
$=\left(\frac{(\mathrm{KA}) \Delta \mathrm{T}}{3 \ell}+\frac{\left(\mathrm{K}^{\prime}\right) \mathrm{A} \Delta \mathrm{T}}{\ell}\right)$
$\frac{4 \mathrm{K}}{3} \times 2=\frac{\mathrm{K}}{3}+\mathrm{K}^{\prime}$
$K^{\prime}=\frac{7 K}{3}$
$(A)$ 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 $D$.
[$A$] The amount of energy radiated by the body in $1$ second is close to $60$ Joules.
[$B$] If the surrounding temperature reduces by a small amount $\Delta \mathrm{T}_0<<\mathrm{T}_0$, then to maintain the same body temperature the same (living) human being needs to radiate $\Delta \mathrm{W}=4 \sigma \mathrm{T}_0^3 \Delta \mathrm{T}_0$ more energy per unit time.
[$C$] Reducing the exposed surface area of the body ($e.g$ by curling up) allows humans to maintain the same body temperature while reducing the energy lost by radiation.
[$D$] If the body temperature rises significantly then the peak in the spectrum of electromagnetic radiation emitted by the body would shift to longer wavelengths.