EQUAÇÕES GRACELI [21]

INTEGRAL DE GRACELI.

S [x] = A sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . dt + S [x] = B sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

C [x] = A cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . dt + C [x] = B cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

S [x] = A sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ dt + S [x] = Bsin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

C [x] = Acos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ dt + C [x] = B cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

S [x] = A sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ dt + S [x] = B sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

C [x] = Acos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ dt + C [x] = Bcos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

S [x] = A sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\zeta (s)$ dt + S [x] = B sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\zeta (s)$ ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

C [x] = A cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ $e^{-{\frac {1}{2}}t^{2}}$ . $\zeta (s)$ dt + C [x] = Bcos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ $e^{-{\frac {1}{2}}t^{2}}$ . $\zeta (s)$ ${\sqrt {\frac {2}{\pi }}}$ [[ $n!,] / PK]$ dt

INTEGRAL DE GRACELI.

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . [[ $n!,] / PK]$ $\Gamma (z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . [[ $n!,] / PK]$ $\Gamma (z)$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ [[ $n!,] / PK]$ $\Gamma (z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ [[ $n!,] / PK]$ $\Gamma (z)$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ [[ $n!,] / PK]$ $\Gamma (z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ [[ $n!,] / PK]$ $\Gamma (z)$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\zeta (s)$ [[ $n!,] / PK]$ $\Gamma (z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ $e^{-{\frac {1}{2}}t^{2}}$ . $\zeta (s)$ [[ $n!,] / PK]$ $\Gamma (z)$ dt

INTEGRAL DE GRACELI.

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\psi _{n}(z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\psi _{n}(z)$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ $\psi _{n}(z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ $\psi _{n}(z)$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\psi _{n}(z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\psi _{n}(z)$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\zeta (s)$ $\psi _{n}(z)$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ $e^{-{\frac {1}{2}}t^{2}}$ . $\zeta (s)$ $\psi _{n}(z)$ dt

INTEGRAL DE GRACELI.

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $B_{n}$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $B_{n}$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ $B_{n}$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $\zeta (s)$ $B_{n}$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $B_{n}$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $E_{n}$ dt

S [x] = sin [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ . $e^{-{\frac {1}{2}}t^{2}}$ $\zeta (s)$ $E_{n}$ dt

C [x] = cos [[ $n!,$ ${\frac {\pi }{2}}t^{2}$ ] $({\frac {\pi }{2}})^{1/2}$ $e^{-{\frac {1}{2}}t^{2}}$ . $\zeta (s)$ $E_{n}$ dt

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EQUAÇÕES GRACELI [21]

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