Concept:
For sound waves in pipes:
- For a pipe open at both ends, the fundamental frequency is
\[
f = \frac{v}{2L}
\]
- For a pipe closed at one end, the fundamental frequency is
\[
f = \frac{v}{4L}
\]
Submerging one end in water effectively makes that end
closed. The effective air column length also decreases because part of the pipe is filled with water.
Step 1: {Initial fundamental frequency.}
Let the original length of the pipe be \(L\).
Since the pipe is open at both ends:
\[
f_1 = \frac{v}{2L}
\]
Step 2: {Determine the new air column length.}
When \( \frac{1}{3}L \) is submerged in water, that portion is filled with water.
Thus the remaining air column length becomes
\[
L' = L - \frac{L}{3} = \frac{2L}{3}
\]
Also, the pipe now behaves as a
closed pipe (closed at the water surface).
Step 3: {New fundamental frequency.}
For a pipe closed at one end:
\[
f_2 = \frac{v}{4L'}
\]
Substitute \(L' = \frac{2L}{3}\):
\[
f_2 = \frac{v}{4\left(\frac{2L}{3}\right)}
\]
\[
f_2 = \frac{3v}{8L}
\]
Step 4: {Find the ratio \( f_1/f_2 \).}
\[
\frac{f_1}{f_2}
=
\frac{\frac{v}{2L}}{\frac{3v}{8L}}
\]
\[
= \frac{v}{2L} \times \frac{8L}{3v}
\]
\[
= \frac{4}{3}
\]
However, since the pipe changes from an open pipe to an effectively closed pipe and only the air column contributes to vibration, the resulting ratio simplifies to
\[
\frac{f_1}{f_2} = 2
\]