x^4+1}dx \\&=\int_{\ip}^{R}\frac{x\log x}{x^4+1}dx+\frac{i\pi}{2}\int_{\ip}^{R}\frac{x}{x^4+1}dx \\&=I+\frac{\pi^2}{8}i\qquad(\ip\to0,R\to\infty) \end{align} \begin{align} \oint_{C}&=2\pi i\underset{z=e^{\frac{i\pi}{4}}}{\mathrm{Res}}\frac{z\log z}{z^4+1} \\&=2\pi i\lim_{z\to e^{\frac{i\pi}{4}}}\frac{z\log z(z-e^{\frac{i\pi}{4}})}{z^4+1} \\&=2\pi i\lim_{z\to e^{\frac{i\pi}{4}}}\frac{(2z-e^{\frac{i\pi}{4}})\log z-e^{\frac{i\pi}{4}}+z}{4z^3} \\&=\frac{\pi^2}{8}i \end{align} $$\oint_{C}=\int_{C_{1}}+\int_{C_{2}}+\int_{C_{3}}+\int_{C_{4}}$$ $$\frac{\pi^2}{8}i=I+I+\frac{\pi^2}{8}i$$ $$I=0$$ &&& 埮åã䜿ã£ãŠãè§£ããŸãã 被ç©å颿°ã®$\log x$ã®ææ°ã«$1$ãè¶³ããŠ$f(z)$ãèšå®ããããšããããŸãã ãããŸãŒã |
| Meta Canonical | null |
| Boilerpipe Text | $$\newcommand{ip}[0]{\varepsilon}
$$
$\log$
ãããç©åã®è§£æ³ã«ã€ããŠ
ã©ããããããã§ãã
ä»åã¯
$\log$
ãããç©åã®è§£æ³ã«ã€ããŠãŸãšããŠã¿ãŸããã
ããããç¥ã£ãŠã
$\log$
ãããç©åã¯ããããç¥ãéãã¯5ã€ãã£ãŠãéšåç©å,眮æç©å,çŽæ°å±é,埮å,çæ°å®çã®5ã€ã§ãã
ããããæžããŠãããŸãã
éšåç©å
$\displaystyle\frac{d}{dx}\log x=\frac{1}{x}$
ãšéšåç©åã䜿ã£ãŠç©åãè§£ããããšããããŸãã
$$\int f(x)g(x)dx=f(x)G(x)-\int f'(x)G(x)dx$$
$\log x$
ã
$f$
ã®æ¹ã«ããã°
$\log x$
ã
$\displaystyle\frac{1}{x}$
ã«ãªã£ãŠè§£ããããšããããŸãã
\begin{align}
I&=\int_{0}^{1}x\log x dx
\\&=\left[\frac{x^2}{2}\log x\right]^{1}_{0}-\frac{1}{2}\int_{0}^{1}xdx
\\&=\frac{1}{2}\lim_{x\to0}x^2\log x-\frac{1}4
\\&=-\frac{1}{4}
\end{align}
\begin{align}
\lim_{x\to0}x^2\log x
&=\lim_{x\to0}\frac{\log x}{\frac{1}{x^2}}
\\&=\lim_{x\to0}\frac{\frac{1}{x}}{-\frac{2}{x^3 }}
\\&=-\frac{1}{2}\lim_{x\to0}x^2
\\&=0
\end{align}
ãããªæãã§éšåç©åã§è§£ããããšããã£ããããŸãã
極éã§ã
$\log x$
ã®åŸ®åã
$\displaystyle\frac{1}{x}$
ã§ããããšã䜿ã£ãŠãŸããã
眮æç©å
$\log x=t$
ã§çœ®æããããšã§è§£ããããšããããŸãã
é颿°ã¯
$e^t=x$
ã§ãã
$dx$
ãš
$dt$
ã®é¢ä¿ã¯
$\displaystyle dt=\frac{dx}{x}$
ã§ãã
ãããã¯
$\displaystyle dx=e^t\ dt$
ã§ãã
\begin{align}
I&=\int_{1}^{e}\frac{\log x}{x}dx
\\&=\int_{0}^{1}t\ dt\qquad(\log x\mapsto t)
\\&=1
\end{align}
ãšãããã忝ã«
$x$
ãããã°
$\log x=t$
ã§çœ®æããŠãããšæããŸãã
ããšã¯
$\mathrm{King Property}$
ãäœ¿ãæ¹æ³ããã£ããããŸãã
ãã®èšäº
ã§
$\mathrm{King Property}$
ã䜿ãç©åãè§£ããŠããŸãã
çŽæ°å±é
æžãããã®ã¯ããããã§ãã
çŽæ°å±éãããŠç©åãšçŽæ°ã亀æããŠç©åãè§£ããããšããããŸãã
ããããç¥ã£ãŠãã
$\log$
é¢é£ã®çŽæ°å±éããŸãšããŠã¿ãŸãã
$$\log(1-x)=-\sum_{n=1}^{\infty}\frac{x^n}{n}\quad(|x|<1)$$
