A black body has a wavelength \(\lambda_m\) corresponding to maximum energy at \(2000~\text{K}\). Its wavelength corresponding to maximum energy at \(3000~\text{K}\) will be:
1. | \(\dfrac{3}{2}\lambda_m\) | 2. | \(\dfrac{2}{3}\lambda_m\) |
3. | \(\dfrac{16}{81}\lambda_m\) | 4. | \(\dfrac{81}{16}\lambda_m\) |
Wien's displacement law expresses the relation between:
1. | Wavelength corresponding to maximum energy and temperature |
2. | Radiation energy and wavelength |
3. | Temperature and wavelength |
4. | Colour of light and temperature |
If λm denotes the wavelength at which the radioactive emission from a black body at a temperature T K is maximum, then:
1. λm is independent of T
2. λm ∝ T
3. λm ∝ T–1
4. λm ∝ T– 4