Step 1: Understanding the Question:
The question asks how the wavelength of maximum emission ($\lambda_{max}$) from a black body changes if its absolute temperature ($T$) is doubled.
This is governed by the laws of thermal radiation.
Step 2: Key Formula or Approach:
We apply Wien's Displacement Law, which relates the peak wavelength of black body radiation to its absolute temperature:
\[ \lambda_{max} \cdot T = b \]
Where $b$ is Wien's displacement constant ($b \approx 2.898 \times 10^{-3}\text{ m}\cdot\text{K}$).
This indicates that:
\[ \lambda_{max} \propto \frac{1}{T} \]
Step 3: Detailed Explanation:
• Wien's Displacement Law states that the wavelength ($\lambda_{max}$) at which the emissive power of a black body is maximum is inversely proportional to its absolute temperature ($T$).
• Let the initial absolute temperature be $T_1 = T$ and the initial wavelength of maximum emission be $\lambda_1$.
• The final temperature is doubled: $T_2 = 2T$.
• Let the final wavelength of maximum emission be $\lambda_2$.
• Using the inverse proportionality:
\[ \frac{\lambda_2}{\lambda_1} = \frac{T_1}{T_2} \]
• Substitute the values into the ratio:
\[ \frac{\lambda_2}{\lambda_1} = \frac{T}{2T} = \frac{1}{2} \]
\[ \lambda_2 = \frac{\lambda_1}{2} \]
• Thus, doubling the absolute temperature causes the wavelength of maximum emission to be halved.
Step 4: Final Answer:
The wavelength of maximum emission is halved.