Abstract:
A single point detecting current sensor includes a plurality of magnetic sensor modules, wherein a magnetic sensor module is installed onto each busbars with an insulation displacement contact or is installed adjacent to each busbar, and outputs the current through a busbars measured by a magnetic sensor; a signal collection module collecting measured signals output by the plurality of magnetic sensor modules; and a signal interference compensation module deriving a corrected current value for which interference has been removed, by calculating the mutual interference between said busbars using the signals collected by said signal collection module.

Description:
BACKGROUND 
     The present invention relates to a single point detection current sensor and, more particularly, to an interference correction type single-point detection current sensor for multiple busbars. 
     A method of measuring the amount of current in a contactless way in a panel board and a switch board includes a method using a current transformer and a method using a magnetic sensor. A method using a circular core as in a current transformer is a method of measuring the amount of current through induced electromotive force according to an induced magnetic flux that is formed in the core itself. Such a method has relatively small interference with other power lines, but requires a great installation space because an induced magnetic flux is formed while circulating the core. Furthermore, such a method is vulnerable to a mechanical deformation attributable to vibration or a mechanical shock and has a safety problem in installation and between control systems in an environment in which insulation has not been provided as in a busbar. 
     In contrast, the magnetic sensor method is a method of disposing sensors capable of measuring a magnetic flux, such as hall sensors, on the periphery of busbars, directly measuring the amount of a magnetic flux, and converting the measured amount into the amount of current (refer to Korean Patent Application Nos. 10-2009-0075419 and 10-2012-0028306). A single-point detection type current sensor for obtaining information about current that flows at a single point location of wire or a busbar using a magnetic sensor as described above is advantageous in that the installation of equipment is easy, but has a problem in that the sensor itself is greatly influenced by environments, such as a temperature and the distance, and a problem in that an error of a measured value is severely generated due to severe interference between lines in an environment in which multiple busbars connected to a high-power load are concentrated. 
     The inventor of the present invention has developed a current sensor having improved measurement accuracy by removing interference occurring between busbars while maintaining the advantage of the magnetic sensor method in order to measure the amount of current in an environment in which a plurality of busbars is concentrated (multiple busbars). 
     SUMMARY OF THE INVENTION 
     The present invention has been proposed in order to solve the above problems of the existing proposed methods, and an object of the present invention is to provide an interference correction type single-point detection current sensor for multiple busbars, which does not have interference between lines and has significantly improved accuracy in measuring the amount of current by including a signal interference correction module for deriving corrected current values from which interference has been removed by calculating the amounts of interference between a plurality of busbars. 
     Another object of the present invention is to provide an interference correction type single-point detection current sensor for multiple busbars, wherein the signal interference correction module is configured to include an interference coefficient matrix generation unit, an interference coefficient derivation unit, and a correction current value calculation unit, thereby being capable of deriving a corrected current value from which interference is simply removed based on an interference coefficient matrix and calculation. 
     Yet another object of the present invention is to provide an interference correction type single-point detection current sensor for multiple busbars, wherein a plurality of interference coefficient matrices is generated according to a temperature, the amount of current, the location where current is measured, and the distance between busbars, the plurality of generated interference coefficient matrices is stored, and an interference coefficient matrix suitable for a corresponding temperature, amount of current, and distance is used, thereby minimizing the occurrence of an error attributable to various variables. 
     An interference correction type single-point detection current sensor for multiple busbars according to an aspect of the present invention for accomplishing the above objects includes a plurality of magnetic sensor modules which are brought in insulation contact with or installed adjacent to a plurality of respective busbars, measure currents flowing into the busbars using magnetic sensors, and output the measured currents; a signal collection module which collects the measured signals output by the plurality of magnetic sensor modules; and a signal interference correction module which derives corrected current values from which interference has been removed by calculating the amounts of interference between the plurality of busbars in the signals collected by the signal collection module. 
     Preferably, the magnetic sensor module may be configured to include the magnetic sensor which is brought in insulation contact with or installed adjacent to the busbar and collects a magnetic field line generated by a current flowing into the busbar and a signal analysis circuit which calculates back to information about a current that flows into the busbar by analyzing a signal collected by the magnetic sensor. 
     Preferably, the signal interference correction module may be configured to include an interference coefficient matrix generation unit which generates an interference coefficient matrix; an interference coefficient derivation unit which derives the interference coefficient of a corresponding busbar using the interference coefficient matrix or an interpolation method; and a correction current value calculation unit which derives the corrected current value using the derived corresponding interference coefficient. 
     More preferably, the signal interference correction module may further include interference correction memory which stores an interference correction equation for deriving the corrected current value using the interference coefficient matrix generated by the interference coefficient matrix generation unit and the interference coefficient. The interference coefficient derivation unit and the correction current value calculation unit may read a value necessary to correct the interference of the measured signal from the interference correction memory and calculate the corrected current value. 
     More preferably, a plurality of the interference coefficient matrices may be generated in each predetermined unit within a predetermined range of one or more variables selected from a group including a temperature, current, and measured location, and distance between the busbars. 
     Preferably, the interference coefficient matrix may be modeled and generated according to the following equation. 
     
