MHT CET · Physics · Thermal Properties of Matter
A black body radiates maximum energy at wavelength \(^{\prime} \lambda^{\prime}\) and its emissive power is \({ }^{\prime} \mathrm{E}^{\prime}\). Now, due to change in temperature of that body, it radiates maximum energy at wavelength \(\frac{2 \lambda}{3}\). At that temperature, emissive power is
- A \(\frac{27 \mathrm{E}}{16}\)
- B \(\frac{81 \mathrm{E}}{16}\)
- C \(\frac{91 \mathrm{E}}{16}\)
- D \(\frac{54 \mathrm{E}}{16}\)
Answer & Solution
Correct Answer
(B) \(\frac{81 \mathrm{E}}{16}\)
Step-by-step Solution
Detailed explanation
\(\lambda_{\max } \mathrm{T}_{1}=\lambda_{2 \max } \mathrm{T}_{2} \quad \quad \mathrm{E}=\sigma \mathrm{A} \mathrm{T}_{1}^{4}\)
\(\mathrm{T}_{2}=\frac{\lambda_{1} \mathrm{~T}_{1}}{\lambda_{2}}\)
\(\frac{E_{2}}{E_{1}}=\frac{T_{2}^{4}}{T_{1}^{4}}\)
\(\therefore \mathrm{E}_{2}=\mathrm{E}_{1} \times \frac{\lambda_{1}^{4} \mathrm{~T}_{1}^{4}}{\lambda_{2}^{4}} \times \frac{1}{\mathrm{~T}_{1}^{4}}=\mathrm{E} \times \frac{\lambda_{1}^{4}}{\frac{16}{81} \lambda_{1}^{4}}=\frac{81}{16} \mathrm{E}\)
\(\mathrm{T}_{2}=\frac{\lambda_{1} \mathrm{~T}_{1}}{\lambda_{2}}\)
\(\frac{E_{2}}{E_{1}}=\frac{T_{2}^{4}}{T_{1}^{4}}\)
\(\therefore \mathrm{E}_{2}=\mathrm{E}_{1} \times \frac{\lambda_{1}^{4} \mathrm{~T}_{1}^{4}}{\lambda_{2}^{4}} \times \frac{1}{\mathrm{~T}_{1}^{4}}=\mathrm{E} \times \frac{\lambda_{1}^{4}}{\frac{16}{81} \lambda_{1}^{4}}=\frac{81}{16} \mathrm{E}\)
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