`S_(1)` and `S_(2)` are two coherent sources of sound of frequency `110Hz` each they have no initial phase difference. The intensity at a point P due to `S_(1)` is `I_0` and due to `S_2` is `4I_0`. If the velocity of sound is `330m//s` then the resultant intensity at P is

S_1 and S_2 are two coherent sources of sound having no initial phase difference. The velocity of sound is 330m//s . No minimal will be formed on the line passing through S_2 and perpendicular to the line jouning S_1 and S_2 . If the frequency of both the sources is:

S_(1) and S_(2) are two coherent sources of sound having no intial phase difference. The velocity of sound is 330 m//s . No maximum will be formed on the line passing through S_(2) and prependicular to the line joining S_(1) and S_(2) . If the frequency of both the sources is

S_(1) and S_(2) are two coherent sources of sound having no intial phase difference. The velocity of sound is 330 m//s . No maximum will be formed on the line passing through S_(2) and prependicular to the line joining S_(1) and S_(2) . If the frequency of both the sources is

S_(1) and S_(2) are two coherent sources. The intensity of both sources are same. If the intensity at the point of maxima is 4Wm^(-2) , the intensity of each source is

In the figure the intensity of waves arriving at D from two coherent sources S_1 and S_2 is I_0 The wavelength of the wave is lamda=4m . Resultant intensity at D will be:

In the figure , the intensity of waves arriving at D from two coherent soucrces s_(1) and s_(2) is I_(0) . The wavelength of the wave is lambda = 4 m . Resultant intensity at D will be

In the figure , the intensity of waves arriving at D from two coherent soucrces s_(1) and s_(2) is I_(0) . The wavelength of the wave is lambda = 4 m . Resultant intensity at D will be

In the figure , the intensity of waves arriving at D from two coherent soucrces s_(1) and s_(2) is I_(0) . The wavelength of the wave is lambda = 4 m . Resultant intensity at D will be

In an interference arrangement similar to young's double slit experiment the slits S_(1) and S_(2) are illuminated with coherent microwave sources each of frequency 10^(6)Hz the sources are synchronized to have zero phase difference. the slits are separated by a distance d=150.0m. The intensity I(theta) is measured as a funtion of theta , where theta is defined as shown. if I_(0) is the maximum intensity then I(theta) for 0lethetale90^(@) is given by: