Measurement microphone calibration

<h2 id="reciprocity-calibration">Reciprocity calibration</h2>
Reciprocity calibration is currently the favoured <a href="/facts/Primary_standard/h8nX7X9K">primary standard</a> for calibration of measurement microphones. The technique exploits the reciprocal nature of certain transduction mechanisms such as the electrostatic transducer principle used in <a href="/facts/Condenser_microphones/7YWGlXCl"> condenser measurement microphones</a>. In order to carry out a reciprocity calibration, three uncalibrated microphones 
 
 
 
 i
 
 
 {\displaystyle i}
 
, 
 
 
 
 j
 
 
 {\displaystyle j}
 
 and 
 
 
 
 k
 
 
 {\displaystyle k}
 
 are used. Microphones 
 
 
 
 i
 
 
 {\displaystyle i}
 
 and 
 
 
 
 j
 
 
 {\displaystyle j}
 
 are placed facing each other with a well known acoustical coupler between their <a href="/facts/Diaphragm_(acoustics)/fYq3PwtC"> diaphragms</a>, allowing the <a href="/facts/Acoustic_impedance/FdXaKVjo"> acoustic transfer impedance</a> 
 
 
 
 
 Z
 
 ac
 
 
 
 
 {\displaystyle Z_{\text{ac}}}
 
 to be easily modelled. One of the microphones is then driven by a current 
 
 
 
 
 I
 
 i
 
 
 
 
 {\displaystyle I_{i}}
 
 to act as the source of sound and the other responds to the pressure generated in the coupler, producing an output voltage 
 
 
 
 
 U
 
 j
 
 
 
 
 {\displaystyle U_{j}}
 
 resulting in the electrical transfer impedance 
 
 
 
 
 Z
 
 i
 j
 
 
 
 
 {\displaystyle Z_{ij}}
 
. Provided that the microphones are reciprocal in behaviour, which means the open circuit sensitivity in V/Pa as a receiver is the same as the sensitivity in m3/s/A as a transmitter, it can be shown that the product of the transmission factors 
 
 
 
 
 M
 
 i
 
 
 
 
 {\displaystyle M_{i}}
 
, 
 
 
 
 
 M
 
 j
 
 
 
 
 {\displaystyle M_{j}}
 
, and the acoustical transfer impedance equals the electrical transfer impedance.

Z
          
            i
            j
          
        
        =
        
          
            
              U
              
                j
              
            
            
              I
              
                i
              
            
          
        
        =
        
          M
          
            i
          
        
        
        
          Z
          
            ac
          
        
        
        
          M
          
            j
          
        
      
    
    {\displaystyle Z_{ij}={\frac {U_{j}}{I_{i}}}=M_{i}\;Z_{\text{ac}}\;M_{j}}

Having determined the product of the transmission factors for one pair of microphones, the process is repeated with the other two possible pair-wise combinations 
 
 
 
 i
 k
 
 
 {\displaystyle ik}
 
 and 
 
 
 
 j
 k
 
 
 {\displaystyle jk}
 
. The set of three measurements then allows the individual microphone transmission factor to be deduced by solving three simultaneous equations.

M
          
            i
          
        
        =
        
          
            
              
                1
                
                  Z
                  
                    ac
                  
                
              
            
            
              
                
                  
                    Z
                    
                      i
                      j
                    
                  
                  
                    Z
                    
                      i
                      k
                    
                  
                
                
                  Z
                  
                    j
                    k
                  
                
              
            
          
        
      
    
    {\displaystyle M_{i}={\sqrt {{\frac {1}{Z_{\text{ac}}}}{\frac {Z_{ij}Z_{ik}}{Z_{jk}}}}}}

The electrical transfer impedance is determined during the calibration procedure by measuring the current and voltage and the acoustic transfer impedance depends on the acoustical coupler.

Z
          
            ac
          
        
        =
        
          
            p
            Q
          
        
        =
        
          
            F
            
              v
              
                S
                
                  2
                
              
            
          
        
      
    
    {\displaystyle Z_{\text{ac}}={\frac {p}{Q}}={\frac {F}{vS^{2}}}}

Commonly used acoustical couplers are <a href="/facts/Anechoic_chamber/J6XjAMKx"> free field</a>, diffuse field and compression chamber. For free field conditions between the two microphones the sound pressure in the far field can be calculated and it follows

Z
          
            
              ac
            
            ,
            
            
              free
            
          
        
        =
        
          
            
              
                ρ
                
                  0
                
              
              ω
            
            
              4
              π
              r
            
          
        
        
          e
          
            −
            
              
                m
                2
              
            
            r
          
        
        
          e
          
            −
            j
            (
            k
            r
            −
            
              
                π
                2
              
            
            )
          
        
      
    
    {\displaystyle Z_{{\text{ac}},\,{\text{free}}}={\frac {\rho _{0}\omega }{4\pi r}}e^{-{\frac {m}{2}}r}e^{-j(kr-{\frac {\pi }{2}})}}

where 
 
 
 
 r
 
 
 {\displaystyle r}
 
 is the distance between the microphones. For diffuse field conditions follows

Z
          
            
              ac
            
            ,
            
            
              diff
            
          
        
        =
        
          
            
              
                ρ
                
                  0
                
              
              ω
            
            
              π
              A
            
          
        
        =
        
          
            
              
                ρ
                
                  0
                
              
              ω
            
            
              4
              π
              
                d
                
                  c
                
              
            
          
        
      
    
    {\displaystyle Z_{{\text{ac}},\,{\text{diff}}}={\frac {\rho _{0}\omega }{\sqrt {\pi A}}}={\frac {\rho _{0}\omega }{4\pi d_{c}}}}

where 
 
 
 
