EQUAÇÃO GRACELI [31]

fevereiro 12, 2023

L G [x,s] = $\delta$ [- $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] [s] =

L u [x] = f [- $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)]] =

L G [x,s] = $\delta$ - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)]=

L G [x,s] = $\delta$ [- $\Gamma (z)$ [x - [ $\Phi \,\!$ , (λ)] [s] =

L u [x] = f [- $\Gamma (z)$ [x - [ $\Phi \,\!$ , (λ)]] =

L G [x,s] = $\delta$ - $\Gamma (z)$ [x - [ $\Phi \,\!$ , (λ)]=

L G [x,s] = $\delta$ [- $\psi _{n}(z)$ [x - [ $\Phi \,\!$ , (λ)] [s] =

L u [x] = f [- $\psi _{n}(z)$ [x - [ $\Phi \,\!$ , (λ)]] =

L G [x,s] = $\delta$ - $\psi _{n}(z)$ [x - [ $\Phi \,\!$ , (λ)]=

L G [x,s] = $\delta$ [- $\operatorname {Li} _{s}(z)$ [x - [ $\Phi \,\!$ , (λ)] [s] =

L u [x] = f [- $\operatorname {Li} _{s}(z)$ [x - [ $\Phi \,\!$ , (λ)]] =

L G [x,s] = $\delta$ - $\operatorname {Li} _{s}(z)$ [x - [ $\Phi \,\!$ , (λ)]=

f [t] [ $\Phi \,\!$ , (λ)] = ${\frac {\pi }{2}}t^{2}$ [[t] [ $\Phi \,\!$ , (λ)] - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] / $(n-1)!={\frac {n!}{n}}$

[x [t] f [t] [ $\Phi \,\!$ , (λ)] [f[t] + ${\frac {\pi }{2}}t^{2}$ [[t] [ $\Phi \,\!$ , (λ)] - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] / $(n-1)!={\frac {n!}{n}}$

[x [t] f [t] [ $\Phi \,\!$ , (λ)] [f[t] + ${\frac {\pi }{2}}t^{2}$ [[t] [ - ] [ $\Phi \,\!$ , (λ)] - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] / $(n-1)!={\frac {n!}{n}}$

f [t] [ $\Phi \,\!$ , (λ)] = cos ${\frac {\pi }{2}}t^{2}$ [[t] [ $\Phi \,\!$ , (λ)] - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] / $(n-1)!={\frac {n!}{n}}$

[x [t] f [t] [ $\Phi \,\!$ , (λ)] [f[t] + cos ${\frac {\pi }{2}}t^{2}$ [[t] [ $\Phi \,\!$ , (λ)] - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] / $(n-1)!={\frac {n!}{n}}$

[x [t] f [t] [ $\Phi \,\!$ , (λ)] [f[t] + cos ${\frac {\pi }{2}}t^{2}$ [[t] [ - ] [ $\Phi \,\!$ , (λ)] - $\zeta (s)$ [x - [ $\Phi \,\!$ , (λ)] / $(n-1)!={\frac {n!}{n}}$

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EQUAÇÃO GRACELI [31]

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