Heat flow from $$B$$ to $$A, A$$ to $$C$$ and $$C$$ to $$B$$ (for steady state condition, $$\frac{{DQ}}{{Dt}}$$ is same)
Where, $$\frac{{\Delta Q}}{{\Delta t}} = \frac{{k\,A\,\Delta T}}{\ell }$$
For sides $$AC$$ and $$CB{\left( {\frac{{\Delta T}}{{\sqrt 2\, a}}} \right)_{AC}}$$
$$ = {\left( {\frac{{\Delta T}}{a}} \right)_{CB}}$$

$$\eqalign{
& \Rightarrow \,\,\frac{{T - {T_c}}}{{\sqrt 2\, a}} = \frac{{{T_c} - \sqrt 2\, T}}{a} \cr
& \Rightarrow \,\,T - {T_c} = \sqrt 2 \,{T_c} - 2\,T \cr
& \Rightarrow \,\,3\,T = {T_c}\left( {\sqrt 2 + 1} \right) \cr
& \Rightarrow \,\,\frac{{{T_c}}}{T} = \frac{3}{{\sqrt 2 + 1}} \cr} $$