λm is independent of T
λm ∝ T
λm ∝ T–1
λm ∝ T–4
To solve this problem, we need to understand the physical concept related to the wavelength at which a black body emits radiation most efficiently at a given temperature. The concept in question here pertains to Wien's Displacement Law.
**Wien's Displacement Law**
Wien's Displacement Law states that the wavelength \(\lambda_m\) corresponding to the maximum emission from a black body is inversely proportional to its temperature. Mathematically, this is expressed as:
\(\lambda_m \propto \frac{1}{T}\)
This indicates that as the temperature of the black body increases, the peak wavelength at which it emits radiation decreases. This law is derived from Planck's radiation law and is fundamental in understanding black body radiation.
**Step-by-Step Explanation**
**Conclusion**: The correct option is \(\lambda_m \propto T^{-1}\), which matches the statement: λm ∝ T–1.
**Rule Out Other Options**