INTEGRAIS COMPLEXAS E DE SUPERFÍCIE DE ANCELMO LUIZ GRACELI [2]

INTEGRAIS DE ANCELMO GRACELI

p = progressão.

$G_{\mu \nu }\$ = tensor de Graceli

[Gn] número de Ancelmo l. Graceli = 1/ p [3] = 1 dividido por progressão geométrica de 3.

INTEGRAIS DE ANCELMO GRACELI

p = progressão.

[-] p $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = Z [e - ${\frac {\sin t}{t}}.$ ] $S$ [ $\Gamma (z)$ sin $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ } $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = [-/] $S$ } [-/] $S$ } Z [e - ${\frac {\sin t}{t}}.$ ][ $\Gamma (z)$ Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = [ $\Gamma (z)$ Z [e - ${\frac {\sin t}{t}}.$ ] [ $\Gamma (z)$ $S$ sin $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $G_{\mu \nu }\$ [-] $S$ $G_{\mu \nu }\$ $d\sigma$ d $G_{\mu \nu }\$ d $S$

p = progressão.

$G_{\mu \nu }\$ = número de Ancelmo l. Graceli = 1/ p [3] = 1 dividido por progressão geométrica de 3.

[-] p $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = Z [e - ${\frac {\sin t}{t}}.$ ] $S$ sin $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = Z [e - ${\frac {\sin t}{t}}.$ ] [ $\Gamma (z)$ $d\sigma$ d $G_{\mu \nu }\$

p = progressão.

$G_{\mu \nu }\$ = número de Ancelmo l. Graceli = 1/ p [3] = 1 dividido por progressão geométrica de 3.

[-] p $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ Z [e - ${\frac {\sin t}{t}}.$ ] = $S$ sin Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ [-/] $S$ } = Z [e - ${\frac {\sin t}{t}}.$ ] Z [e - ${\frac {\sin t}{t}}.$ ] $S$ sin $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = z [-] $S$ $G_{\mu \nu }\$ Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $G_{\mu \nu }\$ Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d $G_{\mu \nu }\$ d $S$

[-] $S$

G = { $f$ [ $\Gamma (z)$ Z [e - ${\frac {\sin t}{t}}.$ ]} = [-] $S$ $G_{\mu \nu }\$ z [-] $S$ $G_{\mu \nu }\$ z $S$ sinz $d\sigma$ d $G_{\mu \nu }\$ d $S$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = cos Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $G_{\mu \nu }\$ z cos Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $G_{\mu \nu }\$ z $S$ sinz $d\sigma$ d $G_{\mu \nu }\$ d $S$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = COS Z [e - ${\frac {\sin t}{t}}.$ ] Z [e - $S$ sinZ [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ } $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = [-/] $S$ } [-/] $S$ } COS $S$ sin Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = COS $S$ sin Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ dT

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = [-] COS Z [e - ${\frac {\sin t}{t}}.$ ] $S$ $G_{\mu \nu }\$ COS Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $G_{\mu \nu }\$ $S$ sin $d\sigma$ d $G_{\mu \nu }\$ d $S$

p = progressão.

$G_{\mu \nu }\$ = número de Ancelmo l. Graceli = 1/ p [3] = 1 dividido por progressão geométrica de 3.

[-] p $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = $S$ Z [e - ${\frac {\sin t}{t}}.$ ] sin $d\sigma$ d T

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = Z [e - ${\frac {\sin t}{t}}.$ ] Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $\Gamma (z)$

p = progressão.

$G_{\mu \nu }\$ = número de Ancelmo l. Graceli = 1/ p [3] = 1 dividido por progressão geométrica de 3.

[-] p $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = $S$ sinZ [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d $G_{\mu \nu }\$

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = [-] $S$ sin Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ dT

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = z [-] $S$ $G_{\mu \nu }\$ Z [e - ${\frac {\sin t}{t}}.$ ] [-] $S$ $G_{\mu \nu }\$ $S$ Z [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ dT

[-] $S$ $G_{\mu \nu }\$

G = { $f$ [c [-/] $S$ } = [-] $S$ $G_{\mu \nu }\$ z [-] $S$ $G_{\mu \nu }\$ zZ [e - ${\frac {\sin t}{t}}.$ ] $S$ sinz $d\sigma$ d T d $S$

G = { $f$ [ $\Gamma (z)$ [-/] $S$ } = cos [-] Z [e - ${\frac {\sin t}{t}}.$ ] $S$ $G_{\mu \nu }\$ z cos [-] Z [e - ${\frac {\sin t}{t}}.$ ] $S$ $G_{\mu \nu }\$ $S$ sinZ [e - ${\frac {\sin t}{t}}.$ ] $d\sigma$ d Z [e - ${\frac {\sin t}{t}}.$ ] d $S$

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INTEGRAIS COMPLEXAS E DE SUPERFÍCIE DE ANCELMO LUIZ GRACELI [2]

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