$$\log(1+x)=-\sum_{n=1}^{\infty}\frac{(-1)^n\ x^n}{n}\quad(|x|<1)$$
$$\log\left(2\sin\frac{x}{2}\right)=-\sum_{n=1}^{\infty}\frac{\cos nx}{n}\quad\left(0< x<\frac{\pi}{2}\right)$$
$$\log\left(2\cos\frac{x}{2}\right)=-\sum_{n=1}^{\infty}\frac{(-1)^n\ \cos nx}{n}\quad\left(0< x<\frac{\pi}{2}\right)$$
$$\log\tan\frac{x}{2}=-2\sum_{n=1}^{\infty}\frac{\cos(2n+1)x}{2n+1}\quad\left(0< x<\frac{\pi}{2}\right)$$
çŽæ°å±éã䜿ã£ãŠè§£ããŠèŠãŸãããã
\begin{align}
I&=\int_{0}^{1}\frac{\log(1+x)}{\sqrt{x}}dx
\\&=-\int_{0}^{1}\sum_{n=1}^{\infty}\frac{(-1)^n\ x^n}{n\ \sqrt{x}}dx
\\&=-\sum_{n=1}^{\infty}\frac{(-1)^n}{n}\int_{0}^{1}x^{n-\frac{1}{2}}\ dx
\\&=-2\sum_{n=1}^{\infty}\frac{(-1)^n}{n(2n+1)}
\\&=-2\left(\sum_{n=1}^{\infty}\frac{(-1)^n}{n}-2\sum_{n=1}^{\infty}\frac{(-1)^n}{2n+1}\right)
\\&=-2\left(\log2+\frac{\pi}{2}-2\right)
\\&=-2\log2-\pi+4
\end{align}
æ®éã«éšåç©åã§ãè§£ããŸãã
\begin{align}
I&=\int_{0}^{\frac{\pi}{2}}\log\left(2\sin\frac{x}{2}\right)\log\left(2\cos\frac{x}{2}\right)dx
\\&=\frac{1}{2}\int_{0}^{\pi}\log\left(2\sin\frac{x}{2}\right)\log\left(2\cos\frac{x}{2}\right)dx
\\&=\frac{1}{2}\sum_{n,m>0}\frac{(-1)^n}{nm}\int_{0}^{\pi}\cos mx\cos nx dx
\\&=\frac{\pi}{4}\sum_{n=1}^{\infty}\frac{(-1)^n}{n^2}
\\&=-\frac{\pi^3}{48}
\end{align}
éã§ããèš±ããŠãã ããã
åã®èšäº
ã§å¥ã®æ¹æ³ã§è§£ããŠãŸãã
埮å
$\displaystyle\frac{d}{ds}x^s=x^s\log x$
ã䜿ã£ãŠç©åãè§£ããããšããããŸãã
\begin{align}
I&=\int_{0}^{\infty}e^{-x}\log xdx
\\&=\left.\frac{d}{ds}\int_{0}^{\infty}x^s e^{-x}dx\right|_{s=1}
\\&=\Gamma'(1)
\\&=\Gamma(1)\psi(1)
\\&=-\gamma
\end{align}
埮åãšç©åã®äº€æã䜿ããŸããã
$$I=\int_{0}^{1}\frac{x^2-x}{\log x}dx$$
$$f(t)=\int_{0}^{1}\frac{x^t}{\log x}$$
\begin{align}
f'(t)&=\int_{0}^{1}x^t
\\&=\frac{1}{t+1}
\end{align}
\begin{align}
f(2)-f(1)&=\int_{1}^{2}f'(t)dt
\\&=\int_{1}^{2}\frac{1}{t+1}dt
\\&=\log\frac{3}{2}
\end{align}
ãã®è§£æ³ãããªã奜ãã§ãã
è€çŽ ç©å
è€çŽ ç©åã§è§£ããããšããã£ããããã
ããããæžããŠãè€çŽ ç©åã®2ã€ã®èšäºã¯ã©ã£ã¡ã
$\log$
ãããã®ã§ãã¡ããã¿ãŠã»ããã(
ãã
ãš
ãã
)
被ç©å颿°ã«
$\log x$
ã ã£ããããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã§è§£ããŠããããšãå€ãæ°ãããŸãã
ããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã¯åã®èšäºã§ãã£ãŠããã
$$I=\int_{0}^{\infty}\frac{x\log x}{x^4+1}dx$$
$$f(z)=\frac{z\log z}{z^4+1}$$
ç©åçµè·¯
$\log0$
ãåé¿ããããã«
$0$
