EQUAÇÕES GRACELI [15]

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ S [x] = sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ C [ x] = cos [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ $dx=C'(t)dt=\cos(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ $dy=S'(t)dt=\sin(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ S [x] = sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ C [ x] = cos [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ $dx=C'(t)dt=\cos(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ $dy=S'(t)dt=\sin(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ S [x] = sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ C [ x] = cos [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ $dx=C'(t)dt=\cos(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ $dy=S'(t)dt=\sin(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ S [x] = sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ C [ x] = cos [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ $dx=C'(t)dt=\cos(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-(x+b)^{2}/c^{2}}\,dx=c{\sqrt {\pi }}.$ $dy=S'(t)dt=\sin(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ S [x] = sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ C [ x] = cos [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ $dx=C'(t)dt=\cos(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ $dy=S'(t)dt=\sin(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ S [x] = sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ C [ x] = cos [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ $dx=C'(t)dt=\cos(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

$\int _{-\infty }^{\infty }e^{-x^{2}+bx+c}\,dx={\sqrt {\pi }}\,e^{b^{2}/4+c},$ $dy=S'(t)dt=\sin(t^{2})dt\,$ sin [ ${\frac {\pi }{2}}t^{2}$ ] dt $[pk] n!, ] [$ $\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}$ $\zeta (s)$ / [ $\pi$ / pk]

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EQUAÇÕES GRACELI [15]

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