We have given that "L_1 \\& L_2" are equation of line whose direction cosines are given as "(l_1,m_1,n_1) \\& (l_2,m_2,n_2)" respectively obtained from solution of two given equation as follows,
where "abc \\neq 0" ,also given that "L_1 \\bot L_2 \\implies l_1l_2+m_1m_2+n_1n_2=0 \\: (\\star)" .
Let's eliminate one of the variable from "(1)" ,say "l" ,thus "l=-\\frac{bm+cn}{a}" and substitute to "(2)" we get,
where
"y=\\frac{m}{n}"Clearly, equation "(\\clubs)" is quadratic in "y" ,hence by relation between roots and coefficients(Vieta's Theorem) we get,
Hence,from equation "(4)" ,
"\\frac{m_1}{n_1}\\frac{m_2}{n_2}=\\frac{gc}{hb}\\\\\n\\implies \\frac{m_1m_2}{\\frac{g}{b}}=\\frac{n_1n_2}{\\frac{h}{c}} \\hspace{1cm}(5)"In the same manner if we eliminate other two variables "n ,m" (say "n" ) and do the same calculation as above we get,
"\\frac{m_1m_2}{\\frac{g}{b}}=\\frac{l_1l_2}{\\frac{f}{a}} \\hspace{1cm}(6)"
Now from equation "5" and "6" we finally get
Thus from equation "7" if we consider "\\frac{m_1m_2}{\\frac{g}{b}}=\\frac{l_1l_2}{\\frac{f}{a}} =\\frac{n_1n_2}{\\frac{h}{c}}=p" ,clearly "p \\neq 0" ,hence,
but from equation "(\\star)" we get,
Therefore we are done.
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