(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 $2.85 \times 10^{11}$
Point source $d =100 m$
$R_c=3 mm$
$(A)$ $P =\sigma AeT ^4$
$=5.67 \times 10^{-3} \times 64 \times 10^{-6} \times 1 \times(2500)^4(e=1 \text { black body })$
$=141.75 w$
Option $(A)$ is wrong
$(B)$ Power reaching to the eye
$=\frac{ P }{4 \pi d ^2} \times\left(\pi R _e^2\right)$
$=\frac{141.75}{4 \pi \times(100)^2} \times \pi \times\left(3 \times 10^{-1}\right)^2$
$=3.189375 \times 10^{-8} W$
Option $(B)$ is correct
$(C)$
$\lambda_{ m } T = b$
$\lambda_{ m } \times 2500=2.9 \times 10^{-3}$
$\Rightarrow \lambda_{ m } =1.16 \times 10^{-6}$
$ =1160 mm$
Option $(C)$ is correct
$(D)$ Power received by one eye of observer $=\left(\frac{ hc }{\lambda}\right) \times \dot{ N }$
$\dot{ N }=\text { Number of photons entering into eye per second }$
$\Rightarrow 3.189375 \times 10^{-8}$
$=\frac{6.63 \times 10^{-34} \times 3 \times 10^x}{1740 \times 10^{-9}} \times \dot{N}$
$\Rightarrow \dot{N}=2.79 \times 10^{11}$

$(A)$ heat flow through $A$ and $E$ slabs are same.
$(B)$ heat flow through slab $E$ is maximum.
$(C)$ temperature difference across slab $E$ is smallest.
$(D)$ heat flow through $C =$ heat flow through $B +$ heat flow through $D$.