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US-2024422466-A1 · Dec 19, 2024 · US
US9319785B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9319785-B2 |
| Application number | US-201213424869-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 20, 2012 |
| Priority date | Dec 9, 2011 |
| Publication date | Apr 19, 2016 |
| Grant date | Apr 19, 2016 |
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Disclosed is a technique for localizing a sound source. In the technique, a sound pressure signal measured by microphones is acquired using a spherical microphone array sensor where the microphones are fixedly arranged on a surface of a spherical body. A sound pressure distribution on the surface of the spherical body is obtained by a controller from a sound pressure calculation formula for calculating a sound pressure at a certain location of a spherical surface using the sound pressure signal measured by the microphones as an input value. A location of the sound source is estimated from the obtained sound pressure distribution.
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What is claimed is: 1. A method for localizing a sound source, comprising: acquiring, by a controller, a sound pressure signal measured by microphones, using a spherical microphone array sensor wherein the microphones are fixedly arranged on a surface of a spherical body; obtaining a sound pressure distribution on the surface of the spherical body from a sound pressure calculation formula for calculating a sound pressure at a certain location of a spherical surface using the sound pressure signal measured by the microphones as an input value; and estimating a location of the sound source from the obtained sound pressure distribution, wherein, from Equation (1) below the sound pressure calculation formula is obtained by meeting r=a (here, a is a radius of the spherical body) and limiting a sound field distribution order n to a maximum order N of Equation (2) below that considers a total number of microphones; p ( r , θ , ϕ ) = ∑ n = 0 ∞ j n ( kr ) j n ( ka ) ∑ m = - n n Y n m ( θ , ϕ ) ∫ 0 2 π ∫ 0 π p ( a , θ 0 , ϕ o ) Y n m ( θ 0 , ϕ 0 ) * sin θ ⅆ θ ⅆ ϕ ( 1 ) where j n (kr) is a spherical Bessel function, n is an order of sound field distribution, m={−n, −n−1, . . . , 0, 1, . . . , n−1, n}, Y n m (θ,φ) are spherical harmonic functions, r denotes a radius of a sphere, θ denotes a horizontal angle of a spherical coordinate, φ denotes a vertical angle of the spherical coordinate, θ 0 and φ o denote the horizontal angle and the vertical angle of microphone location respectively, and p(a,θ 0 ,φ o ) denotes a sound pressure mea
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