Patent Publication Number: US-7710826-B2

Title: Method and apparatus for measuring sound source distance using microphone array

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
   This application claims the benefit of Korean Patent Application No. 10-2007-0104061, filed on Oct. 16, 2007, in the Korean Intellectual Property Office, the disclosure of which is incorporated herein in its entirety by reference. 
   BACKGROUND 
   1. Field 
   One or more embodiments of the present invention relate to an acoustic system, and more particularly, to a method and apparatus for measuring a distance to a sound source by using a microphone array. 
   2. Description of the Related Art 
   There are various application fields for technology which measures a distance to a sound source by only using an input to a microphone. When a distance to a speaker is known, a volume of a speaker can be regulated according to the distance so that the speaker can be heard well. In addition, during recording, an input-gain of a microphone can be appropriately regulated according to the distance to a speaker. In regulating an input-gain of a microphone based on a volume level, a speaker&#39;s voice cannot be heard if there is a large amount of ambient noise. However, if the distance to the speaker is known, an input-gain of a microphone can be regulated according to the distance. 
   In addition, a map indicating a location of a sound source can be drawn. Here, when a direction of and a distance to a sound source are known, which sound source is located in which location can be measured. In other words, the location generating noise can be determined. In addition, if information on the distance to a sound source is known, such information can be used to classify a sound source according to the distance. Moreover, various signal processing technologies using a distance can be applied to devices with microphones. 
   When a number of sound sources are mixed, technologies for removing only a sound source that is not desired, picking out only a desired sound source, and grouping according to the sound sources, use various sound source characteristics. 
   When noise can be easily detected, noise is removed using noise subtraction from sound in which noise and desired sound sources are mixed so that the desired signals remain. Also, when statistical characteristics of the sound sources are different to each other, a sound sources classifying method using the statistical differences of the sound sources, is used. 
   In addition, in the case of using geometrical characteristics of the sound sources, when the directions between the sound sources are different, only a sound source which can be heard from where the desired sound exists can be detected using a beam-forming technology. In addition to the directions, the distance between a sound source and a microphone is also important as geometrical characteristics of the sound sources. 
   As a method of obtaining the distance between the sound source and the microphone, a technology for calculating the distance between the sound source and the microphone, by using a level difference between a reference microphone and other microphone and an arrival time difference is disclosed. However, in such a method, an attenuation rate according to a distance to a general microphone is used and thus sensitivity according to the distance decreases. Moreover, if the distance of the sound source is to be used in signal processing at a back end, the distance should be measured based on frequency so that more detailed information can be provided. However, the distance based on the frequency cannot be measured using the method described above. 
   SUMMARY 
   One or more embodiments of the present invention provide a method and apparatus for measuring a distance to a sound source, regardless of the strength of the sound source, by using microphone outputs having high sensitivity and each having a different attenuation rate according to the distance by forming a microphone system having a high attenuation rate according to the distance from a microphone to the sound source. 
   Additional aspects and/or advantages will be set forth in part in the description which follows and, in part, will be apparent from the description, or may be learned by practice of the invention. 
   According to an aspect of the present invention, there is provided a method of measuring a distance to a sound source, including combining sound source signals input through at least two microphones and generating at least two microphone output signals, and performing an operation on the generated microphone output signals and calculating a distance to a sound source by using the relationship between a result of the operation and the distance according to a frequency of the input sound source signals. 
   According to another aspect of the present invention, there is provided an apparatus for measuring a distance to a sound source, including at least two microphone output generating units which combine sound source signals input through at least two microphones and generating at least two microphone output signals, and a distance measuring unit which performs an operation on the microphone output signals generated by the microphone output generating units and calculates a distance to a sound source using a relationship between the a result of the operation and the distance according to a frequency of the input sound source signals. 
   According to another aspect of the present invention, there is provided a computer readable recording medium having embodied thereon a computer program for executing the method above. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
     These and/or other aspects and advantages will become apparent and more readily appreciated from the following description of the embodiments, taken in conjunction with the accompanying drawings of which: 
       FIG. 1  is a block diagram schematically illustrating an apparatus for measuring a distance to a sound source, according to an embodiment of the present invention; 
       FIG. 2  is a block diagram schematically illustrating an apparatus for measuring a distance to a sound source, according to another embodiment of the present invention; 
       FIG. 3  is a diagram for describing the direction measuring unit illustrated in  FIG. 2 ; 
       FIGS. 4A through 4C  are diagrams for describing the microphone output generating unit and a distance measuring unit illustrated in  FIG. 1 ; 
       FIG. 5  is a detailed block diagram of an apparatus for measuring a distance to a sound source, according to another embodiment of the present invention; 
       FIGS. 6A through 6C  are diagrams for describing the first microphone output generating unit illustrated in  FIG. 5 ; 
       FIGS. 7A through 7C  are diagrams for describing the second microphone output generating unit illustrated in  FIG. 5 ; and 
       FIG. 8  is a detailed block diagram of the distance measuring unit illustrated in  FIG. 1 . 
   

