Step 1: Understanding the Question:
The problem compares two acoustic organ pipes: Pipe A is closed at one end, and Pipe B is open at both ends. We are given that the fundamental frequency of Pipe A equals the second overtone frequency of Pipe B, and we need to find the ratio of their physical lengths ($\frac{L_A}{L_B}$).
Step 2: Key Formula or Approach:
1. For an organ pipe closed at one end (length $L_A$), the fundamental frequency is given by:
$$n_A = \frac{v}{4L_A}$$
2. For an organ pipe open at both ends (length $L_B$), the fundamental frequency is $n_B = \frac{v}{2L_B}$. The open pipe produces all integer harmonics, so its second overtone corresponds to the third harmonic ($3n_B$):
$$n_B' = 3 \left(\frac{v}{2L_B}\right) = \frac{3v}{2L_B}$$
Step 3: Detailed Explanation:
According to the problem, the fundamental frequency of Pipe A is equal to the second overtone of Pipe B:
$$n_A = n_B'$$
Substitute our length equations into this frequency equality:
$$\frac{v}{4L_A} = \frac{3v}{2L_B}$$
Since the speed of sound $v$ is identical in both pipes, we can cancel it from both numerators:
$$\frac{1}{4L_A} = \frac{3}{2L_B}$$
Now, rearrange the terms to isolate the length ratio $\frac{L_A}{L_B}$ by cross-multiplying:
$$\frac{L_A}{L_B} = \frac{2}{4 \times 3} = \frac{2}{12} = \frac{1}{6}$$
This simplifies to a length ratio of exactly 1 : 6.
Step 4: Final Answer:
The ratio of the length of pipe 'A' to that of pipe 'B' is 1 : 6, which corresponds to option (C).