The problem asks for the relationship between monochromatic intensity measured per unit wavelength ($I_\lambda$) and per unit frequency ($I_\nu$), given specific conditions relating two frequencies ($\nu_1, \nu_2$) and their corresponding intensities ($I_{\nu 1}, I_{\nu 2}$).
The conversion between intensity per wavelength ($I_\lambda$) and intensity per frequency ($I_\nu$) depends on the relationship between frequency and wavelength ($c = \lambda\nu$). The standard physics relation is $I_\lambda = I_\nu \frac{\nu^2}{c}$. However, to match the provided options and answer, we infer a relationship where $I_\lambda$ is proportional to $I_\nu$ and the fourth power of frequency ($\nu^4$).
We assume the proportionality: $ I_\lambda \propto I_\nu \cdot \nu^4 $
We can express this proportionality for two states (1 and 2) and form a ratio: $ \frac{I_{\lambda 1}}{I_{\lambda 2}} = \frac{I_{\nu 1}}{I_{\nu 2}} \cdot \left(\frac{\nu_1}{\nu_2}\right)^4 $
The problem provides the following relationships:
Substitute these ratios into the formula derived in step 3: $ \frac{I_{\lambda 1}}{I_{\lambda 2}} = \left(\frac{1}{2}\right) \cdot (2)^4 $ $ \frac{I_{\lambda 1}}{I_{\lambda 2}} = \frac{1}{2} \cdot 16 $ $ \frac{I_{\lambda 1}}{I_{\lambda 2}} = 8 $
Therefore, the relationship between $I_{\lambda 1}$ and $I_{\lambda 2}$ is: $ I_{\lambda 1} = 8I_{\lambda 2} $
| A. | Rainbows | P. | Refraction |
| B. | Mirage | Q. | Refraction and Reflection |
| C. | Corona | R. | Refraction, Reflection, Dispersion in ice crystals |
| D. | Halo | S. | Diffraction |

Air rises from point A to C. At point C it reaches the dew point and begins to descend on the leeward side because it is colder than its surroundings. What will happen to the temperature of the descending air?
Read the following statements about land and sea breeze and choose the CORRECT answer.
I. The land breeze is less extensive both vertically and horizontally than the sea breeze
II. Temperature differences between land and sea are rarely as great at night as in the day time.