For the air column closed at one end, let
L = the length of the air column,
nc = the fundamental frequency,
nq, nq + 1 = the frequencies of the qth and (q + 1)th overtones, where q = 1, 2, 3, … Since only odd harmonics are present as overtones, nq = (2q + 1)nc and nq+ 1 = [2(q + 1) + n]nc
= (2q + 3)nc
Data : nq = 405 Hz, nq + 1 = 675 Hz

Solving for q, q = 1
Therefore, the two given frequencies correspond to the first and second overtones, i.e., the third and fifth harmonics.
∴ 3nc = 405 Hz
∴ nc = 135 Hz
This gives the fundamental frequency of the air column closed at one end.
The fundamental frequency (no) of an air column of same length but open at both ends is double that of the air column closed at one end (ignoring the end correction).
∴ no = 2nc = 2 × 135 = 270 Hz
This gives the fundamental frequency of a similar air column but open at both ends.
Data : n = 480 Hz, l1 = 16.8 cm, l2 = 51.8 cm
(1) The speed of sound in air is v = 2n (l2 – l1) = 2 × 480 × (51.8 – 16.8) = 33600 cm/s = 336 m/s
(2) Let λ be the wavelength of sound waves and e be the end correction. For the first resonance, l1 + e = \(\frac λ4\) … (1)
For the second resonance, l2 + e = \(\frac {3λ}4\)… (2)
From Eq. (1), λ = 4(l1 + e).
Substituting this value in Eq. (2), we get,
