A pipe open at both ends has a fundamental frequency \( f \) in air, calculated as \( f = \frac{v}{2L} \), where \( v \) is the speed of sound and \( L \) is the pipe length.
When submerged in water to half its length, the pipe functions as a closed pipe with an effective length of \( \frac{L}{2} \).
The fundamental frequency \( f' \) for a closed pipe is \( f' = \frac{v}{4L'} \).
Substituting \( L' = \frac{L}{2} \) yields \( f' = \frac{v}{4 \times \frac{L}{2}} = \frac{v}{2L} \), which equals the original frequency \( f \).
Consequently, the fundamental frequency remains \( f \) when the pipe is dipped to half its length in water.
The correct answer is \( f \).