   DETAILED DESCRIPTION OF THE EMBODIMENTS 
   Reference will now be made in detail to the embodiments, examples of which are illustrated in the accompanying drawings, wherein like reference numerals refer to the like elements throughout. In this regard, embodiments of the present invention may be embodied in many different forms and should not be construed as being limited to embodiments set forth herein. Accordingly, exemplary embodiments are merely described below, by referring to the figures, to explain aspects of the present invention. 
     FIG. 1  is a block diagram schematically illustrating an apparatus for measuring a distance to a sound source  100 , according to an embodiment of the present invention. Herein, in the present application, the term apparatus should be considered synonymous with the term system, and not limited to a single enclosure or all described elements embodied in single respective enclosures in all embodiments, but rather, depending on embodiment, is open to being embodied together or separately in differing enclosures and/or locations through differing elements, e.g., a respective apparatus/system could be a single processing element or implemented through a distributed network, noting that additional and alternative embodiments are equally available. 
   Referring to  FIG. 1 , the apparatus for measuring a distance to a sound source  100  includes a microphone output generating unit  110  and a distance measuring unit  120 . 
   The microphone output generating unit  110  combines sound source signals e 1 , . . . e N , respectively input through at least two microphones Mic  1 , . . . Mic N and generates at least two microphone output signals E 1 , . . . E k , . . . E M . 
   The distance measuring unit  120  performs an operation on the microphone output signals E 1 , . . . E k , . . . E M  which are generated from the microphone output generating unit  110 . Also, the distance measuring unit  120  calculates a distance to a sound source by using the relationship between the operation result and the distance according to a frequency of the input sound source signals. The distance measuring unit  120  will be described in more detail with reference to  FIG. 8 . 
   The microphone output generating unit  110  manufactures outputs of a microphone system and uses at least two microphones Mic  1 , . . . Mic N. Here, characteristics of the microphones can be the same or different from each other. Inputs to these microphones are combined and outputs E 1 -E M  are generated through a first microphone output generating unit, a K th  microphone output generating unit, and an M th  microphone output generating unit. Here, such a combination of inputs to the microphones can be any function including a linear function and a non-linear function. In addition, an attenuation rate according to a distance should be different from each other in outputs from each of the microphone output generating units. Accordingly, regardless of the strength of a sound source, a distance to a sound source can be measured by using the microphone outputs each having a different attenuation rate according to a distance. 
     FIG. 2  is a block diagram schematically illustrating an apparatus for measuring a distance to a sound source  200 , according to another embodiment of the present invention. 
   Referring to  FIG. 2 , the apparatus for measuring a distance to a sound source  200  includes a direction measuring unit  220 , a microphone output generating unit  210  and a distance measuring unit  230 . The direction measuring unit  220  receives sound source signals e 1 , . . . e N , from the microphones Mic  1 , . . . Mic N and calculates input directions E of the sound source signals. 
   Calculating the input directions θ of the sound source signals will be described with reference to  FIG. 3 . 
     FIG. 3  is a diagram for describing a direction measuring unit  220  illustrated in  FIG. 2 . Referring to  FIG. 3 , the directions of the sound sources are obtained by using time delays between the sound source signals input to the microphones Mic  1 , . . . Mic N. That is, a delay-and-sum method is used, which obtains a direction of a sound source by using the time delays between signals and the time delays can be calculated by using a correlation between inputs to the microphones. Also, when a distance to a sound source is very short, compared with an aperture size of the microphone, the sound source can be assumed to be a plane wave. Accordingly, an angle can be obtained using Equations 1 and 2. 
   
     
       
         
           
             
               
                 
                   
                     τ 
                     k 
                   
                   · 
                   c 
                 
                 = 
                 
                   
                     r 
                     · 
                     cos 
                   
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   θ 
                 
               
             
             
               
                 Equation 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 1 
               
             
           
           
             
               
                 θ 
                 = 
                 
                   
                     cos 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       
                         
                           τ 
                           k 
                         
                         · 
                         c 
                       
                       r 
                     
                     ) 
                   
                 
               
             
             
               
                 Equation 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 2 
               
             
           
         
       
     
   
   Here, t k  denotes a delay between a K th  microphone and a K+1 th  microphone and c denotes the speed of a sound wave in air. 
     FIGS. 4A through 4C  are diagrams for describing the microphone output generating unit  110  and the distance measuring unit  120  illustrated in  FIG. 1 . 
     FIG. 4A  illustrates an example of the first microphone output generating unit and  FIG. 4B  illustrates an example of the K th  microphone output generating unit. Here, functions F 1 (•) and F K (•) operate upon attenuation rates of each different sound.  FIG. 4C  illustrates an example of the distance measuring unit  120 . Here, DF(•) can be any function including a linear function and a non-linear function. 
     FIG. 5  is a detailed block diagram of the apparatus for measuring a distance to a sound source  500 , according to another embodiment of the present invention. 
   Referring to  FIG. 5 , microphones M 1 , . . . M 4 ,  101  and  102  respectively, a microphone output generating unit  510  including a first microphone output generating unit  511  and a second microphone output generating unit  512 , and a distance measuring unit  520  are illustrated. 
   Sound source signals e 1 , . . . e 4  input from the microphones M 1 , . . . M 4 ,  101  and  102  respectively, are input to the first microphone output generating unit  511  and the second microphone output generating unit  512 . The first microphone output generating unit  511  is a 2 nd  order gradient microphone system and the second microphone output generating unit  512  is an omni microphone system. In  FIG. 5 , the microphones are 4 omni microphones and use 2 microphone systems. However, the microphones can use two or more microphone systems. In addition, the direction measuring unit  220  of  FIG. 2  can be further included. 
   The relationship between the input and output of the 2 nd  order gradient microphone system is illustrated in  FIGS. 6A through 6C . 
   As illustrated in  FIGS. 6A and 6B , function F 1 (•) can be a linear transformation in which elements of the g matrix, [g11, g22, g33, g44]=[1, −1, −1, 1] and the rest of the g matrix is 0. As illustrated in  FIG. 6C , if the input sound source has the angle θ between a line R from the center of the microphones to the sound source and an x-axis, a microphone output is as given by Equation 3. 
   
     
       
         
           
             
               
                 
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                 Equation 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 3 
               
             
           
         
       
     
   
   The relationship between the input and output of the omni microphone system is illustrated in  FIGS. 7A through 7C . For the sum of the omni microphone, as illustrated in  FIGS. 5A and 5B , function F 2 (•) can be a linear transformation in which elements of matrix g, [g11, g22, g33, g44]=[1, 1, 1, 1] and the rest of the matrix g is 0. As illustrated in  FIG. 5C , if the input sound source has the angle θ between a line R from the center of the microphone to the sound source and an x-axis, a microphone output is as given by Equation 4. 
   
     
       
         
           
             
               
                 
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                                 ⁢ 
                                 
                                   
                                     sin 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ψ 
                                   
                                   
                                     r 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                 
                               
                               ) 
                             
                             2 
                           
                         
                       
                     
                   
                   , 
                   
                     
 
                   
                   ⁢ 
                   where 
                   , 
                   
                     ψ 
                     = 
                     
                       
                         
                           2 
                           ⁢ 
                           π 
                         
                         λ 
                       
                       · 
                       
                         
                           r 
                           ⁡ 
                           
                             ( 
                             j 
                             ) 
                           
                         
                         . 
                       
                     
                   
                 
               
             
             
               
                 Equation 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 4 
               
             
           
         
       
     
   
   Referring back to  FIG. 5 , the distance measuring unit  520  receives the output E 1  of the first microphone output generating unit  511  and the output E 2  of the second microphone output generating unit  512  and an operation is performed to obtain the ratio of E 1  and E 2  as given by Equation 5. 
   
     
       
         
           
             
               
                 
                   
                     E 
                     1 
                   
                   = 
                   
                     A 
                     ⁢ 
                     
                       
                         
                           
                             ( 
                             
                               
                                 ∑ 
                                 
                                   j 
                                   = 
                                   1 
                                 
                                 4 
                               
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 
                                   g 
                                   ⁡ 
                                   
                                     ( 
                                     j 
                                     ) 
                                   
                                 
                                 ⁢ 
                                 
                                   
                                     cos 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ψ 
                                   
                                   
                                     r 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                 
                               
                             
                             ) 
                           
                           2 
                         
                         + 
                         
                           
                             ( 
                             
                               
                                 ∑ 
                                 
                                   j 
                                   = 
                                   1 
                                 
                                 4 
                               
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 
                                   g 
                                   ⁡ 
                                   
                                     ( 
                                     j 
                                     ) 
                                   
                                 
                                 ⁢ 
                                 
                                   
                                     sin 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ψ 
                                   
                                   
                                     r 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                 
                               
                             
                             ) 
                           
                           2 
                         
                       
                     
                   
                 
                 ⁢ 
                 
                   
 
                 
                 ⁢ 
                 
                   
                     E 
                     2 
                   
                   = 
                   
                     A 
                     ⁢ 
                     
                       
                         
                           
                             ( 
                             
                               
                                 ∑ 
                                 
                                   j 
                                   = 
                                   1 
                                 
                                 4 
                               
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 
                                   cos 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   ψ 
                                 
                                 
                                   r 
                                   ⁡ 
                                   
                                     ( 
                                     j 
                                     ) 
                                   
                                 
                               
                             
                             ) 
                           
                           2 
                         
                         + 
                         
                           
                             ( 
                             
                               
                                 ∑ 
                                 
                                   j 
                                   = 
                                   1 
                                 
                                 4 
                               
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               
                                 
                                   sin 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   ψ 
                                 
                                 
                                   r 
                                   ⁡ 
                                   
                                     ( 
                                     j 
                                     ) 
                                   
                                 
                               
                             
                             ) 
                           
                           2 
                         
                       
                     
                   
                 
                 ⁢ 
                 
                   
 
                 
                 ⁢ 
                 
                   
                     
                       E 
                       1 
                     
                     
                       E 
                       2 
                     
                   
                   = 
                   
                     
                       
                         ⁢ 
                         
                           
                             
                               
                                 ( 
                                 
                                   
                                     ∑ 
                                     
                                       j 
                                       = 
                                       1 
                                     
                                     4 
                                   
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     
                                       g 
                                       ⁡ 
                                       
                                         ( 
                                         j 
                                         ) 
                                       
                                     
                                     ⁢ 
                                     
                                       
                                         cos 
                                         ⁢ 
                                         
                                             
                                         
                                         ⁢ 
                                         ψ 
                                       
                                       
                                         r 
                                         ⁡ 
                                         
                                           ( 
                                           j 
                                           ) 
                                         
                                       
                                     
                                   
                                 
                                 ) 
                               
                               2 
                             
                             + 
                             
                               
                                 ( 
                                 
                                   
                                     ∑ 
                                     
                                       j 
                                       = 
                                       1 
                                     
                                     4 
                                   
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     
                                       g 
                                       ⁡ 
                                       
                                         ( 
                                         j 
                                         ) 
                                       
                                     
                                     ⁢ 
                                     
                                       
                                         sin 
                                         ⁢ 
                                         
                                             
                                         
                                         ⁢ 
                                         ψ 
                                       
                                       
                                         r 
                                         ⁡ 
                                         
                                           ( 
                                           j 
                                           ) 
                                         
                                       
                                     
                                   
                                 
                                 ) 
                               
                               2 
                             
                           
                         
                       
                       
                         ⁢ 
                         
                           
                             
                               
                                 ( 
                                 
                                   
                                     ∑ 
                                     
                                       j 
                                       = 
                                       1 
                                     
                                     4 
                                   
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       ψ 
                                     
                                     
                                       r 
                                       ⁡ 
                                       
                                         ( 
                                         j 
                                         ) 
                                       
                                     
                                   
                                 
                                 ) 
                               
                               2 
                             
                             + 
                             
                               
                                 ( 
                                 
                                   
                                     ∑ 
                                     
                                       j 
                                       = 
                                       1 
                                     
                                     4 
                                   
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     
                                       sin 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       ψ 
                                     
                                     
                                       r 
                                       ⁡ 
                                       
                                         ( 
                                         j 
                                         ) 
                                       
                                     
                                   
                                 
                                 ) 
                               
                               2 
                             
                           
                         
                       
                     
                     = 
                     
                       
                         
                           
                             
                               ( 
                               
                                 
                                   ∑ 
                                   
                                     j 
                                     = 
                                     1 
                                   
                                   4 
                                 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   
                                     g 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                   ⁢ 
                                   
                                     
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       ψ 
                                     
                                     
                                       r 
                                       ⁡ 
                                       
                                         ( 
                                         j 
                                         ) 
                                       
                                     
                                   
                                 
                               
                               ) 
                             
                             2 
                           
                           + 
                           
                             
                               ( 
                               
                                 
                                   ∑ 
                                   
                                     j 
                                     = 
                                     1 
                                   
                                   4 
                                 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   
                                     g 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                   ⁢ 
                                   
                                     
                                       sin 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       ψ 
                                     
                                     
                                       r 
                                       ⁡ 
                                       
                                         ( 
                                         j 
                                         ) 
                                       
                                     
                                   
                                 
                               
                               ) 
                             
                             2 
                           
                         
                       
                       
                         
                           
                             
                               ( 
                               
                                 
                                   ∑ 
                                   
                                     j 
                                     = 
                                     1 
                                   
                                   4 
                                 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   
                                     cos 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ψ 
                                   
                                   
                                     r 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                 
                               
                               ) 
                             
                             2 
                           
                           + 
                           
                             
                               ( 
                               
                                 
                                   ∑ 
                                   
                                     j 
                                     = 
                                     1 
                                   
                                   4 
                                 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   
                                     sin 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ψ 
                                   
                                   
                                     r 
                                     ⁡ 
                                     
                                       ( 
                                       j 
                                       ) 
                                     
                                   
                                 
                               
                               ) 
                             
                             2 
                           
                         
                       
                     
                   
                 
                 ⁢ 
                 
                   
 
                 
                 ⁢ 
                 
                   where 
                   , 
                   
                     ψ 
                     = 
                     
                       
                         
                           2 
                           ⁢ 
                           
                             π 
                             · 
                             
                               r 
                               ⁡ 
                               
                                 ( 
                                 j 
                                 ) 
                               
                             
                           
                         
                         λ 
                       
                       = 
                       
                         
                           
                             2 
                             ⁢ 
                             
                               π 
                               · 
                               f 
                               · 
                               
                                 r 
                                 ⁡ 
                                 
                                   ( 
                                   j 
                                   ) 
                                 
                               
                             
                           
                           c 
                         
                         = 
                         
                           
                             2 
                             ⁢ 
                             
                               π 
                               · 
                               f 
                               · 
                               
                                 
                                   
                                     
                                       
                                         
                                           
                                             ( 
                                             
                                               
                                                 x 
                                                 ⁡ 
                                                 
                                                   ( 
                                                   j 
                                                   ) 
                                                 
                                               
                                               - 
                                               
                                                 
                                                   R 
                                                   · 
                                                   cos 
                                                 
                                                 ⁢ 
                                                 
                                                     
                                                 
                                                 ⁢ 
                                                 θ 
                                               
                                             
                                             ) 
                                           
                                           2 
                                         
                                         + 
                                       
                                     
                                   
                                   
                                     
                                       
                                         
                                           ( 
                                           
                                             
                                               y 
                                               ⁡ 
                                               
                                                 ( 
                                                 j 
                                                 ) 
                                               
                                             
                                             - 
                                             
                                               
                                                 R 
                                                 · 
                                                 cos 
                                               
                                               ⁢ 
                                               
                                                   
                                               
                                               ⁢ 
                                               θ 
                                             
                                           
                                           ) 
                                         
                                         2 
                                       
                                     
                                   
                                 
                               
                             
                           
                           c 
                         
                       
                     
                   
                 
               
             
             
               
                 Equation 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 5 
               
             
           
         
       
     
   
   Here, A, which corresponds to the amplitude of the sound source, cancels out by division. Accordingly, regardless of the amplitude of the sound source, a distance to the sound source can be obtained. Thus, E 1 /E 2  can be a function of the frequency f and the distance R. That is, if the value of E 1 /E 2  and the frequency f are known, the distance R can be obtained. 
   Referring back to  FIG. 2 , when additionally a direction of the input sound source signal is considered, if the value of E 1 /E 2  with respect to the input direction θ calculated by the direction measuring unit  220  and the frequency f are known, the distance R can be obtained. 
     FIG. 8  is a detailed block diagram of the distance measuring unit  120  illustrated in  FIG. 1 . 
   Referring to  FIG. 8 , the distance measuring unit  120  includes an output operator  121 , a calculating unit  122 , and a storage unit  123 . 
   The output operator  121  performs an operation upon the microphone output signals E 1 , . . . E M  generated from the microphone output generating unit. For example, as illustrated in  FIG. 5 , an operation is performed using the ratio of E 1  and E 2  with respect to the output E 1  of the first microphone output generating unit  511  and the output E 2  of the second microphone output generating unit  512 . 
   The calculating unit  122  calculates the distance to a sound source by using the relationship between the operation result of the microphone output signals and the distance according to the frequency of the sound source signals. Here, the relationship between the frequency of the input sound source signal and the distance according to the frequency is stored in the storage unit  123 . Accordingly, if the relationship between the output signals of each different microphone output system, for example, the value of E 1 /E 2  in  FIG. 5 , is known, the distance to a sound source having a specific frequency can be calculated by performing an operation. In particular, regardless of the magnitude of sound from a sound source, when a sound source varies with time, the distance can be calculated. 
   In addition to the above described embodiments, embodiments of the present invention can also be implemented on a computer through computer readable code/instructions in/on a medium, e.g., a computer readable medium, to control at least one processing element to implement any above described embodiment. The medium can correspond to any medium/media permitting the storing of the computer readable code. 
   The units discussed herein can be implemented on a computer and the results displayed on a computer display. 
   The computer readable code can be recorded/transferred on a medium in a variety of ways, with examples of the medium including recording media, such as magnetic storage media (e.g., ROM, floppy disks, hard disks, etc.) and optical recording media (e.g., CD-ROMs, or DVDs). 
   The instructions/code can also be transferred over a transmission medium such as media carrying or including carrier waves, as well as elements of the Internet, for example. Thus, the transmission medium may be such a defined and measurable structure including or carrying a signal or information, such as a device carrying a bitstream, for example, according to embodiments of the present invention. The transmission media may also be a distributed network, so that the computer readable code is transferred and executed in a distributed fashion. Still further, as only an example, the computer implementing embodiments of the present invention may include a processor or a computer processor, and processing elements may be distributed and/or included in a single device. 
   While aspects of the present invention has been particularly shown and described with reference to differing embodiments thereof, it should be understood that these exemplary embodiments should be considered in a descriptive sense only and not for purposes of limitation. Descriptions of features or aspects within each embodiment should typically be considered as available for other similar features or aspects in the remaining embodiments. 
   Thus, although a few embodiments have been shown and described, it would be appreciated by those skilled in the art that changes may be made in these embodiments without departing from the principles and spirit of the invention, the scope of which is defined in the claims and their equivalents.