       
         
           
             
               
                 
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     (wherein B=a magnetic flux density, u 0 =permeability in vacuum, I=current, r=a distance from a conductor (a distance from the busbar or an adjacent busbar), dl=a curvilinear integral of a current direction, and r^=a unit vector in a direction r) 
     Preferably, the single-point detection current sensor may further include a temperature measurement module. A plurality of interference coefficient matrices may be generated in each predetermined unit within a predetermined temperature range, and the signal interference correction module may derive the corrected current value using the interference coefficient matrix that complies with a temperature measured by the temperature measurement module. 
     Preferably, the single-point detection current sensor may further include a measurement error correction module which derives the measurement error correction value of each sensor by calculating environment variables, including a temperature, distance from the busbar, and intensity of a magnetic flux in the measured signal output by the magnetic sensor module. The signal interference correction module may derive the corrected current value based on the measurement error correction value derived by the measurement error correction module. 
     In accordance with the interference correction type single-point detection current sensor for multiple busbars proposed by the present invention, since the signal interference correction module for deriving corrected current values from which interference has been removed by calculating the amounts of interference between a plurality of busbars is included, interference between lines is removed, and accuracy in measuring the amount of current is significantly improved. 
     Furthermore, in accordance with the present invention, a corrected current value from which interference is simply removed can be derived based on an interference coefficient matrix and calculation because the signal interference correction module is configured to include an interference coefficient matrix generation unit, an interference coefficient derivation unit, and a correction current value calculation unit. 
     Furthermore, in accordance with the present invention, the occurrence of an error attributable to various variables can be minimized because a plurality of interference coefficient matrices is generated according to a temperature, the amount of current, the location where current is measured, and the distance between busbars, the plurality of generated interference coefficient matrices is stored, and an interference coefficient matrix suitable for a corresponding temperature, amount of current, and distance is used. 
    
    
     
