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303   phase shifter, multielement                                              phase shifter, switched-line



           A multielement phase shifter is a discrete phase shifter pro-
           viding phase variation in a specified range with the specified
                     Ac
           discrete Df. tually, it is multidigit phase shifter, each digit
           of which can be in either of two states: the phase shift of the
           ith digit Df is present or absent. The number of digits n is
                     i
                               as
           defined via specified Df
                            n = 1 + log (p/Df)
                                     2
               Multielement phase  shifters are realized through diode
           phase shifters, field-effect transistor phase shifters, and other
           electrical phase  shifters. They  are widely used in phased
           arrays (number of digits is typically 5 or 6). IAM
           Ref.: Voskresenskiy (1981), p. 369.
           A  piezoceramic phase shifter is  an electromechanical  Figure P11 Typical Reggia-Spencer phase-shifter configura-
           waveguide phase shifter based on the reverse piezoelectric  tion (from Skolnik, 1970, Fig. 27, p. 12.27, reprinted by per-
           effect. It consists of a waveguide section, a phase shifting ele-  mission of McGraw-Hill).
           ment made as a springy metal plate close to the narrow wall  comparatively weak control field intensities, the disadvantage
           of the waveguide connected to the piezoceramic element, and  is worse switching time and switching power in comparison
           a short circuit element. The phase shifter operation is based  to latching ferrite phase shifters. IAM
           on the metal plate motion as the piezoceramic element bends  Ref.: Skolnik (1970), pp. 12.23–12.29.
           under the exposure of control voltage. This is a continuous
                                                                Semiconductor phase shifters use semiconductor devices as
                                              ,
           phase shifter, with a phase shift up to 315° active losses less
                                                                control components. Typically, they are divided  into  diode
           than 0.5 dB, and a switch time of 20 ms. The advantages of
                                                                phase shifters, field-effect transistor phase shifters, and field-
           this phase shifter is the linear dependence of the phase shift,
                                                                effect tetrode phase shifters. When the phase shift is large,
           the capability for initial phase setting mechanical adjustment,
                                                                diode phase shifters have considerable insertion loss, nonlin-
           and the capability of incorporating in the structure of phased
                                                                ear dependence of phase shift on control voltage, and a com-
           array. IAM
                                                                paratively large switch time. Transistor and  tetrode-based
           Ref.: Skalzhakin, A. I., Radiotekhnika, no. 6, 1991, p. 76 (in Russian).
                                                                phase shifters have an order better speed of phase shifting (a
           A  plasma phase  shifter is one  using plasma  in the  few  nanoseconds or  less) and  lower losses. Semiconductor
           waveguide so the electromagnetic waves going through this  phase shifters are the main type of phase shifters used in high-
           section get a phase shift depending on plasma density. This  speed phase control units in modern radars. IAM
           density can be controlled by static electrical and  magnetic  Ref.: Skolnik (1970) pp. 12.45–12.63; Sazonov (1988) p. 178.
           fields. IAM
                                                                A strip-(transmission-)line phase shifter is based on varia-
           Ref.: Popov (1980), p. 290.
                                                                tion of the electrical length of a strip transmission line. Typi-
           A reflex phase shifter operates on the principle of the phase  cally, these phase shifters use ferrite dielectric inserted into
           variation of a reflected signal when the length of a transmis-  the transmission line. Toroid cores  from ferrite  or garnet
           sion line is switched. To separate coming and reflected waves,  materials are used. To diminish the size of the phase shifter, a
           the microwave  bridges and circulators are used. The reflex  slow-wave structure (e.g., a meander line located in the center
           section of circulators of a diode phase shifter incorporates a  slot of a ferromagnetic toroid) can be used. Strip-transmis-
           varactor, the short circuit section of transmission line shorter  sion-line phase shifters operate in frequency bands of 0.18 to
           than l/4 providing bias to the diode and the compensation of  7 GHz, they have a bandwidth of 8 to 10%, and an insertion
           its spurious reactance parameters, and the elements for decou-  loss less than 2  dB. In  comparison  to waveguide phase
           pling of microwave and supply circuits. The main advantage  shifters,  they have lower  size  and weight,  but lower  power
           of the reflex phase shifter is that the voltage standing wave  handling capacity. IAM
           ratio is less than for the transmission phase shifter. IAM  Ref.: Skolnik (1970), p. 12.20; Sokolov (1984), p. 124.
           Ref.: Gassanov (1988), p. 146.                       A switched-line phase shifter is a discrete phase shifter of
           A Reggia-Spencer phase shifter is a reciprocal ferrite phase  the feed-through typed based on variation of microwave path
           shifter consisting of a bar of ferromagnetic material located  by diode or transistor  switches. (See  diode phase shifter,
           axially within a section of waveguide (Fig. P11). The longitu-  field-effect transistor phase shifter.) This  type of phase
           dinal magnetic field produced by a  solenoid wound  around  shifter is simple and the insertion loss has a weak dependence
           waveguide causes variation in the permeability of material  on phase shift that is beneficial for large values of phase shift.
           and  variation  in propagation constant of  the energy that  However, the upper frequency of these phase shifters is lim-
           results in a phase shift that can be controlled by a driving cur-  ited  by the resonant phenomena  due to the  capacitance  of
           rent. Operating frequencies are 8 to 70 GHz, the advantage is  switching diode or transistor. IAM
           simplicity and phase control implemented up to 360° with  Ref.: Voskresenskiy (1981), p. 363; Kaganov (1981), p. 79; Fink (1982),
                                                                   p. 25.64.
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