Note: The original, more step-by-step approach is below the line.
Notations used in this answer:
\begin{align}
S_r&=\sum_{1\le i \le 6}{x_i^r}\\
e_r&=\displaystyle{\sum_{{{1\le \underbrace{i\le j \le k \le \ldots}_{\displaystyle{{r \text{ indices}}}}} \le 6}}}\underbrace{x_ix_jx_k\cdots x_{\dots}}_{r \text{ factors}}\\
e_1&=x_1+\dots+x_6\\
e_2&=x_1x_2+x_1x_3+\dots+x_2x_3+\dots+x_5x_6\\
e_6&=x_1x_2\cdots x_6\\
\left(e_r\right)_{r>6}&=0
\end{align}
Identities: refer to Newton's identities
\end{align}
The 'one-shot' proof:
\begin{align}
& \frac{{{S}_{7}}}{{{S}_{2}}{{S}_{5}}}=\frac{\overbrace{{{e}_{1}}}^{={{S}_{1}}=0}{{S}_{6}}-{{e}_{2}}{{S}_{5}}+{{e}_{3}}{{S}_{4}}-{{e}_{4}}\overbrace{{{S}_{3}}}^{=0}+{{e}_{5}}{{S}_{2}}-{{e}_{6}}\overbrace{{{S}_{1}}}^{=0}+7\overbrace{{{e}_{7}}}^{=0}}{\left( \underbrace{{{e}_{1}}}_{=0}\underbrace{{{S}_{1}}}_{=0}-2{{e}_{2}} \right)\left( \underbrace{{{e}_{1}}}_{=0}{{S}_{4}}-{{e}_{2}}\underbrace{{{S}_{3}}}_{=0}+{{e}_{3}}{{S}_{2}}-{{e}_{4}}\underbrace{{{S}_{1}}}_{=0}+5{{e}_{5}} \right)} \\
& =\frac{-{{e}_{2}}{{S}_{5}}+{{e}_{3}}{{S}_{4}}+{{e}_{5}}{{S}_{2}}}{\left( -2{{e}_{2}} \right)\left( {{e}_{3}}{{S}_{2}}+5{{e}_{5}} \right)} \\
& =\frac{-{{e}_{2}}{{S}_{5}}+0\cdot {{S}_{4}}+{{e}_{5}}{{S}_{2}}}{\left( -2{{e}_{2}} \right)\left( 0\cdot {{S}_{2}}+5{{e}_{5}} \right)}\qquad\qquad\qquad\because 3{{e}_{2}}={{e}_{2}}\underbrace{{{S}_{1}}}_{=0}-\underbrace{{{e}_{1}}}_{=0}{{S}_{2}}+\underbrace{{{S}_{3}}}_{=0}=0 \\
& =\frac{-{{e}_{2}}{{S}_{5}}+{{e}_{5}}{{S}_{2}}}{\left( -2{{e}_{2}} \right)\left( 5{{e}_{5}} \right)} \\
& =\frac{-\frac{1}{2}\left( {{e}_{1}}{{S}_{1}}-{{S}_{2}} \right){{S}_{5}}+{{e}_{5}}{{S}_{2}}}{\left( -2\left( {{e}_{1}}{{S}_{1}}-{{S}_{2}} \right) \right)\left( 5{{e}_{5}} \right)}\qquad\qquad\qquad\because 2{{e}_{2}}=\underbrace{{{e}_{1}}{{S}_{1}}}_{=0}-{{S}_{2}}\Rightarrow {{S}_{2}}=-\frac{1}{2}{{e}_{2}} \\
& =\frac{\frac{1}{2}{{S}_{2}}{{S}_{5}}+{{e}_{5}}{{S}_{2}}}{5{{e}_{5}}{{S}_{2}}} \\
& =\frac{{{S}_{5}}+2{{e}_{5}}}{10{{e}_{5}}}\qquad\qquad\because 5{{e}_{5}}={{e}_{4}}\underbrace{{{S}_{1}}}_{=0}-\underbrace{{{e}_{3}}}_{=0}{{S}_{2}}+{{e}_{2}}\underbrace{{{S}_{3}}}_{=0}-\underbrace{{{e}_{1}}}_{=0}{{S}_{4}}+{{S}_{5}}\Rightarrow {{S}_{5}}=5{{e}_{5}} \\
& =\frac{5{{e}_{5}}+2{{e}_{5}}}{10{{e}_{5}}} \\
& =\frac{7}{10}
\end{align}
Consider
\begin{align}
\sum_{1\le i\le6}{x^2_i}
&=\left(\sum_{1\le i\le6}{x_i}\right)^2
-2(\underbrace{x_1x_2+x_2x_3+\ldots+x_5x_6}_\text{all permuations of pairs})\\
&=0-2(\underbrace{x_1x_2+x_2x_3+\ldots+x_5x_6}_\text{all permuations of pairs})\\
\frac12S_2&=-\sum_{1\le i\le j \le6}{x_ix_j}=-e_2
\end{align}
Using Newton's identities (which you can sort of observe yourself also)
\begin{align}
S_5
&=\underbrace{\left(\sum_{1\le i\le6}{x_i}\right)}_{=0}S_4
-\left(\overbrace{\sum_{1\le i\le j\le6}{x_ix_j}}^{e_2}\right)\underbrace{S_3}_{=0}
+\left(\overbrace{\sum_{1\le i\le j\le k \le6}{x_ix_jx_k}}^{e_3}\right)S_2
-\left(\overbrace{\sum_{1\le i\le j\le k \le k \le 6}{x_ix_jx_kx_l}}^{e_4}\right)\underbrace{S_1}_{=0}+e_5\\
&=0-0+e_3S_2-0\\
&=e_3S_2+5e_5
\end{align}
and
\begin{align}
S_7
&=\underbrace{e_1}_{=S_1=0}S_6
-e_2S_5
+e_3S_4
-e_4S_3
+e_5S_2-e_6S_1+7\underbrace{e_7}_{=0}\\
&=-e_2S_5
+e_3S_4
+e_5S_2\\
\end{align}
Then we settle some unfinished business with our dear $e_3$,
\begin{align}
S_3&=e_1S_2-e_2S_1+3e_3\\
0&=0-0+3e_3\\
e_3&=0
\end{align}
so we have
\begin{align}
S_5&=e_3S_2+5e_5\\
S_5&=0+5e_5\\
e_5&=\frac{1}{5}S_5
\end{align}
and
\begin{align}
S_7
&=-e_2S_5+e_3S_4+e_5S_2\\
&=\frac12S_2S_5+0+\frac15S_2S_5\\
&=\frac7{10}S_2S_5
\end{align}