Step 1: Apply Bragg's law.
\[
2d\sin\theta = n\lambda
\]
For first order (\(n=1\)):
\[
d = \frac{\lambda}{2\sin\theta} = \frac{0.2}{2\sin21^\circ} = \frac{0.2}{0.716} = 0.279\, \text{nm}
\]
Step 2: Relate interplanar spacing to lattice constant.
For cubic crystals:
\[
d_{hkl} = \frac{a}{\sqrt{h^2 + k^2 + l^2}} = \frac{a}{\sqrt{4}}
\]
\[
a = 2d = 2(0.279) = 0.558 \, \text{nm} \approx 0.56\, \text{nm}
\]
Step 3: Conclusion.
Hence, unit cell size \(a = 0.56\, \text{nm}\).

At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/m³, which is dimensionally incorrect for a spectral density. The correct unit J/(m³·Hz) or J·s/m³ is used here for the solution.)