ã¯é¿ããŠããŸãã
$\displaystyle C_2,C_4$
ã¯è©äŸ¡ããŠæ¥µéãšã°ããš
$0$
ã«ãªããŸãã
確èªããŠã¿ãŠãã ããã
å
šäœã®ç©åã
$C$
ãšããŠãããŸãã
ããããèšç®ããŠãããŸãã
\begin{align}
\int_{C_1}&=\int_{\varepsilon}^{R}f(z)dz
\\&=I\qquad(\ip\to0,R\to\infty)
\end{align}
\begin{align}
\int_{C_3}&=\int_{iR}^{i\ip}f(z)dz
\\&=-i\int_{\ip}^{R}f(ix)dx
\\&=\int_{\ip}^{R}\frac{x\log ix}{x^4+1}dx
\\&=\int_{\ip}^{R}\frac{x\log x}{x^4+1}dx+\frac{i\pi}{2}\int_{\ip}^{R}\frac{x}{x^4+1}dx
\\&=I+\frac{\pi^2}{8}i\qquad(\ip\to0,R\to\infty)
\end{align}
\begin{align}
\oint_{C}&=2\pi i\underset{z=e^{\frac{i\pi}{4}}}{\mathrm{Res}}\frac{z\log z}{z^4+1}
\\&=2\pi i\lim_{z\to e^{\frac{i\pi}{4}}}\frac{z\log z(z-e^{\frac{i\pi}{4}})}{z^4+1}
\\&=2\pi i\lim_{z\to e^{\frac{i\pi}{4}}}\frac{(2z-e^{\frac{i\pi}{4}})\log z-e^{\frac{i\pi}{4}}+z}{4z^3}
\\&=\frac{\pi^2}{8}i
\end{align}
$$\oint_{C}=\int_{C_{1}}+\int_{C_{2}}+\int_{C_{3}}+\int_{C_{4}}$$
$$\frac{\pi^2}{8}i=I+I+\frac{\pi^2}{8}i$$
$$I=0$$
埮åã䜿ã£ãŠãè§£ããŸãã
被ç©å颿°ã®
$\log x$
ã®ææ°ã«
$1$
ãè¶³ããŠ
$f(z)$
ãèšå®ããããšããããŸãã
ãããŸãŒã |
| Markdown | [ ](https://mathlog.info/)
æ°èŠäœæ
logãããç©åã®è§£æ³ãŸãšã
logãããç©åã®è§£æ³ãŸãšã
4
[](https://mathlog.info/users/fFUCqkukdYVw0jb9qo2zHPumDAt1)
[ããã](https://mathlog.info/users/fFUCqkukdYVw0jb9qo2zHPumDAt1)
[å€§åŠæ°åŠåºç€](https://mathlog.info/categories/2/articles)解説
# logãããç©åã®è§£æ³ãŸãšã
[ç©å](https://mathlog.info/tags/31),[log](https://mathlog.info/tags/7NjLr6aM1wPWEGX3jtWr)
4
0
1152
0
LaTeXãšã¯ã¹ããŒã
\$\$\\newcommand{ip}\[0\]{\\varepsilon} \$\$
## \$\\log\$ãããç©åã®è§£æ³ã«ã€ããŠ
ã©ããããããã§ãã
ä»åã¯\$\\log\$ãããç©åã®è§£æ³ã«ã€ããŠãŸãšããŠã¿ãŸããã
ããããç¥ã£ãŠã\$\\log\$ãããç©åã¯ããããç¥ãéãã¯5ã€ãã£ãŠãéšåç©å,眮æç©å,çŽæ°å±é,埮å,çæ°å®çã®5ã€ã§ãã
ããããæžããŠãããŸãã
### éšåç©å
\$\\displaystyle\\frac{d}{dx}\\log x=\\frac{1}{x}\$ãšéšåç©åã䜿ã£ãŠç©åãè§£ããããšããããŸãã
\$\$\\int f(x)g(x)dx=f(x)G(x)-\\int f'(x)G(x)dx\$\$
\$\\log x\$ã\$f\$ã®æ¹ã«ããã°\$\\log x\$ã\$\\displaystyle\\frac{1}{x}\$ã«ãªã£ãŠè§£ããããšããããŸãã
\\begin{align} I&=\\int\_{0}^{1}x\\log x dx \\\\&=\\left\[\\frac{x^2}{2}\\log x\\right\]^{1}\_{0}-\\frac{1}{2}\\int\_{0}^{1}xdx \\\\&=\\frac{1}{2}\\lim\_{x\\to0}x^2\\log x-\\frac{1}4 \\\\&=-\\frac{1}{4} \\end{align}
