Answer:
Part a)
[tex]\Delta \phi = 2.2 \pi[/tex]
Part b)
[tex]f = 411.3 Hz[/tex]
Explanation:
As we know that the observer is standing in front of one speaker
So here the path difference of the two sound waves reaching to the observer is given as
[tex]\Delta x = 3\sqrt2 - 3[/tex]
[tex]\Delta x = 1.24 m[/tex]
now phase difference is related with path difference as
[tex]\Delta \phi = \frac{2\pi}{\lambda}(\Delta x)[/tex]
[tex]\Delta \phi = \frac{2\pi}{\lambda}(1.24)[/tex]
here in order to find the wavelength
[tex]\lambda = \frac{c}{f}[/tex]
[tex]\lambda = \frac{340}{300} = 1.13[/tex]
now we have
[tex]\Delta \phi = \frac{2\pi}{1.13}(1.24) = 2.2\pi[/tex]
Part b)
Now we know that when phase difference is odd multiple of [tex]\pi[/tex]
then in that case the the sound must be minimum
So nearest value for minimum intensity would be
[tex]\Delta \phi = 3\pi[/tex]
so we have
[tex]3\pi = \frac{2\pi}{\lambda}(1.24)[/tex]
so we have
[tex]\lambda = 0.827 [/tex]
now we have
[tex]\frac{340}{f} = 0.827[/tex]
[tex]f = 411.3 Hz[/tex]