A hot black body emits the energy at the rate of $16\ J\ m^{-2}\ s^{-1}$ and its most intense radiation corresponds to $20,000\ Å$ . When the temperature of this body is further increased and its most intense radiation corresponds to $10,000\ Å$ , then the energy radiated in $Jm^{-2}\ s^{-1}$ will be
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Wein's displacement law is $:$

$\lambda_{\mathrm{m}} \cdot \mathrm{T}=\mathrm{b}$

i.e. $\mathrm{T} \propto \frac{1}{\lambda_{\mathrm{m}}}$

Here, $\lambda_{\mathrm{m}}$ becomes half.

$\therefore$ Temperature doubles.

Also $e$ $=\sigma \mathrm{T}^{4}$

$\Rightarrow \frac{\mathrm{e}_{1}}{\mathrm{e}_{2}}=\left(\frac{\mathrm{T}_{1}}{\mathrm{T}_{2}}\right)^{4}$

$\Rightarrow \mathrm{e}_{2}=\left(\frac{\mathrm{T}_{2}}{\mathrm{T}_{1}}\right)^{4} \cdot \mathrm{e}_{1}=(2)^{4} \cdot 16$

$=16.16=256 \mathrm{J} \mathrm{m}^{-2} \mathrm{s}^{-1}$

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