       BRIEF DESCRIPTION OF DRAWINGS 
         FIG. 1  is a diagram illustrating the configuration of an interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. 
         FIG. 2  is a diagram illustrating a process of measuring current through the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. 
         FIG. 3  is a diagram illustrating the current measurement method of a magnetic sensor module in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. 
         FIG. 4  is a diagram illustrating a case where interference is generated due to current that flows into a busbar adjacent to a single busbar in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. 
         FIG. 5  is a diagram illustrating a detailed configuration of a signal interference correction module in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. 
         FIG. 6  is a diagram illustrating a structure for modeling an interference equation in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. 
         FIG. 7  is a diagram illustrating the configuration of an interference correction type single-point detection current sensor for multiple busbars in accordance with another embodiment of the present invention. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     Hereinafter, preferred embodiments are described in detail with reference to the accompanying drawings so that those skilled in the art to which the present invention pertains may easily practice the present invention. In this case, in describing the preferred embodiments of the present invention in detail, a detailed description of the known functions or elements will be omitted if it is deemed to make the gist of the present invention unnecessarily vague. Furthermore, the same reference numerals designate elements having similar functions and operations throughout the drawings. 
     In addition, throughout the specification, when it is described that one element is ‘connected’ to the other element, the one element may be ‘directly connected’ to the other element or ‘indirectly connected’ to the other element through another element. Furthermore, when it is described that one element ‘includes’ another element, it means that the one element does not exclude another element, but may include other elements, unless otherwise described. 
       FIG. 1  is a diagram illustrating the configuration of an interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention, and  FIG. 2  is a diagram illustrating a process of measuring current through the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. As illustrated in  FIG. 1 , the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention may be configured to include magnetic sensor modules  100 , a signal collection module  200 , and a signal interference correction module  300 . More specifically, in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention, as illustrated in  FIG. 2 , the N magnetic sensor modules  100  installed adjacent to respective N busbars  10  may measure the amounts of current I 0 , I 1 , . . . , I n , . . . , I N  in their respective locations. The signal collection module  200  may collect the measured amounts (measured signals) and transfer the collected amounts to the signal interference correction module  300 . The signal interference correction module  300  may derive corrected current values I′ 0 , I′  1 , . . . , I′  n , . . . , I′ N  from which interference has been removed by calculating the amount of interference between the busbars. Each of the elements of the single-point detection current sensor proposed by the present invention is described below. 
     The magnetic sensor modules  100  are brought in insulation contact with or installed adjacent to the plurality of respective busbars  10 , and they may measure currents flowing into the busbars  10  using magnetic sensors and output the measured currents. Since the magnetic sensor modules  100  are installed in the respective busbars, the magnetic sensor modules  100  and the busbars  10  may be configured to have the same number. The magnetic sensor modules  100  may function to convert magnetic field lines, generated by currents flowing into the multiple busbars  10 , into electrical signals.  FIG. 3  is a diagram illustrating the current measurement method of the magnetic sensor module in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. As illustrated in  FIG. 3 , when current flows into the busbar  10 , a magnetic field line is formed according to the right-handed screw rule. The magnetic sensor module  100  may convert the magnetic field line into an electrical signal and measure current flowing into the busbar  10 . 
     In accordance with an embodiment of the present invention, the magnetic sensor module  100  may be configured to include a magnetic sensor which is brought in insulation contact with or installed adjacent to the busbar  10  and which collects a magnetic field line generated by current flowing into the busbar  10  and a signal analysis circuit which interprets a signal collected by the magnetic sensor and calculates back to information about current that flows into the busbar  10 . The magnetic sensor may use a hall sensor, but is not limited thereto. Various sensors may be used as the magnetic sensor. 
       FIG. 4  is a diagram illustrating a case where interference is generated due to current that flows into a busbar adjacent to a single busbar in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. As illustrated in  FIG. 4 , if several busbars  10  are disposed as in a common switch board or panel board environment, a magnetic sensor module  101  mounted on a busbar  11  whose amount of current is to be measured is also influenced by a magnetic field that is subject to interference attributable to current flowing into an adjacent busbar  12  in addition to current flowing into the corresponding busbar  11 . This may be a further serious problem if the distance between the busbars  10  is close, if current flowing into an adjacent busbar is strong, or if perfect shielding is difficult due to a problem, such as the discharging of high voltage. Furthermore, although physical shielding is performed, a certain amount of an interference phenomenon is generated because a leaking magnetic field is not perfectly shielded. In order to solve such a problem, the inventor of the present invention proposes that an accurately corrected current value from which interference has been removed can be derived using an interference coefficient, formulated or modeled from a previously measured value, in a measured signal measured by each busbar  10  by including the signal collection module  200  and the signal interference correction module  300 . 
     The signal collection module  200  may function to collect measured signals output by the plurality of magnetic sensor modules  100  and transfer the collected signals to the signal interference correction module  300 . 
     The signal interference correction module  300  may derive corrected current values from which interference has been removed by calculating the amounts of interference between the plurality of busbars  10  in the signal collected by the signal collection module  300 . 
       FIG. 5  is a diagram illustrating a detailed configuration of a signal interference correction module in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. As illustrated in  FIG. 5 , the signal interference correction module  300  of the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention may be configured to further include an interference coefficient matrix generation unit  310 , an interference coefficient derivation unit  320 , and a correction current value calculation unit  330 . In some embodiments the signal interference correction module  300  may be configured to include interference correction memory  340 . 
     The interference coefficient matrix generation unit  310  may generate an interference coefficient matrix. The interference coefficient may be represented by h n,m , which means the amount of current that flows into an n th  busbar  10  and that interferes with an m th  busbar  10 .  FIG. 6  is a diagram illustrating a structure for modeling an interference equation in the interference correction type single-point detection current sensor for multiple busbars in accordance with an embodiment of the present invention. As illustrated in  FIG. 6 , the amount of interference current measured by an (n+1) th  magnetic sensor modules  100  due to current I′ n  actually flowing into the n th  busbar  10  may be represented by h n,n+1 *I′ n . Accordingly, current In measured by the n th  busbar  10  may be represented by the amounts of interference current h 0, n *I′ 0 +h 1, n *I′ 1 +h 2, n *I′ 2  . . . based on the amount of current I′n actually flowing into the n th  busbar  10  and the amounts of current I′ 0 , I′ 1 , I′ n−1 , and I′ n+1  flowing into adjacent busbars  10 . 
     Assuming that a matrix indicative of current actually flowing into each busbar  10  is I′ and a matrix indicative of current measured by the magnetic sensor modules  100  is I, a measured current I may be equal to H*I′ (a value obtained by multiplying actual current by an interference coefficient) according to an interference coefficient matrix H (refer to Equation 1 and a matrix below). That is, the measured current I may be considered to be a value influenced by interference attributable to the actual current I′ that flows into the adjacent busbars  10 . The interference coefficient matrix H may be defined in a table form by measuring a temperature and the distance through experiments. If H is the function of I′, that is, if H is influenced by I′, I′ may be calculated as a converging value by repeatedly calculating I=H −1 *I and obtaining H after obtaining h in the state in which the initial value of I′ is set to I. 
     
