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Show that the fundamental frequency of vibration of the air column in a pipe open at both ends is double that of a pipe of the same length and closed at one end.

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Let LO and LC be the lengths of a pipe open at both ends and a pipe closed at one end, respectively. Let nO and nC be their corresponding fundamental frequencies. Then, ignoring the end corrections,

n\(\frac v{2L_O}\) and n\(\frac v{4L_C}\)

where v is the speed of the sound in air.

Given that L= LC = L (say),

n\(\frac v{2L}\) and n\(\frac v{4L}\)

∴ n= 2 \((\frac v{4L})\) = 2nC

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