\\begin{align} \\lim\_{x\\to0}x^2\\log x &=\\lim\_{x\\to0}\\frac{\\log x}{\\frac{1}{x^2}} \\\\&=\\lim\_{x\\to0}\\frac{\\frac{1}{x}}{-\\frac{2}{x^3 }} \\\\&=-\\frac{1}{2}\\lim\_{x\\to0}x^2 \\\\&=0 \\end{align}
ãããªæãã§éšåç©åã§è§£ããããšããã£ããããŸãã
極éã§ã\$\\log x\$ã®åŸ®åã\$\\displaystyle\\frac{1}{x}\$ã§ããããšã䜿ã£ãŠãŸããã
### 眮æç©å
\$\\log x=t\$ã§çœ®æããããšã§è§£ããããšããããŸãã
é颿°ã¯\$e^t=x\$ã§ãã
\$dx\$ãš\$dt\$ã®é¢ä¿ã¯\$\\displaystyle dt=\\frac{dx}{x}\$ã§ãã
ãããã¯\$\\displaystyle dx=e^t\\ dt\$ã§ãã
\\begin{align} I&=\\int\_{1}^{e}\\frac{\\log x}{x}dx \\\\&=\\int\_{0}^{1}t\\ dt\\qquad(\\log x\\mapsto t) \\\\&=1 \\end{align}
ãšãããã忝ã«\$x\$ãããã°\$\\log x=t\$ã§çœ®æããŠãããšæããŸãã
ããšã¯\$\\mathrm{King Property}\$ãäœ¿ãæ¹æ³ããã£ããããŸãã
[ãã®èšäº](https://mathlog.info/articles/6ogbETh0rF02owJLJzbT) ã§\$\\mathrm{King Property}\$ã䜿ãç©åãè§£ããŠããŸãã
### çŽæ°å±é
æžãããã®ã¯ããããã§ãã
çŽæ°å±éãããŠç©åãšçŽæ°ã亀æããŠç©åãè§£ããããšããããŸãã
ããããç¥ã£ãŠãã\$\\log\$é¢é£ã®çŽæ°å±éããŸãšããŠã¿ãŸãã
\$\$\\log(1-x)=-\\sum\_{n=1}^{\\infty}\\frac{x^n}{n}\\quad(\|x\|\<1)\$\$
\$\$\\log(1+x)=-\\sum\_{n=1}^{\\infty}\\frac{(-1)^n\\ x^n}{n}\\quad(\|x\|\<1)\$\$
\$\$\\log\\left(2\\sin\\frac{x}{2}\\right)=-\\sum\_{n=1}^{\\infty}\\frac{\\cos nx}{n}\\quad\\left(0\< x\<\\frac{\\pi}{2}\\right)\$\$
\$\$\\log\\left(2\\cos\\frac{x}{2}\\right)=-\\sum\_{n=1}^{\\infty}\\frac{(-1)^n\\ \\cos nx}{n}\\quad\\left(0\< x\<\\frac{\\pi}{2}\\right)\$\$
\$\$\\log\\tan\\frac{x}{2}=-2\\sum\_{n=1}^{\\infty}\\frac{\\cos(2n+1)x}{2n+1}\\quad\\left(0\< x\<\\frac{\\pi}{2}\\right)\$\$
çŽæ°å±éã䜿ã£ãŠè§£ããŠèŠãŸãããã
\\begin{align} I&=\\int\_{0}^{1}\\frac{\\log(1+x)}{\\sqrt{x}}dx \\\\&=-\\int\_{0}^{1}\\sum\_{n=1}^{\\infty}\\frac{(-1)^n\\ x^n}{n\\ \\sqrt{x}}dx \\\\&=-\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n}\\int\_{0}^{1}x^{n-\\frac{1}{2}}\\ dx \\\\&=-2\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n(2n+1)} \\\\&=-2\\left(\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n}-2\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{2n+1}\\right) \\\\&=-2\\left(\\log2+\\frac{\\pi}{2}-2\\right) \\\\&=-2\\log2-\\pi+4 \\end{align}
æ®éã«éšåç©åã§ãè§£ããŸãã
\\begin{align} I&=\\int\_{0}^{\\frac{\\pi}{2}}\\log\\left(2\\sin\\frac{x}{2}\\right)\\log\\left(2\\cos\\frac{x}{2}\\right)dx \\\\&=\\frac{1}{2}\\int\_{0}^{\\pi}\\log\\left(2\\sin\\frac{x}{2}\\right)\\log\\left(2\\cos\\frac{x}{2}\\right)dx \\\\&=\\frac{1}{2}\\sum\_{n,m\>0}\\frac{(-1)^n}{nm}\\int\_{0}^{\\pi}\\cos mx\\cos nx dx \\\\&=\\frac{\\pi}{4}\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n^2} \\\\&=-\\frac{\\pi^3}{48} \\end{align}
