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\begin{align}
  & \frac{d{{s}^{2}}{{|}_{{{{\bar{x}}}^{0}}+\delta {{{\bar{x}}}^{0}}=\text{const}}}}{d{{s}^{2}}{{|}_{{{{\bar{x}}}^{0}}=\text{const}}}}=1+\delta {{{\bar{x}}}^{0}}h\left( {{{\bar{x}}}^{0}} \right)+O\left( {{\left( \delta {{{\bar{x}}}^{0}} \right)}^{2}} \right) \\ 
 & \Rightarrow {{g}_{ik}}\left( {{{\bar{x}}}^{0}},{{x}^{k}} \right)={{S}^{2}}\left( {{{\bar{x}}}^{0}} \right){{\gamma }_{ij}}\left( {{x}^{k}} \right) \\ 
 & \Rightarrow d{{s}^{2}}={{\left( d{{{\bar{x}}}^{0}} \right)}^{2}}+{{S}^{2}}\left( {{{\bar{x}}}^{0}} \right){{\gamma }_{ij}}\left( {{x}^{k}} \right) \\ 
\end{align}

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ds2|x¯0+δx¯0=constds2|x¯0=const=1+δx¯0h(x¯0)+O((δx¯0)2)gik(x¯0,xk)=S2(x¯0)γij(xk)ds2=(dx¯0)2+S2(x¯0)γij(xk)
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