So, we get lengths of two open pipes as $L _{1}=\frac{ v }{2 n _{1}}$ and $L _{2}=\frac{ v }{2 n _{2}}$ Now the pipes are join in series.
Fundamental frequency of new open pipe of length $L _{1}+ L _{2},$
$n =\frac{ v }{2\left( L _{1}+ L _{2}\right)}$
$n =\frac{ v }{2\left(\frac{ v }{2 n _{1}}+\frac{ v }{2 n _{2}}\right)}$
$n=\frac{1}{\frac{1}{n_{1}}+\frac{1}{n_{2}}}$
$\Rightarrow n =\frac{ n _{1} n _{2}}{ n _{1}+ n _{2}}$
$(I)$ a high-pressure pulse starts travelling up the pipe, if the other end of the pipe is open
$(II)$ a low -pressure pulse starts travelling up the pipe, if the other end of the pipe is open
$(III)$ a low pressure pulse starts travelling up the pipe, if the other end of the pipe is closed
$(IV)$ a high-pressure pulse starts travelling up the pipe, if the other end of the pipe is closed
$(A)$ the intensity of the sound heard at the first resonance was more than that at the second resonance
$(B)$ the prongs of the tuning fork were kept in a horizontal plane above the resonance tube
$(C)$ the amplitude of vibration of the ends of the prongs is typically around $1 \mathrm{~cm}$
$(D)$ the length of the air-column at the first resonance was somewhat shorter than $1 / 4$ th of the wavelength of the sound in air
$y = 0.02sin\left[ {2\pi \left( {\frac{t}{{0.04\left( s \right)}} - \frac{x}{{0.50\left( m \right)}}} \right)} \right]m$ The tension in the string is .... $N$