éã§ããèš±ããŠãã ããã
[åã®èšäº](https://mathlog.info/articles/nFkkmCBNuFHtPOyrFUSk) ã§å¥ã®æ¹æ³ã§è§£ããŠãŸãã
### 埮å
\$\\displaystyle\\frac{d}{ds}x^s=x^s\\log x\$ã䜿ã£ãŠç©åãè§£ããããšããããŸãã
\\begin{align} I&=\\int\_{0}^{\\infty}e^{-x}\\log xdx \\\\&=\\left.\\frac{d}{ds}\\int\_{0}^{\\infty}x^s e^{-x}dx\\right\|\_{s=1} \\\\&=\\Gamma'(1) \\\\&=\\Gamma(1)\\psi(1) \\\\&=-\\gamma \\end{align}
埮åãšç©åã®äº€æã䜿ããŸããã
\$\$I=\\int\_{0}^{1}\\frac{x^2-x}{\\log x}dx\$\$
\$\$f(t)=\\int\_{0}^{1}\\frac{x^t}{\\log x}\$\$
\\begin{align} f'(t)&=\\int\_{0}^{1}x^t \\\\&=\\frac{1}{t+1} \\end{align}
\\begin{align} f(2)-f(1)&=\\int\_{1}^{2}f'(t)dt \\\\&=\\int\_{1}^{2}\\frac{1}{t+1}dt \\\\&=\\log\\frac{3}{2} \\end{align}
ãã®è§£æ³ãããªã奜ãã§ãã
### è€çŽ ç©å
è€çŽ ç©åã§è§£ããããšããã£ããããã
ããããæžããŠãè€çŽ ç©åã®2ã€ã®èšäºã¯ã©ã£ã¡ã\$\\log\$ãããã®ã§ãã¡ããã¿ãŠã»ããã( [ãã](https://mathlog.info/articles/dGB4ngusgBuBJM1K6rG6) ãš [ãã](https://mathlog.info/articles/uqiFFCC5kXHH58DYZkks) )
被ç©å颿°ã«\$\\log x\$ã ã£ããããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã§è§£ããŠããããšãå€ãæ°ãããŸãã
ããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã¯åã®èšäºã§ãã£ãŠããã
\$\$I=\\int\_{0}^{\\infty}\\frac{x\\log x}{x^4+1}dx\$\$
\$\$f(z)=\\frac{z\\log z}{z^4+1}\$\$
 ç©åçµè·¯
\$\\log0\$ãåé¿ããããã«\$0\$ã¯é¿ããŠããŸãã
\$\\displaystyle C\_2,C\_4\$ã¯è©äŸ¡ããŠæ¥µéãšã°ããš\$0\$ã«ãªããŸãã
確èªããŠã¿ãŠãã ããã
å
šäœã®ç©åã\$C\$ãšããŠãããŸãã
ããããèšç®ããŠãããŸãã
\\begin{align} \\int\_{C\_1}&=\\int\_{\\varepsilon}^{R}f(z)dz \\\\&=I\\qquad(\\ip\\to0,R\\to\\infty) \\end{align}
\\begin{align} \\int\_{C\_3}&=\\int\_{iR}^{i\\ip}f(z)dz \\\\&=-i\\int\_{\\ip}^{R}f(ix)dx \\\\&=\\int\_{\\ip}^{R}\\frac{x\\log ix}{x^4+1}dx \\\\&=\\int\_{\\ip}^{R}\\frac{x\\log x}{x^4+1}dx+\\frac{i\\pi}{2}\\int\_{\\ip}^{R}\\frac{x}{x^4+1}dx \\\\&=I+\\frac{\\pi^2}{8}i\\qquad(\\ip\\to0,R\\to\\infty) \\end{align}
\\begin{align} \\oint\_{C}&=2\\pi i\\underset{z=e^{\\frac{i\\pi}{4}}}{\\mathrm{Res}}\\frac{z\\log z}{z^4+1} \\\\&=2\\pi i\\lim\_{z\\to e^{\\frac{i\\pi}{4}}}\\frac{z\\log z(z-e^{\\frac{i\\pi}{4}})}{z^4+1} \\\\&=2\\pi i\\lim\_{z\\to e^{\\frac{i\\pi}{4}}}\\frac{(2z-e^{\\frac{i\\pi}{4}})\\log z-e^{\\frac{i\\pi}{4}}+z}{4z^3} \\\\&=\\frac{\\pi^2}{8}i \\end{align}