       
         
           
             
               
                 
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     h 00 , h 11 , h 22 , and h NN  denote ratios of the busbars  10  to be measured which are influenced by the respective busbars  10  and each may be 1, but may not be 1 depending on variables, such as a temperature, the amount of current, and the distance. The aforementioned interference coefficient matrix may be derived in an equation form according to the physical shape of the busbars  10  and the magnetic sensor modules  100  or may be derived by measurement in an actual environment. Furthermore, the aforementioned interference coefficient matrix may be featured according to environment variables, such as a temperature, the distance from a busbar, and the intensity of a magnetic flux, and a value in an environment in which measurement is not performed may be estimated through an interpolation method. 
     Experimentally, if current is made sequentially flow into the busbars and measured, when current of 1 A flows into only a No. 1 busbar  10 , 
     that is, if an actual current (I′) matrix is 
     
       
         
           
             
               
                 
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     a measured current I 0  in a No. 0 busbar is I 0 =h 0,0 *I′ 0 +h 1,0 *I′ 1 +h 2,0 *I′ 2 + . . . +h n,0 *I′ n + . . . +h N,0 *I′ N . 
     (In this case, I=current measured by the magnetic sensor module, h n, m =an interference coefficient of current that flows into the n th  busbar and that interferes with the m th  busbar, I′=actual current, n=order of a busbar to be measured) 
     If the actual current is substituted in the measured current, I 0 =h 1,0 *I′ 1 . That is, if current of 0.1 A is measured in the No. 0 busbar  10  when an actual current of 1 A flows into the No. 1 busbar  10 , the No. 0 busbar  10  is subject to interference of 10% due to the No. 1 busbar  10 . In this case, an interference coefficient h 1.0  becomes 0.1. 
     Meanwhile, although the busbars  10  are assumed to be very regularly installed, such an interference coefficient has a basic physical difference attributable to the distance between the busbars  10  and the distance between the magnetic sensor module  100  and the busbar  10 . Accordingly, an interference coefficient needs to be calculated in each of the regularly configured busbars  10 . 
     Meanwhile, the interference coefficient may differ depending on a temperature, the intensity of a magnetic flux (the amount of current), and the distance between a measured location and the busbar  10 . Preferably, a plurality of the interference coefficient matrices may be generated in each predetermined unit within a predetermined range of one or more variables selected from the group consisting of a temperature, the amount of current, and the distance between a measured location and the busbar  10 . The plurality of generated interference coefficient matrices may be stored in the interference correction memory  340  or another separate memory. 
     That is, the interference coefficient may be measured based on a temperature and the intensity of a magnetic flux. The amount of physical interference is proportional to the amount of current, but may be different depending on the arrangement of busbars and a degree that interference is shielded. The matrix H according to a temperature and the amount of current may be derived by measuring the interference coefficient using a different amount of current for each temperature in the aforementioned experiments, and a coefficient may be extracted using an interpolation method with respect to a required part and may be used. Accordingly, a plurality of the matrices H may be present with respect to a temperature value and a current value. 
     Input for selecting the actual coefficient includes a temperature and the intensity of current. Reference may be made to a coefficient corresponding to a temperature value suitable to a matrix H using the temperature value measured by a temperature sensor. As a similar method, a matrix value for the intensity of current has only to be selected based on the current I measured after a temperature value is determined. For example, the aforementioned experiments correspond to a case where the matrices were measured using the amounts of current 1 A, 10 A, 25 A, and 50 A at temperatures of −40 degrees, −20 degrees, 0 degrees, 20 degrees, 40 degrees, 60 degrees, and 80 degrees with respect to the busbar  10  of 50 A standard, which is represented by H(T, C) for convenience sake. In this case, T is assumed to be a temperature, and C is assumed to be the amount of current. With respect to such a combination, the matrix H has a total number of 4 (the number of types of the amounts of current)*7(the number of types of temperature) types=28 types. If a temperature when the busbar  10  operates is about 40 degrees, the amount of current I′ 0  is 10 A, and the amount of current I′ 1  is 20 A, H(T, C) results in H(T=40 degrees, C=10 A) because the first row of the matrix H is an interference coefficient attributable to I′ 0 , and H(T, C) results in H(T=40 degrees, C=20 A) because the second row is an interference coefficient attributable to I′ 1 . If a temperature or a current value is not included in the table, H(T, C) may be calculated using an interpolation method. 
     Mathematical modeling is possible because an influence attributable to the distance and the amount of current that belong to the interference coefficients corresponds to a physical phenomenon. The interference coefficient matrix may be modeled based on the distance from the busbar and the amount of current measured in the busbar because a magnetic flux density B is in inverse proportion to the distance and is proportional to the amount of current. 
     That is, the interference coefficient matrix may be modeled and generated according to the following equation. 
     