 A
 
 
 {\displaystyle A}
 
 is the equivalent absorption area and 
 
 
 
 
 d
 
 c
 
 
 
 
 {\displaystyle d_{c}}
 
 is the <a href="/facts/Critical_distance/pPnS7bcK">critical distance</a> for reverberation. For compression chamber conditions follows

Z
          
            
              ac
            
            ,
            
            
              comp
            
          
        
        =
        
          
            
              
                ρ
                
                  0
                
              
              
                c
                
                  2
                
              
            
            
              j
              ω
              
                V
                
                  0
                
              
            
          
        
      
    
    {\displaystyle Z_{{\text{ac}},\,{\text{comp}}}={\frac {\rho _{0}c^{2}}{j\omega V_{0}}}}

where 
 
 
 
 
 V
 
 0
 
 
 
 
 {\displaystyle V_{0}}
 
 is the air volume in the chamber.
The technique provides a measurement of the sensitivity of a microphone without the need for comparison with another previously calibrated microphone, and is instead traceable to reference electrical quantities such as <a href="/facts/Volts/KF18MXP2">volts</a> and <a href="/facts/Ohm/QNVrlGjw">ohms</a>, as well as <a href="/facts/Length/EwFyAqGH">length</a>, <a href="/facts/Mass/HHdc8XmF">mass</a> and <a href="/facts/Time/HceJKUGB">time</a>. Although a given calibrated microphone will often have been calibrated by other (secondary) methods, all can be traced (through a process of <a href="/facts/Dissemination/D3eh1QDb">dissemination</a>) back to a microphone calibrated using the reciprocity method at a National Measurement Institute. Reciprocity calibration is a specialist process, and because it forms the basis of the primary standard for sound pressure, many national measurement institutes have invested significant research efforts to refine the method and develop calibration facilities. A system is also commercially available from <a href="/facts/Br%C3%BCel_%26_Kj%C3%A6r/SNNcqsFI">Brüel & Kjær</a>.
For airborne acoustics, the reciprocity technique is currently the most precise method available for microphone calibration (i.e. has the smallest <a href="/facts/Uncertainty_of_measurement/Fhxgrufh">uncertainty of measurement</a>). <a href="/facts/Anechoic_chamber/J6XjAMKx"> Free field</a> reciprocity calibration (to give the free-field response, as opposed to the pressure response of the microphone) follows the same principles and roughly the same method as pressure reciprocity calibration, but in practice is much more difficult to implement. As such it is more usual to perform reciprocity calibration in an acoustical coupler, and then apply a correction if the microphone is to be used in free-field conditions; such corrections are standardised for laboratory standard microphones (IEC/TS 61094-7) and are generally available from the manufacturers of most of the common microphone types.

<h2 id="calibration-using-pistonphones-and-sound-calibrators">Calibration using pistonphones and sound calibrators</h2>
A pistonphone is an acoustical calibrator (sound source) that uses a closed coupling volume to generate a precise sound pressure for the calibration of measurement microphones. The principle relies on a <a href="/facts/Piston/z7pN46u7">piston</a> mechanically driven to move at a specified cyclic rate, pushing on a fixed volume of air to which the microphone under test is coupled. The air is assumed to be compressed <a href="/facts/Adiabiatic/nWI25Wvf"> adiabatically</a> and the <a href="/facts/Sound_pressure_level/MgJAcp2I">sound pressure level</a> in the chamber can, potentially, be calculated from internal physical dimensions of the device and the <a href="/facts/Adiabatic/rJj42U5h">adiabatic</a> gas law, which requires that PVγ is a constant, where P is the pressure in the chamber, V is the volume of the chamber, and γ is the ratio of the specific heat of air at constant pressure to its <a href="/facts/Specific_heat/9P0U6YgI">specific heat</a> at constant volume. Pistonphones are highly dependent on ambient pressure (always requiring a correction to ambient pressure conditions) and are generally only made to reproduce low frequencies (for practical reasons), typically 250 Hz. However, pistonphones can be very precise, with good stability over time. 
However, commercially available pistonphones are not calculable devices and must themselves be calibrated using a calibrated microphone if the results are to be traceable; though generally very stable over time, there will be small differences in the sound pressure level generated between different pistonphones. Since their output is also dependent on the volume of the chamber (coupling volume), differences in shape and load volume between different models of microphone will have an influence on the resulting SPL, requiring the pistonphone to be calibrated accordingly.
Sound calibrators are used in an identical way to pistonphones, providing a known sound pressure field in a cavity to which a test microphone is coupled. Sound calibrators are different from pistonphones in that they work electronically and use a low-impedance (electrodynamic) source to yield a high degree of volume independent operation. Furthermore, modern devices often use a feedback mechanism to monitor and adjust the <a href="/facts/Sound_pressure_level/MgJAcp2I">sound pressure level</a> in the cavity so that it is constant regardless of the cavity / microphone size. Sound calibrators normally generate a 1 kHz sine tone; 1 kHz is chosen since the <a href="/facts/A_weighting/nvBjQ5We"> A-weighted SPL</a> is equal to the linear level at 1 kHz. Sound calibrators should also be calibrated regularly at a nationally accredited calibration laboratory to ensure traceability. Sound calibrators tend to be less precise than pistonphones, but are (nominally) independent of internal cavity volume and ambient pressure.

<ul><li>IEC 61094-2, edition 2. (February 20, 2009) "Measurement Microphones, part 2". IEC Standard for Pressure Reciprocity Calibration of Measurement Microphones</li>
<li>IEC 61094-5, edition 1. (October 16, 2001) "Measurement Microphones, part 5". IEC Standard for Comparison Calibration of Measurement Microphones</li></ul>

Measurement microphone calibration open-in-new

Measurement microphone calibration