
For least intense sound, $1 \,m$ can cause a destructive interference. So, path difference is an odd multiple of half wavelength.
$\Rightarrow \Delta L=(2 n+1) \frac{\lambda_1}{2}$
$\Rightarrow 1 \,m =\frac{\lambda_1, 3 \lambda_1, 5 \lambda_1}{2}, \frac{2}{2}, \text { etc. }$
Above condition is satisfied, when $\lambda_1=2 \,m$.
And for most intense sound, path difference of $1 m$ can cause a constructive interference. So, path difference must be a whole number multiple of one wavelength.
$\Rightarrow \Delta L=n \lambda_2$
$\Rightarrow 1 \,m =\lambda_2, 2 \lambda_2, 3 \lambda_2, \ldots, \text { etc. }$
Above condition is satisf ied with $\lambda_2=1 \,m$.
So, correct option is $(c)$.

$y(x,t)\, = \,0.6\,\sin \,\left( {\frac{{2\pi }}{3}x} \right)\,\cos \,(120\,\pi t)$
where $x$ and $y$ are in $metre$ and $t$ in $second$ . The length of the string is $1.5\,m$ and its mass is $3.0\times 10^{-2}\,kg$ the tension in the string will be .... $N$

(Velocity of sound in air is $340\,ms ^{-1}$ )