       
         
           
             
               
                 
                   B 
                   = 
                   
                     
                       
                         
                           
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                             0 
                           
                           ⁢ 
                           I 
                         
                         
                           4 
                           ∏ 
                         
                       
                       ⁢ 
                       
                         ∫ 
                         
                           
                             d 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             l 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             X 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               r 
                               ^ 
                             
                           
                           
                             r 
                             2 
                           
                         
                       
                     
                     = 
                     
                       
                         
                           
                             u 
                             0 
                           
                           ⁢ 
                           I 
                         
                         
                           4 
                           ∏ 
                         
                       
                       · 
                       
                         I 
                         r 
                       
                     
                   
                 
               
               
                 
                   Equation 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   2 
                 
               
             
           
         
       
     
     (In this case, B=a magnetic flux density, u 0 =permeability in vacuum, I=current, r=the distance from a conductor (the distance from the busbar or an adjacent busbar), dl=the curvilinear integral of a current direction, and r^=a unit vector in a direction r) 
     In summary, each element h n, m  of the matrix H may be considered to be a function, such as each distance, current, shielding, or temperature. The element may be determined by performing measurement for each temperature, for each current, and for each distance, performing measurement in the state in which the busbar  10  has been installed, or performing modeling. 
     The interference coefficient derivation unit  320  may derive the interference coefficient of a corresponding busbar  10  using an interference coefficient matrix or an interpolation method. The correction current value calculation unit  330  may derive a corrected current value using a corresponding interference coefficient. 
     Furthermore, the interference correction memory  340  may store the interference coefficient matrix generated by the interference coefficient matrix generation unit and an interference correction equation for deriving the corrected current value using an interference coefficient. The interference coefficient derivation unit  320  and the correction current value calculation unit  330  may read a value necessary to correct the interference of a measured signal from the interference correction memory  340  and calculate the corrected current value. 
     Meanwhile, an actual interference coefficient having sufficient accuracy may be obtained by taking into consideration only interference with a secondarily adjacent busbar because interference in the busbar  10  is rapidly attenuated according to the distance. Accordingly, the actual interference coefficient may be represented very simply as in the following equation and the matrix. 
     