\$\$\\oint\_{C}=\\int\_{C\_{1}}+\\int\_{C\_{2}}+\\int\_{C\_{3}}+\\int\_{C\_{4}}\$\$
\$\$\\frac{\\pi^2}{8}i=I+I+\\frac{\\pi^2}{8}i\$\$
\$\$I=0\$\$
埮åã䜿ã£ãŠãè§£ããŸãã
被ç©å颿°ã®\$\\log x\$ã®ææ°ã«\$1\$ãè¶³ããŠ\$f(z)\$ãèšå®ããããšããããŸãã
ãããŸãŒã
æçš¿æ¥ïŒ2023幎10æ10æ¥
[ ](https://mathlog.info/recruit)
## ãã®èšäºãé«è©äŸ¡ãã人
é«è©äŸ¡ãããŠãŒã¶ã¯ããŸãã
## ãã®èšäºã«éããããããž
ãããžã¯ãããŸããã
## æçš¿è
[](https://mathlog.info/users/fFUCqkukdYVw0jb9qo2zHPumDAt1)
[ããã](https://mathlog.info/users/fFUCqkukdYVw0jb9qo2zHPumDAt1)
234
18462
é©åœã«æžãããããšãæžããŸãã
40Followers
19Follow
## ã³ã¡ã³ã
### ä»ã®äººã®ã³ã¡ã³ã
ã³ã¡ã³ãã¯ãããŸããã
èªã¿èŸŒã¿äž...
èªã¿èŸŒã¿äž
[ ](https://mathlog.info/recruit)
[](https://mathlog.info/users/fFUCqkukdYVw0jb9qo2zHPumDAt1)
[ããã](https://mathlog.info/users/fFUCqkukdYVw0jb9qo2zHPumDAt1)
[logãããç©åã®è§£æ³ãŸãšã](https://mathlog.info/articles/eD5JeKj6fR5nUna80ejj) |
| Readable Markdown | \$\$\\newcommand{ip}\[0\]{\\varepsilon} \$\$
## \$\\log\$ãããç©åã®è§£æ³ã«ã€ããŠ
ã©ããããããã§ãã
ä»åã¯\$\\log\$ãããç©åã®è§£æ³ã«ã€ããŠãŸãšããŠã¿ãŸããã
ããããç¥ã£ãŠã\$\\log\$ãããç©åã¯ããããç¥ãéãã¯5ã€ãã£ãŠãéšåç©å,眮æç©å,çŽæ°å±é,埮å,çæ°å®çã®5ã€ã§ãã
ããããæžããŠãããŸãã
### éšåç©å
\$\\displaystyle\\frac{d}{dx}\\log x=\\frac{1}{x}\$ãšéšåç©åã䜿ã£ãŠç©åãè§£ããããšããããŸãã
\$\$\\int f(x)g(x)dx=f(x)G(x)-\\int f'(x)G(x)dx\$\$
\$\\log x\$ã\$f\$ã®æ¹ã«ããã°\$\\log x\$ã\$\\displaystyle\\frac{1}{x}\$ã«ãªã£ãŠè§£ããããšããããŸãã
\\begin{align} I&=\\int\_{0}^{1}x\\log x dx \\\\&=\\left\[\\frac{x^2}{2}\\log x\\right\]^{1}\_{0}-\\frac{1}{2}\\int\_{0}^{1}xdx \\\\&=\\frac{1}{2}\\lim\_{x\\to0}x^2\\log x-\\frac{1}4 \\\\&=-\\frac{1}{4} \\end{align}
\\begin{align} \\lim\_{x\\to0}x^2\\log x &=\\lim\_{x\\to0}\\frac{\\log x}{\\frac{1}{x^2}} \\\\&=\\lim\_{x\\to0}\\frac{\\frac{1}{x}}{-\\frac{2}{x^3 }} \\\\&=-\\frac{1}{2}\\lim\_{x\\to0}x^2 \\\\&=0 \\end{align}
ãããªæãã§éšåç©åã§è§£ããããšããã£ããããŸãã
極éã§ã\$\\log x\$ã®åŸ®åã\$\\displaystyle\\frac{1}{x}\$ã§ããããšã䜿ã£ãŠãŸããã
### 眮æç©å
\$\\log x=t\$ã§çœ®æããããšã§è§£ããããšããããŸãã
é颿°ã¯\$e^t=x\$ã§ãã
\$dx\$ãš\$dt\$ã®é¢ä¿ã¯\$\\displaystyle dt=\\frac{dx}{x}\$ã§ãã
ãããã¯\$\\displaystyle dx=e^t\\ dt\$ã§ãã
\\begin{align} I&=\\int\_{1}^{e}\\frac{\\log x}{x}dx \\\\&=\\int\_{0}^{1}t\\ dt\\qquad(\\log x\\mapsto t) \\\\&=1 \\end{align}
ãšãããã忝ã«\$x\$ãããã°\$\\log x=t\$ã§çœ®æããŠãããšæããŸãã
ããšã¯\$\\mathrm{King Property}\$ãäœ¿ãæ¹æ³ããã£ããããŸãã
[ãã®èšäº](https://mathlog.info/articles/6ogbETh0rF02owJLJzbT) ã§\$\\mathrm{King Property}\$ã䜿ãç©åãè§£ããŠããŸãã
### çŽæ°å±é
æžãããã®ã¯ããããã§ãã
çŽæ°å±éãããŠç©åãšçŽæ°ã亀æããŠç©åãè§£ããããšããããŸãã
ããããç¥ã£ãŠãã\$\\log\$é¢é£ã®çŽæ°å±éããŸãšããŠã¿ãŸãã
\$\$\\log(1-x)=-\\sum\_{n=1}^{\\infty}\\frac{x^n}{n}\\quad(\|x\|\<1)\$\$
\$\$\\log(1+x)=-\\sum\_{n=1}^{\\infty}\\frac{(-1)^n\\ x^n}{n}\\quad(\|x\|\<1)\$\$
\$\$\\log\\left(2\\sin\\frac{x}{2}\\right)=-\\sum\_{n=1}^{\\infty}\\frac{\\cos nx}{n}\\quad\\left(0\< x\<\\frac{\\pi}{2}\\right)\$\$
\$\$\\log\\left(2\\cos\\frac{x}{2}\\right)=-\\sum\_{n=1}^{\\infty}\\frac{(-1)^n\\ \\cos nx}{n}\\quad\\left(0\< x\<\\frac{\\pi}{2}\\right)\$\$
\$\$\\log\\tan\\frac{x}{2}=-2\\sum\_{n=1}^{\\infty}\\frac{\\cos(2n+1)x}{2n+1}\\quad\\left(0\< x\<\\frac{\\pi}{2}\\right)\$\$
çŽæ°å±éã䜿ã£ãŠè§£ããŠèŠãŸãããã
\\begin{align} I&=\\int\_{0}^{1}\\frac{\\log(1+x)}{\\sqrt{x}}dx \\\\&=-\\int\_{0}^{1}\\sum\_{n=1}^{\\infty}\\frac{(-1)^n\\ x^n}{n\\ \\sqrt{x}}dx \\\\&=-\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n}\\int\_{0}^{1}x^{n-\\frac{1}{2}}\\ dx \\\\&=-2\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n(2n+1)} \\\\&=-2\\left(\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n}-2\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{2n+1}\\right) \\\\&=-2\\left(\\log2+\\frac{\\pi}{2}-2\\right) \\\\&=-2\\log2-\\pi+4 \\end{align}
æ®éã«éšåç©åã§ãè§£ããŸãã
\\begin{align} I&=\\int\_{0}^{\\frac{\\pi}{2}}\\log\\left(2\\sin\\frac{x}{2}\\right)\\log\\left(2\\cos\\frac{x}{2}\\right)dx \\\\&=\\frac{1}{2}\\int\_{0}^{\\pi}\\log\\left(2\\sin\\frac{x}{2}\\right)\\log\\left(2\\cos\\frac{x}{2}\\right)dx \\\\&=\\frac{1}{2}\\sum\_{n,m\>0}\\frac{(-1)^n}{nm}\\int\_{0}^{\\pi}\\cos mx\\cos nx dx \\\\&=\\frac{\\pi}{4}\\sum\_{n=1}^{\\infty}\\frac{(-1)^n}{n^2} \\\\&=-\\frac{\\pi^3}{48} \\end{align}
éã§ããèš±ããŠãã ããã
[åã®èšäº](https://mathlog.info/articles/nFkkmCBNuFHtPOyrFUSk) ã§å¥ã®æ¹æ³ã§è§£ããŠãŸãã
### 埮å
\$\\displaystyle\\frac{d}{ds}x^s=x^s\\log x\$ã䜿ã£ãŠç©åãè§£ããããšããããŸãã
