
==> $\frac{{{K_1}A({\theta _A} - {\theta _C})}}{l} = \frac{{{K_2}A({\theta _C} - {\theta _B})}}{l}$
==> $\frac{{{\theta _A} - {\theta _C}}}{{{\theta _C} - {\theta _B}}} = \frac{{{K_2}}}{{{K_1}}}$...$(i)$
Also ${\left( {\frac{Q}{t}} \right)_{AD}} = {\left( {\frac{Q}{t}} \right)_{DB}}$
==>$\frac{{{K_3}A({\theta _A} - {\theta _D})}}{l} = \frac{{{K_4}A({\theta _D} - {\theta _B})}}{l}$
==>$\frac{{{\theta _A} - {\theta _D}}}{{{\theta _D} - {\theta _B}}} = \frac{{{K_4}}}{{{K_3}}}$ ...$(ii)$
It is given that ${\theta _C} = {\theta _D},$ hence from equation $(i)$ and $(ii)$ we get $\frac{{{K_2}}}{{{K_1}}} = \frac{{{K_4}}}{{{K_3}}}$
==> ${K_1}{K_4} = {K_2}{K_3}$
(Take Stefan-Boltzmann constant $=5.67 \times 10^{-8} Wm ^{-2} K ^{-4}$, Wien's displacement constant $=2.90 \times 10^{-3} m - K$, Planck's constant $=6.63 \times 10^{-34} Js$, speed of light in vacuum $=3.00 \times 10^8 ms ^{-1}$ )-
$(A)$ power radiated by the filament is in the range $642 W$ to $645 W$
$(B)$ radiated power entering into one eye of the observer is in the range $3.15 \times 10^{-8} W$ to $3.25 \times 10^{-8} W$
$(C)$ the wavelength corresponding to the maximum intensity of light is $1160 nm$
$(D)$ taking the average wavelength of emitted radiation to be $1740 nm$, the total number of photons entering per second into one eye of the observer is in the range $2.75 \times 10^{11}$ to $2.85 \times 10^{11}$




