Step 1: Find the temperature of the perfect radiator using Wien's Displacement Law.
Wien's Law states that \( \lambda_{max} T = b \), where b is Wien's constant.
We are given the wavelength of maximum intensity, \( \lambda_{max} = 2900 \) Å.
Convert this wavelength to meters: \( \lambda_{max} = 2900 \times 10^{-10} \text{ m} = 2.9 \times 10^{-7} \text{ m} \).
Wien's constant is \( b = 2.9 \times 10^{-3} \) mK.
Now, solve for the temperature T.
\( T = \frac{b}{\lambda_{max}} = \frac{2.9 \times 10^{-3}}{2.9 \times 10^{-7}} = 1 \times 10^{(-3 - (-7))} = 10^4 \) K.
Step 2: Find the intensity of radiation using the Stefan-Boltzmann Law.
The Stefan-Boltzmann Law states that the total intensity (or emissive power) I of a perfect radiator (black body) is given by \( I = \sigma T^4 \), where \(\sigma\) is the Stefan-Boltzmann constant.
We are given \( \sigma = 5.67 \times 10^{-8} \) Wm\(^{-2}\)K\(^{-4}\).
We found \( T = 10^4 \) K.
Substitute these values into the formula.
\( I = (5.67 \times 10^{-8}) \times (10^4)^4 \).
\( I = 5.67 \times 10^{-8} \times 10^{16} = 5.67 \times 10^{16-8} = 5.67 \times 10^8 \) Wm\(^{-2}\).