Three identical sources of sound are placed on a straight line as shown in the figure . A detector D is placed at a distance d from S1. The wavelength of sound is λ.
Determine the value of d so that the intensity of the wave at the detector may be
(a) zero
(b) nine times the intensity of each source.
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Constructive interference and destructive interference. Intensity of the wave.
We are given identical sources. There is no phase difference. Frequency f, ω, time period T, wavelength λ and speed v are all identical. Also their amplitudes are equal.
k = 2π/λ = ω/v. ω = 2πf = 2π/T = k v
A sound wave is a pressure wave and is a progressive wave. The excess pressure (compared to the equilibrium pressure) at a point is specified in the (longitudinal) wave equation as :
Sound from S1 at :
p1 = p0 * Sin(k x - ωt) = p0 * Sin (3d k - ωt), as x = 3d
Sound from S2:
p2 = p0 * Sin (kx- ωt) = p0 * Sin (2d k - ωt), as x = 2d
Sound from S3 : p 3 = p0 * Sin (d k - ωt) as x = d
Interference of the three waves at point D means the waves are added algebraically.
Resultant wave = p1+ p2 + p3
= 2 p0 Sin(2 k d - ωt) Cos (dk) + p0 Sin (2d k - ωt)
= p0 * SIn(2 d k - ωt) * [2 Cos(dk) + 1 ]
The resultant wave is zero with destructive interference, if
Cos (dk) = -1/2
d k = (2n+1) π + π/3
The constructive interference occurs when
Cos(dk) = 1 = max value.
d k = 2 n π
d * 2π/λ = 2 n π
=> d = n λ So integral multiple of wave length.
Then the resultant wave is : 3 p0 Sin(2 kd - ωt)
Since the amplitude is 3 p0 , the intensity I is (square of amplitude) 9 times the original amplitude of each source of sound.
We are given identical sources. There is no phase difference. Frequency f, ω, time period T, wavelength λ and speed v are all identical. Also their amplitudes are equal.
k = 2π/λ = ω/v. ω = 2πf = 2π/T = k v
A sound wave is a pressure wave and is a progressive wave. The excess pressure (compared to the equilibrium pressure) at a point is specified in the (longitudinal) wave equation as :
Sound from S1 at :
p1 = p0 * Sin(k x - ωt) = p0 * Sin (3d k - ωt), as x = 3d
Sound from S2:
p2 = p0 * Sin (kx- ωt) = p0 * Sin (2d k - ωt), as x = 2d
Sound from S3 : p 3 = p0 * Sin (d k - ωt) as x = d
Interference of the three waves at point D means the waves are added algebraically.
Resultant wave = p1+ p2 + p3
= 2 p0 Sin(2 k d - ωt) Cos (dk) + p0 Sin (2d k - ωt)
= p0 * SIn(2 d k - ωt) * [2 Cos(dk) + 1 ]
The resultant wave is zero with destructive interference, if
Cos (dk) = -1/2
d k = (2n+1) π + π/3
The constructive interference occurs when
Cos(dk) = 1 = max value.
d k = 2 n π
d * 2π/λ = 2 n π
=> d = n λ So integral multiple of wave length.
Then the resultant wave is : 3 p0 Sin(2 kd - ωt)
Since the amplitude is 3 p0 , the intensity I is (square of amplitude) 9 times the original amplitude of each source of sound.
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