To solve the problem of determining the maximum and minimum possible intensities when two coherent monochromatic light beams are superimposed, we must understand the principle of superposition and interference.
When two light beams interfere, the resultant intensity depends on the phase difference between them. The resultant intensity \( I_r \) is given by:
Ir = \( I_1 + I_2 + 2\sqrt{I_1 I_2}\cos(\phi) \)
where \( I_1 \) and \( I_2 \) are the intensities of the individual beams, and \( \phi \) is the phase difference between the beams. Let's apply this for the given problem:
Given: \( I_1 = I \) and \( I_2 = 4I \)
1. **Maximum Intensity**: This occurs when the beams interfere constructively, i.e., \( \phi = 0 \). The cosine term becomes 1.
\( I_{max} = I + 4I + 2\sqrt{I \cdot 4I}\cdot 1 \)
= \( 5I + 4I \)
= \( 9I \)
2. **Minimum Intensity**: This occurs when the beams interfere destructively, i.e., \( \phi = \pi \). The cosine term becomes -1.
\( I_{min} = I + 4I + 2\sqrt{I \cdot 4I}\cdot (-1) \)
= \( 5I - 4I \)
= \( I \)
Thus, the maximum and minimum possible intensities in the resulting beam are \( 9I \) and \( I \) respectively.
Since the two beams are coherent, their electric field amplitudes add directly when they overlap, and intensity is proportional to the square of the amplitude. If the amplitude of the weaker beam is \( a \), then its intensity is \( I \propto a^2 = I \), and since the second beam has intensity \( 4I \), its amplitude must be \( 2a \) (because \( (2a)^2 = 4a^2 = 4I \)). The two extreme cases of overlap are when the two waves arrive perfectly in step, so the amplitudes simply add, and when they arrive perfectly out of step, so the amplitudes simply subtract. Let's use this to check each option.
Working from the amplitudes directly, rather than the resultant-intensity formula, still gives a maximum of \( 9a^2 \) and a minimum of \( a^2 \), which in terms of \( I \) are \( 9I \) and \( I \).
Therefore, the correct answer is 9I and I.