(c) In closed organ pipe. First resonance occurs at $\lambda/4.$
So, in fundamental mode of vibration of organ pipe
$\frac{\lambda}{4} = (l + 0.3\ d)$
Where $0.3\ d$ is necessary end correction
Frequency of vibration $n = \frac{v}{\lambda} = \frac{v}{4(l + 0.3d)}$
As $l$ is same, wider pipe $A$ will resonate at a lower frequency, $i.e.,\ n_{A} < n_{B}$
Note : The value of end correction $\theta$ is $0.6\ r$ for closed organ pipe and $1.2\ r$ for an open organ pipe, where $r$ is the radius of the pipe