CÁLCULO GRACELI SINTÉTICO [85]

f [x] = ω ${\frac {1}{2\pi }}F(\omega )$ , $O(t)\;=\;Ae^{2\pi ft\;+\;\phi }$ . ${\frac {\omega }{2\pi }}$ . dω =

f [x] = ω ${\frac {1}{2\pi }}F(\omega )$ , $O(t)\;=\;Ae^{2\pi ft\;+\;\phi }$ . ${\frac {\omega }{2\pi }}$ . $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ dω =

G[x] [ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

G[x] [ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ [ e $({\frac {\pi }{2}})^{1/2}$ .] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

G[x] [ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ [ e [ ${\sqrt {\frac {2}{\pi }}}$ e] .] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

G[x] [ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ [ e ${\frac {\pi }{2}}t^{2}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

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

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

$\int _{-\infty }^{\infty }e^{-x^{2}}\,dx={\sqrt {\pi }}.$ [ e $({\frac {\pi }{2}})^{1/2}$ .]

$f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] = A COS .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\zeta (s)$ + B SEN $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\zeta (s)$ =

G [ $\zeta (s)$ ] = [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

G [ $\zeta (s)$ ] = [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $E_{n}$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] =

G [ $\zeta (s)$ ] = [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\Gamma (z)$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

G [ $\zeta (s)$ ] = [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\psi _{n}(z)$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

G [ $\zeta (s)$ ] = [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\operatorname {Li} _{s}(z)$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] =

FUNÇÃO SINC GRACELI.

$\operatorname {sinc} (x)={\frac {\sin(\pi x)}{\pi x}}.\,\!$ /[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] =

$\operatorname {sinc} (x)={\frac {\sin(x)}{x}}.\,\!$ [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

INTEGRAL GRACELI.

S [x] sin /[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] dt =

C [x] cos /[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]dt =

G [ $\zeta (s)$ ] = [A, B , C] [SEN, COS] [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] =

G [ $\zeta (s)$ ] = [A, B , C] [SEN, COS] [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $E_{n}$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

G [ $\zeta (s)$ ] = [A, B , C] [SEN, COS] [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\Gamma (z)$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

G [ $\zeta (s)$ ] = [A, B , C] [SEN, COS] [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\psi _{n}(z)$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

G [ $\zeta (s)$ ] = [A, B , C] [SEN, COS] [ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .] $\operatorname {Li} _{s}(z)$ $\zeta (s)$ $f(x)=A(e^{{ix}})$ .[ ${\frac {\pi }{2}}t^{2}$ ] [ ${\sqrt {\frac {2}{\pi }}}$ e] [ e $({\frac {\pi }{2}})^{1/2}$ .]=

FUNÇÃO SINC GRACELI.

INTEGRAL GRACELI.

Pesquisar este blog

CÁLCULO GRACELI SINTÉTICO [85]

Comentários

Postar um comentário

Postagens mais visitadas deste blog