
When only \(π_2\) is emitting sound and it is at \(π\), 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:
\(f'=f\times\frac{v+v_0}{v+v_s}\)ββ
Where:
Initially, only π2 emits sound at π. To calculate the frequency observed at π, let's determine the relative speed of π2 towards the detector at π.
The observer's speed \((v_oβ)\) is 0 since the detector is stationary at π.
Now, the speed of π2 concerning the detector at π will be the component of the speed of π2 perpendicular to the line ππ.
Given that π2 moves at a uniform speed of 4\(\sqrt{2}\) \(ms^{β1}\) on a circular path around π, and π is equidistant from π and π
, which are diametrically opposite, the speed of π2 towards the detector at π is 4\(\sqrt{2}\)β \(ms^{β1}\)
Now, let's use the Doppler effect formula:
\(f'=f\times\frac{v+v_0}{v+v_s}\)
Given that \(f\)= \(656\) Hz, \(v\) = \(324 \;ms^{β1}\), \(v_o\)β=\(0\) \(ms^{β1}\) and \(v_s\)β = 4\(\sqrt{2}\) msβ1, let's calculate the observed frequency at \(π\) when only \(π_2\)emits sound
at \(π\).\(f'=656\times\frac{324+0}{324+4\sqrt{2}}\)
\(f'=656\times\frac{324}{324+4\sqrt{2}}\)
\(f' = 648.00\)

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
β΄ Beat frequency \(Ξ f = f_1 β f_2 \)
\(=656(\frac{324}{320}-1)\)
\(Ξ f = 8.2\)
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