\\begin{align} I&=\\int\_{0}^{\\infty}e^{-x}\\log xdx \\\\&=\\left.\\frac{d}{ds}\\int\_{0}^{\\infty}x^s e^{-x}dx\\right\|\_{s=1} \\\\&=\\Gamma'(1) \\\\&=\\Gamma(1)\\psi(1) \\\\&=-\\gamma \\end{align}
埮åãšç©åã®äº€æã䜿ããŸããã
\$\$I=\\int\_{0}^{1}\\frac{x^2-x}{\\log x}dx\$\$
\$\$f(t)=\\int\_{0}^{1}\\frac{x^t}{\\log x}\$\$
\\begin{align} f'(t)&=\\int\_{0}^{1}x^t \\\\&=\\frac{1}{t+1} \\end{align}
\\begin{align} f(2)-f(1)&=\\int\_{1}^{2}f'(t)dt \\\\&=\\int\_{1}^{2}\\frac{1}{t+1}dt \\\\&=\\log\\frac{3}{2} \\end{align}
ãã®è§£æ³ãããªã奜ãã§ãã
### è€çŽ ç©å
è€çŽ ç©åã§è§£ããããšããã£ããããã
ããããæžããŠãè€çŽ ç©åã®2ã€ã®èšäºã¯ã©ã£ã¡ã\$\\log\$ãããã®ã§ãã¡ããã¿ãŠã»ããã( [ãã](https://mathlog.info/articles/dGB4ngusgBuBJM1K6rG6) ãš [ãã](https://mathlog.info/articles/uqiFFCC5kXHH58DYZkks) )
被ç©å颿°ã«\$\\log x\$ã ã£ããããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã§è§£ããŠããããšãå€ãæ°ãããŸãã
ããŒã ã¯ãŒãã³ã®ãããªçµè·¯ã¯åã®èšäºã§ãã£ãŠããã
\$\$I=\\int\_{0}^{\\infty}\\frac{x\\log x}{x^4+1}dx\$\$
\$\$f(z)=\\frac{z\\log z}{z^4+1}\$\$
 ç©åçµè·¯
\$\\log0\$ãåé¿ããããã«\$0\$ã¯é¿ããŠããŸãã
\$\\displaystyle C\_2,C\_4\$ã¯è©äŸ¡ããŠæ¥µéãšã°ããš\$0\$ã«ãªããŸãã
確èªããŠã¿ãŠãã ããã
å
šäœã®ç©åã\$C\$ãšããŠãããŸãã
ããããèšç®ããŠãããŸãã
\\begin{align} \\int\_{C\_1}&=\\int\_{\\varepsilon}^{R}f(z)dz \\\\&=I\\qquad(\\ip\\to0,R\\to\\infty) \\end{align}
\\begin{align} \\int\_{C\_3}&=\\int\_{iR}^{i\\ip}f(z)dz \\\\&=-i\\int\_{\\ip}^{R}f(ix)dx \\\\&=\\int\_{\\ip}^{R}\\frac{x\\log ix}{x^4+1}dx \\\\&=\\int\_{\\ip}^{R}\\frac{x\\log x}{x^4+1}dx+\\frac{i\\pi}{2}\\int\_{\\ip}^{R}\\frac{x}{x^4+1}dx \\\\&=I+\\frac{\\pi^2}{8}i\\qquad(\\ip\\to0,R\\to\\infty) \\end{align}
\\begin{align} \\oint\_{C}&=2\\pi i\\underset{z=e^{\\frac{i\\pi}{4}}}{\\mathrm{Res}}\\frac{z\\log z}{z^4+1} \\\\&=2\\pi i\\lim\_{z\\to e^{\\frac{i\\pi}{4}}}\\frac{z\\log z(z-e^{\\frac{i\\pi}{4}})}{z^4+1} \\\\&=2\\pi i\\lim\_{z\\to e^{\\frac{i\\pi}{4}}}\\frac{(2z-e^{\\frac{i\\pi}{4}})\\log z-e^{\\frac{i\\pi}{4}}+z}{4z^3} \\\\&=\\frac{\\pi^2}{8}i \\end{align}
\$\$\\oint\_{C}=\\int\_{C\_{1}}+\\int\_{C\_{2}}+\\int\_{C\_{3}}+\\int\_{C\_{4}}\$\$
\$\$\\frac{\\pi^2}{8}i=I+I+\\frac{\\pi^2}{8}i\$\$
\$\$I=0\$\$
埮åã䜿ã£ãŠãè§£ããŸãã
被ç©å颿°ã®\$\\log x\$ã®ææ°ã«\$1\$ãè¶³ããŠ\$f(z)\$ãèšå®ããããšããããŸãã
ãããŸãŒã |
| Shard | 46 (laksa) |
| Root Hash | 792424158193528446 |
| Unparsed URL | info,mathlog!/articles/eD5JeKj6fR5nUna80ejj s443 |