
When only \(𝑆_2\) is emitting sound and it is at \(𝑄\), the frequency of sound measured by the detector in Hz is \(\underline{648.00}.\)
Explanation:
The Doppler effect formula for sound when the source is moving towards the observer is given by:
\(f'=f\times\frac{v+v_0}{v+v_s}\)
Where:
Initially, only 𝑆2 emits sound at 𝑄. To calculate the frequency observed at 𝑃, let's determine the relative speed of 𝑆2 towards the detector at 𝑃.
The observer's speed \((v_o)\) is 0 since the detector is stationary at 𝑃.
Now, the speed of 𝑆2 concerning the detector at 𝑃 will be the component of the speed of 𝑆2 perpendicular to the line 𝑄𝑃.
Given that 𝑆2 moves at a uniform speed of 4\(\sqrt{2}\) \(ms^{−1}\) on a circular path around 𝑂, and 𝑄 is equidistant from 𝑃 and 𝑅, which are diametrically opposite, the speed of 𝑆2 towards the detector at 𝑃 is 4\(\sqrt{2}\) \(ms^{−1}\)
Now, let's use the Doppler effect formula:
\(f'=f\times\frac{v+v_0}{v+v_s}\)
Given that \(f\)= \(656\) Hz, \(v\) = \(324 \;ms^{−1}\), \(v_o\)=\(0\) \(ms^{−1}\) and \(v_s\) = 4\(\sqrt{2}\) ms−1, let's calculate the observed frequency at \(𝑃\) when only \(𝑆_2\)emits sound
at \(𝑄\).\(f'=656\times\frac{324+0}{324+4\sqrt{2}}\)
\(f'=656\times\frac{324}{324+4\sqrt{2}}\)
\(f' = 648.00\)

f0 = 656 Hz
v = 324 m/s Frequency heard due to movement of (S1)
\(f_1=(\frac{v}{v-u_s})f_0\)
\(f_1=\frac{324}{3520}\times656\)
And frequency heard due to movement of (S2)
f2 = 656 Hz
∴ Beat frequency \(Δ f = f_1 – f_2 \)
\(=656(\frac{324}{320}-1)\)
\(Δ f = 8.2\)