       
         
           
             
               
                 
                   
                     I 
                     n 
                   
                   = 
                   
                       
                   
                   ⁢ 
                   
                     
                       
                         h 
                         
                           
                             n 
                             - 
                             2 
                           
                           , 
                           n 
                         
                       
                       * 
                       
                         I 
                         
                           n 
                           - 
                           2 
                         
                         ′ 
                       
                     
                     + 
                     
                       
                         h 
                         
                           
                             n 
                             - 
                             1 
                           
                           , 
                           n 
                         
                       
                       * 
                       
                         I 
                         
                           n 
                           - 
                           1 
                         
                         ′ 
                       
                     
                     + 
                     
                       
                         h 
                         
                           n 
                           , 
                           n 
                         
                       
                       * 
                       
                         I 
                         n 
                         ′ 
                       
                     
                     + 
                     
                       
                         h 
                         
                           
                             n 
                             + 
                             1 
                           
                           , 
                           n 
                         
                       
                       * 
                       
                         I 
                         
                           n 
                           + 
                           1 
                         
                         ′ 
                       
                     
                     + 
                     
                       
                         h 
                         
                           
                             n 
                             + 
                             2 
                           
                           , 
                           n 
                         
                       
                       * 
                       
                         
                           I 
                           
                             n 
                             + 
                             2 
                           
                           ′ 
                         
                         . 
                       
                     
                   
                 
               
               
                 
                   Equation 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   3 
                 
               
             
             
               
                 
                   
                     [ 
                     
                       
                         
                           
                             I 
                             0 
                           
                         
                       
                       
                         
                           
                             I 
                             1 
                           
                         
                       
                       
                         
                           
                             I 
                             2 
                           
                         
                       
                       
                         
                           
                             I 
                             3 
                           
                         
                       
                       
                         
                           · 
                         
                       
                       
                         
                           · 
                         
                       
                       
                         
                           · 
                         
                       
                       
                         
                           
                             I 
                             n 
                           
                         
                       
                       
                         
                           · 
                         
                       
                       
                         
                           · 
                         
                       
                       
                         
                           · 
                         
                       
                     
                     ] 
                   
                   = 
                   
                     
                       [ 
                       
                         
                           
                             
                               h 
                               
                                 0 
                                 , 
                                 0 
                               
                             
                           
                           
                             
                               h 
                               
                                 1 
                                 , 
                                 0 
                               
                             
                           
                           
                             
                               h 
                               
                                 2 
                                 , 
                                 0 
                               
                             
                           
                           
                             0 
                           
                           
                             0 
                           
                           
                             … 
                           
                           
                             0 
                           
                         
                         
                           
                             
                               h 
                               
                                 0 
                                 , 
                                 1 
                               
                             
                           
                           
                             
                               h 
                               
                                 1 
                                 , 
                                 1 
                               
                             
                           
                           
                             
                               h 
                               
                                 2 
                                 , 
                                 1 
                               
                             
                           
                           
                             
                               h 
                               
                                 3 
                                 , 
                                 1 
                               
                             
                           
                           
                             0 
                           
                           
                             … 
                           
                           
                             0 
                           
                         
                         
                           
                             
                               h 
                               
                                 0 
                                 , 
                                 2 
                               
                             
                           
                           
                             
                               h 
                               
                                 1 
                                 , 
                                 2 
                               
                             
                           
                           
                             
                               h 
                               
                                 2 
                                 , 
                                 2 
                               
                             
                           
                           
                             
                               h 
                               
                                 3 
                                 , 
                                 2 
                               
                             
                           
                           
                             
                               h 
                               
                                 4 
                                 , 
                                 2 
                               
                             
                           
                           
                             … 
                           
                           
                             0 
                           
                         
                         
                           
                             0 
                           
                           
                             
                               h 
                               
                                 1 
                                 , 
                                 3 
                               
                             
                           
                           
                             
                               h 
                               
                                 2 
                                 , 
                                 3 
                               
                             
                           
                           
                             
                               h 
                               
                                 3 
                                 , 
                                 3 
                               
                             
                           
                           
                             
                               h 
                               
                                 4 
                                 , 
                                 3 
                               
                             
                           
                           
                             … 
                           
                           
                             0 
                           
                         
                         
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             
                                 
                             
                           
                           
                             · 
                           
                         
                         
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             … 
                           
                           
                             · 
                           
                         
                         
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             
                                 
                             
                           
                           
                             
                                 
                             
                           
                         
                         
                           
                             0 
                           
                           
                             … 
                           
                           
                             
                               h 
                               
                                 
                                   n 
                                   - 
                                   2 
                                 
                                 , 
                                 n 
                               
                             
                           
                           
                             
