When a wire of length L vibrates is resonant frequency in nth mode after stretching it by tension T, then frequency, \(v=\frac{n}{2L}\sqrt{\frac{T}{m}}\)
[Here, m = mass per unit length of stretched wire]
Let us consider two given cases:
\(v_1=\frac{n_1}{2L_1}\sqrt{\frac{T_1}{m_1}}\)&v2 = \(\frac{n_2}{2L_2}=\sqrt{\frac{T_2}{m_2}}\)
From question,
T1 = T2 = T, m1 = m2 = m (as wires are same)
L2 = 2L1
\(\frac{v_1}{v_2}=(\frac {n_1}{2L_1}\sqrt{\frac{T}{m}})\div(\frac{n_2}{2(2L_1)}\sqrt{\frac{T}{m}})= \frac{2n_1}{n_2}\)
As turning fork is same, ∴ v1 = v2
\(\frac{2n_1}{n_2}=1 \,or\, n_2=2n_1\)
Hence, when length of wire double the number of harmonics double for same resonant frequency.