
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 \(Ξ f = f_1 β f_2 \)
\(=656(\frac{324}{320}-1)\)
\(Ξ f = 8.2\)
The reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is: