\( \frac{2\pi \lambda}{a}\)
\( \frac{2\pi a}{\lambda}\)
\( \frac{\lambda}{a}\)
\( \frac{a}{\lambda}\)
The general equation for a travelling wave is:
y = A sin(kx − ωt)
where:
A is the amplitude.
k is the wave number ($k = \frac{2\pi}{\lambda}$).
ω is the angular frequency ($\omega = 2\pi f$).
f is the frequency.
Comparing this with given equation: y = C sin($\frac{2\pi}{\lambda}$(at − x)), we get ω = $\frac{2\pi a}{\lambda}$.
Since ω = 2πf: 2πf = $\frac{2\pi a}{\lambda}$
$f = \frac{a}{\lambda}$
Two loudspeakers (\(L_1\) and \(L_2\)) are placed with a separation of \(10 \, \text{m}\), as shown in the figure. Both speakers are fed with an audio input signal of the same frequency with constant volume. A voice recorder, initially at point \(A\), at equidistance to both loudspeakers, is moved by \(25 \, \text{m}\) along the line \(AB\) while monitoring the audio signal. The measured signal was found to undergo \(10\) cycles of minima and maxima during the movement. The frequency of the input signal is _____________ Hz.
(Speed of sound in air is \(324 \, \text{m/s}\) and \( \sqrt{5} = 2.23 \)) 

Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity) 