EQUAÇÕES DE GRACELI

janeiro 29, 2023

[ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\Vert f\Vert _{L^{2}(-\pi ,\pi )}^{2}=\int _{-\pi }^{\pi }|f(x)|^{2}\,dx=2\pi \sum _{n=-\infty }^{\infty }|c_{n}|^{2}$ [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\mid \mid f\mid \mid ^{2}={\frac {1}{\pi }}\int _{-\pi }^{\pi }f(x)^{2}dx={\frac {A_{0}}{2}}+\textstyle \sum _{k=1}^{\infty }\displaystyle (a_{k}^{2}+b_{k}^{2})$ [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

${\frac {f(x_{o}^{+})+f(x_{o}^{-})}{2}}$ [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$f(x)={\frac {A_{0}}{2}}+\textstyle \sum _{k=1}^{\infty }\displaystyle (A_{k}\cos(kx)+B_{k}\operatorname {sen}(kx))$ [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\lim _{N\to \infty }||f-\textstyle \sum _{k=1}^{\infty }\displaystyle (A_{k}\cos(kx)+B_{k}\operatorname {sen}(kx))||\longrightarrow C$ [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

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EQUAÇÕES DE GRACELI

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