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EQUIVALENCE PRINCIPLE                                                         error, beam-steering  164



           given by Schelkunoff. It is widely used in antenna theory to  Angular (measurement) error is the error in measurement
           determine radiation from different types of aperture antennae:  of radar angular coordinates (e.g., azimuth and elevation in a
           horn antennas, reflector antennas, and so forth. SAL  land-based radar, yaw and pitch in an airborne radar or mis-
           Ref.: Johnson (1984), p. 2-8.                        sile seeker, or other angular coordinates depending on the
                                                                nature of the radar platform and application). The  many
           ERROR, measurement. An error is a discrepancy between
                                                                sources of angular error may be divided into tracking errors,
           the true value of a target parameter and its measured value
                                                                which cause the radar antenna axis to depart from the target
           (the estimate at  the output of a radar estimator). The main
                                                                angles; translation errors, which cause the axis angles to be
           measured  parameters  in radar applications are  signal time
                                                                reported incorrectly;  and propagation  errors. The several
           delay (target  range),  signal  angle of arrival (target angular
                                                                components of each type of error may further be divided into
           coordinates), signal doppler frequency (target radial velocity),
                                                                radar-dependent,  target-dependent, and platform-dependent
           and signal amplitude (target RCS). The fundamental source
                                                                classes, and into bias and noise error components, as shown
           of measurement error is the presence of random noise in the
                                                                for a tracking radar of the monopulse type, in Table E4. DKB
           receiver that introduces stochastic uncertainty in the process
                                                                Ref.: Barton (1988), pp. 533–548.
           of radar measurement. In the general case the measurement
           error can be  represented as  a random function of time (see              Table E4
           error model) and of target coordinates, the latter representa-     Angular Error Components
           tion being much more complicated and applying to measure-
           ment in phased-array radars. Based on the representation of  Error class  Bias components  Noise components
           the target-radar measurement channel, the errors may be clas-  Radar-  Boresight axis set-  Thermal noise; multi-
           sified as target-dependent, propagation, radar-dependent, and,  dependent   ting and drift;   path; clutter; jamming;
           if the  radar is located on a  moving platform  (ship,  aircraft,  tracking   torque caused by   torque caused by wind
           spacecraft, etc.), platform-dependent errors. From the view-  errors  wind and gravity;   gusts; servo noise;
           point of the measured parameter, angle, doppler, range, and       servo unbalance   deflection of antenna
           RCS errors are distinguished. From the viewpoint of time          and drift        caused by acceleration
           variation (correlation function), they are classified as system-  Radar-  Pedestal leveling;   Bearing wobble; data
           atic (bias) and varying (slow or  rapid) errors. The  rapidly  dependent   azimuth align-  gear nonlinearity and
           varying errors caused  by receiver  noise are called noise  translation   ment; orthogonal-  backlash; data takeoff
           errors, and as they are uncorrelated from pulse to pulse they  errors  ity of axes;   nonlinearity and granu-
                                                                             pedestal flexure   larity; pedestal deflec-
           can be reduced by data smoothing. As a result, the final accu-
                                                                             caused by gravity   tion caused by
           racy of the data is usually dominated by bias and slowly vary-
                                                                             and solar heating  acceleration; phase
           ing errors. Bias error can be reduced by proper radar pointing
                                                                                              shifter error
           or calibration. SAL
                                                                 Target-     Dynamic lag      Glint; dynamic lag varia-
           Ref.: Barton (1964), (1969), (1988); Leonov (1990).
                                                                 dependent                    tion; scintillation or bea-
           Acceleration error refers to the dynamic lag error in a track-  tracking           con modulation
           ing radar or track-while-scan loop, caused by target accelera-  errors
           tion. This component of error can be found as the ratio of  Propagation   Average refraction   Irregularities in refraction
           target acceleration a  to the acceleration error constant K  of  errors  of troposphere and   of troposphere and iono-
                                                         a
                            t
           the loop:                                                         ionosphere       sphere
                                     a t
                                e =  ------                     An anomalous error is an error in evaluation of parameter
                                 a  K
                                      a                         that exceeds  some specified value.  It  can arise because  the
           When the acceleration is expressed in a linear coordinate, as  conditions under which measurements are made deviate sig-
              2
           m/s , the error will be in meters in that coordinate, while if  nificantly from the standard case (e.g., because of sig-
                                     2
           angular acceleration is used, r/s , the error will be in radians  nal-to-noise ratio decreases caused  by jamming, clutter,  or
           in that coordinate.                                  other adverse factors). AIL
               The acceleration error constant can be expressed in terms
                                                                Ref.: Kulikov (1978), p. 29.
           of the closed-loop (noise) bandwidth, b , in hertz:
                                           n
                                                                Beam-steering error is the error  between the  commanded
                                        2
                                K =  2.5b                       (and indicated) position of  a  phased-array beam and the
                                 a      n
                                                                actual position. For  a linear array or rectangular array with
           For a track-while-scan loop of the a-b filter type, K  may be  common row or column phase-shift settings, the error due to
                                                     a
           found as (Blackman, 1986)
                                                                granularity of an m-bit phase shifter is
                                      b
                              K =  -----------------------                             q
                               a         2                                              3 G q()
                                                                                            d
                                  ( 1 –  a ) T                                    e =  ------ ---------------
                                                                                   q    m
                                                                                       2   G 0
           where T is the data sample interval. DKB
           Ref.: Barton (1988), pp. 463–466; Blackman (1986), p. 46.
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