                               h 
                               
                                 
                                   n 
                                   - 
                                   1 
                                 
                                 , 
                                 n 
                               
                             
                           
                           
                             
                               h 
                               
                                 n 
                                 , 
                                 n 
                               
                             
                           
                           
                             
                                 
                             
                           
                           
                             
                                 
                             
                           
                         
                         
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             
                                 
                             
                           
                           
                             
                                 
                             
                           
                         
                         
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             
                                 
                             
                           
                           
                             
                                 
                             
                           
                         
                         
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             · 
                           
                           
                             
                                 
                             
                           
                           
                             
                                 
                             
                           
                         
                       
                       ] 
                     
                     = 
                     
                       [ 
                       
                         
                           
                             
                               I 
                               0 
                               ′ 
                             
                           
                         
                         
                           
                             
                               I 
                               1 
                               ′ 
                             
                           
                         
                         
                           
                             
                               I 
                               2 
                               ′ 
                             
                           
                         
                         
                           
                             
                               I 
                               3 
                               ′ 
                             
                           
                         
                         
                           
                             · 
                           
                         
                         
                           
                             · 
                           
                         
                         
                           
                             · 
                           
                         
                         
                           
                             
                               I 
                               n 
                               ′ 
                             
                           
                         
                         
                           
                             · 
                           
                         
                         
                           
                             · 
                           
                         
                         
                           
                             · 
                           
                         
                       
                       ] 
                     
                   
                 
               
               
                 
                     
                 
               
             
           
         
       
     
     (In this case, I=current measured by the magnetic sensor module, h n, m =the interference coefficient of current that flows into the n th  busbar and that interferes with the m th  busbar, I′=an actual current, and n=order of a busbar to be measured) 
     The above example illustrates an example in which the interference of a signal sampled on a time axis has been removed. If the interference of current remains constant for a short time, the amount of currents I′ and I may be converted into complex numbers by taking a phase into consideration and calculated at once without calculating them for each current sampling value, thereby being capable of reducing a total computation load. 
       FIG. 7  is a diagram illustrating the configuration of an interference correction type single-point detection current sensor for multiple busbars in accordance with another embodiment of the present invention. As illustrated in  FIG. 7 , the interference correction type single-point detection current sensor for multiple busbars in accordance with another embodiment of the present invention may be configured to further include a temperature measurement module  400 . A plurality of interference coefficient matrices may be generated in each predetermined unit within a predetermined temperature range and stored. The signal interference correction module  300  may derive a corrected current value using an interference coefficient matrix that complies with a temperature measured by the temperature measurement module  400 . 
     Furthermore, the single-point detection current sensor may be configured to further include a measurement error correction module  500  for deriving a measurement error correction value for each sensor by calculating environment variables, including a temperature, the distance from the busbar, and the intensity of a magnetic flux, with respect to a measured signal output by the magnetic sensor module. The signal interference correction module  300  may derive a corrected current value based on a measurement error correction value derived by the measurement error correction module. Each of the magnetic sensor modules  100  may have an error attributable to environment variables, such as a temperature, the distance, and the intensity of a magnetic flux, and thus may derive a measurement error correction variable according to environment variables, such as a temperature and the distance, by comparing the measured amount of current, measured by each busbar not having interference, with the actual amount of current. Such a measurement error correction variable may be stored in separate memory and used. 
     The present invention described above may be modified or applied in various ways by those skilled in the art to which the present invention pertains, and the scope of a technical spirit according to the present invention should be determined by the following claims. 
     
       
         
               
             
               
               
               
             
               
               
             
           
               
                   
               
               
                 &lt;Description of the Reference Numerals&gt; 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                   
                 10: busbar 
                 11: busbars to be measured 
               
               
                   
                 12: adjacent busbar 
                 100: magnetic sensor module 
               
             
          
           
               
                   
                 101: adjacent magnetic sensor module 
               
               
                   
                 102: adjacent magnetic sensor module 
               
               
                   
                 200: signal collection module 
               
               
                   
                 300: signal interference correction module 
               
               
                   
                 310: interference coefficient matrix generation unit 
               
               
                   
                 320: interference coefficient derivation unit 
               
               
                   
                 330: correction current value calculation unit 
               
               
                   
                 340: interference correction memory 
               
               
                   
                 400: temperature measurement module 
               
               
                   
                 500: measurement error correction module