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When the temperature of a black body inc...

When the temperature of a black body increases, it is observed that the wavelength corresponding to maximum energy changes from `0.26mum` to `0.13mum`. The ratio of the emissive powers of the body at the respective temperatures is

A

`(16)/(1)`

B

`(4)/(1)`

C

`(1)/(4)`

D

`(1)/(16)`

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The correct Answer is:
To solve the problem, we need to find the ratio of the emissive powers of a black body at two different temperatures, given the wavelengths corresponding to maximum energy. We will use Wien's displacement law and Stefan-Boltzmann law to derive the solution step by step. ### Step-by-Step Solution: 1. **Identify the Given Values:** - Wavelength at temperature T1, \( \lambda_1 = 0.26 \, \mu m \) - Wavelength at temperature T2, \( \lambda_2 = 0.13 \, \mu m \) 2. **Apply Wien's Displacement Law:** - According to Wien's displacement law, the product of the wavelength of maximum energy (\( \lambda_m \)) and the temperature (T) is a constant: \[ \lambda_1 T_1 = \lambda_2 T_2 \] 3. **Rearrange the Equation:** - From the above equation, we can express the ratio of the temperatures: \[ \frac{\lambda_1}{\lambda_2} = \frac{T_2}{T_1} \] 4. **Substitute the Values:** - Substitute the values of \( \lambda_1 \) and \( \lambda_2 \): \[ \frac{0.26 \, \mu m}{0.13 \, \mu m} = \frac{T_2}{T_1} \] - This simplifies to: \[ 2 = \frac{T_2}{T_1} \] - Thus, we find: \[ T_2 = 2 T_1 \] 5. **Use Stefan-Boltzmann Law:** - The emissive power (E) of a black body is proportional to the fourth power of its absolute temperature: \[ E \propto T^4 \] - Therefore, the ratio of the emissive powers at temperatures T1 and T2 is: \[ \frac{E_1}{E_2} = \frac{T_1^4}{T_2^4} \] 6. **Substitute \( T_2 \) in Terms of \( T_1 \):** - Substitute \( T_2 = 2 T_1 \) into the emissive power ratio: \[ \frac{E_1}{E_2} = \frac{T_1^4}{(2 T_1)^4} \] 7. **Simplify the Expression:** - Simplifying the right-hand side: \[ \frac{E_1}{E_2} = \frac{T_1^4}{16 T_1^4} = \frac{1}{16} \] 8. **Final Result:** - Therefore, the ratio of the emissive powers of the body at the respective temperatures is: \[ \frac{E_1}{E_2} = \frac{1}{16} \]

To solve the problem, we need to find the ratio of the emissive powers of a black body at two different temperatures, given the wavelengths corresponding to maximum energy. We will use Wien's displacement law and Stefan-Boltzmann law to derive the solution step by step. ### Step-by-Step Solution: 1. **Identify the Given Values:** - Wavelength at temperature T1, \( \lambda_1 = 0.26 \, \mu m \) - Wavelength at temperature T2, \( \lambda_2 = 0.13 \, \mu m \) ...
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