SUPERFÍCIE E TORO - GEOMETRIA TOROIDAL DE ANCELMO L. GRACELI.

julho 17, 2026

G {F [f]} = $e /$ [e - ${\frac {\sin t}{t}}.$ ] F [t] dt

G {F [f]} = $e /$ [e - ${\frac {\sin t}{t}}.$ ] / t F [t] dt

G {F [f]} = $e /$ [e - ${\frac {\sin t}{t}}.$ ] / e F [t] dt

G {F [f]} = $e /$ [e - [ $e^{-{\frac {z}{\delta }}}$ /s ]] F [t] dt

G {F [f]} = $e /$ [e - [ $e^{-{\frac {z}{\delta }}}$ /s z]] / e F [t] dt

G {F [f]} = $e /$ [e - ${\frac {\sin t}{t}}.$ / sz] F [t] dt

G {F [f]} = $e /$ [e - ${\frac {\sin t}{t}}.$ / sz] / t F [t] dt

G {F [f]} = $e /$ [e - ${\frac {\sin t}{t}}.$ ] / e F [t] dt

G {F [f]} = $e /$ [e - [ $e^{-{\frac {z}{\delta }}}$ ]] F [t] dt

G {F [f]} = $e /$ [e - [ $e^{-{\frac {z}{\delta }}}$ ]] / e F [t] dt

$ds / dz =$ $cos$ [ $\psi$ ] [ $e^{-{\frac {z}{\delta }}}$ ][e - ${\frac {\sin t}{t}}.$ ] dz, ds.

$ds / dz =$ $cos$ [ $\psi$ ] [ $e^{-{\frac {z}{\delta }}}$ ][e - ${\frac {\sin t}{t}}.$ ] sin $\Psi _{n}$ $\phi (x)$ S [ $\psi$ ] dz, ds.

$ds / dz =$ $cos$ [ $\psi$ ] [ $e^{-{\frac {z}{\delta }}}$ ][e - ${\frac {\sin t}{t}}.$ ] sin $\Psi _{n}$ $\phi (x)$ [ $e^{-{\frac {z}{\delta }}}$ ] S [ $\psi$ ] dz, ds.

$ds / dz =$ $\phi (x)$ [ $e^{-{\frac {z}{\delta }}}$ ] $cos$ [ $\psi$ ] [ $e^{-{\frac {z}{\delta }}}$ ][e - ${\frac {\sin t}{t}}.$ ] sin $\Psi _{n}$ $\phi (x)$ [ $e^{-{\frac {z}{\delta }}}$ ] S [ $\psi$ ] dz, ds.

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SUPERFÍCIE E TORO - GEOMETRIA TOROIDAL DE ANCELMO L. GRACELI.

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