PHASED ARRAY ANTENNAS                    Errata and Additions

updated June 2004
page 1   ¶ 1   line 1   antennas is a task
page 1   ¶ 3   line 6    preclude the ground
page 8   ¶ 3   line 2    becomes a simple result, leaving a real pattern times an                                  exponential
page 9     Fig. 2.2   column 3    heading:    3 wavelengths/4
page 15   Fig. 2.11    SLR = 13 dB
page 28   Fig. 2.22    replace
page 31   Eq'n 2.39    remove integral sign and dp
page 31   remove:    where the integration is over each step
page 38   Eq'n 2.53    remove factor of 2 in numerator
page 50   ¶ 3   line 1    Taylor (1955
page 59   ¶1    line 3   starting point (this reference is summarized here)
page 68   ¶ 1   line 3    integrate the pattern function; this expression is accurate
                                   for apertures large in wavelengths  (Friis and Lewis, 1947)
page 73   Eq'n 3.54-3.56    remove F02
page 73   ¶ 4   line 1    fixed, and the 10 log factor below can be
page 78   ¶ 2   line 3    peak location u0; again accurate for large apertures
page 83   ¶ 2   line 10    Lopez, 1968
page 84   ¶ 1   line 13    (Rao et al, 1996). Rungs are not terminated with
                                                                 loads,thereby increasing efficiency.
page 104   Kinsey    Patent 3509577
page 104   Lopez    July, 1968
page 115   ¶ 2   line 1    Aperture efficiency, accurate for large apertures and                                      constant phase, is obtained from
page 154   ¶ 2   line 4    VSWR 2   the fractional bandwidth is
page 155   Fig. 5.33      epsilon r = 10
page 169   ¶ 1   line 12    Tai and Long, 1961
page 203   ¶ 3   line 4    The spur-free dynamic range is along the noise floor                                       between the f0 and 2f2 - f1 lines; see Fig. 6.46
page 203   Fig. 6.46    replace
page 212    Hadge reference should follow Gustafson
page 226   ¶ 6   line 4    Richmond and Geary (1970)
page 235   ¶ 2   line 12    Diamond (1968). See also Stark (1966).
page 237   Eq'n 7.41    remove wavelength sq in denominator

page 244   ¶ 1   line 7   30 x 30
page 237   Eq'n 7.42    remove wavelength sq in denominator; sin(2k(subzo)h)
page 257   ¶ 1   line 1    Scan Impedance changes
page 270    Richmond, J. H.. and Geary, N. H.
page 271    add:   Stark, L, "Radiation Impedance of a Dipole in an Infinite
                            Planar Phased Array," Radio Science,
                            Vol. 1, March 1966, pp. 361-377
page 280   ¶ 4   line 3   Shubert and Munk
page 358   ¶ 2   line 4    in wavelengths
page 446    Antonucci    Proc. 1985
page 452    Villeneuve, A. T.,  Behnke, M. C.
page 466   ¶ 1   line5     related to the no error mean sidelobe . . .
page 475    add:   Geary, N. H. 226, 270
page 476    Haneishi, M.,  Hilburn, J. L.
page 477    Knudsen
page 480    add:    Stark, L. 235, 271
page 482    add:    Bandwidth, 15, 26, 154, 164
page 483    add:    Delay, 26   Folded matrix, 231
page 483    add:    Directivity: Isotropic array, 36
page 484    add:    Isotropic array, 36   Lagrangian, 305  Lens, 338, 341, 356                              Linear array: bandwidth 15, 26, 164, 309  Matrix, 231
page 486    add:    Time delay, 26   VSWR, 155


                   Inside back cover: normalized to unity; dipole along x-axis

 

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