Let us consider the following diagram organ is open at both ends,
For first harmonic-

L = \(\frac{λ}{2}\)
or λ = 2L
[As, λ= \(\frac{c}{v}\), c = speed of sound air]
\(\frac{c}{v}\)= 2L
or v = \(\frac{c}{2L}\)
For pipe closed at one end-

\(v_1=\frac{c}{4L_1}\)
But v= v1 [for resonance same tuning fort]
\(\frac{c}{2L}=\frac{c}{4L_1}\) [∴ Speed remains constant]
\(\frac {L_1}{L}=\frac{2}{4}=\frac{1}{2}\)
or L1 = \(\frac{L}{2}\)