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Phased Array Antenna

Figure 1: left:two antenna elements, fed with the same phase, right: two antenna elements, fed with different phase shift

The figure shows the interference of two one above the other lying in-phasely radiant antenna elements. The main beam direction is centric. The figure shows the interference of two one above the other lying antenna elements radiating with a different phase shift. The lower antenna element radiates with a phase shift of 15 degrees earlier as the upper antenna element. The main beam direction is steared up.

Figure 1: left:two antenna elements, fed with the same phase, right: two antenna elements, fed with different phase shift

Phased Array Antenna

A phased array antenna is composed of lots of radiating elements each with a phase shifter. Beams are formed by shifting the phase of the signal emitted from each radiating element, to provide constructive/destructive interference so as to steer the beams in the desired direction.
In the figure 1 (left) both radiating elements are fed with the same phase. The signal is amplified by constructive interference in the main direction. The beam sharpness is improved by the destructive interference.

Figure 2: electronic beam-deflection,
left:Boresight, right: Deflected

(click to enlarge: 591·723px = 468 kByte)

Figure 2: Animation of the electronic beam-deflection

In the figure 1 (right), the signal is emitted by the upper radiating element with a phase shift of 22 degrees later than of the lower radiating element. Because of this the main direction of the emitted sum-signal is moved slightly upwards.

(Note: Radiating elements have been used without reflector in the figure. Therefore the back lobe of the shown antenna diagrams is just as large as the main lobe.)

The main beam always points in the direction of the increasing phase shift. Well, if the signal to be radiated is delivered through an electronic phase shifter giving a continuous phase shift then the beam direction will be electronically adjustable. However, this cannot be extended unlimitedly. The highest value, which can be achieved for the Field of View (FOV) of a olanar phased array antenna is 120° (60° left and 60° right). With the sine theorem the necessary phase moving can be calculated.

The following figure graphically shows the matrix of radiating elements. Arbitrary antenna constructions can be used as a spotlight in an antenna field. For a phased array antenna is decisive that the single radiating elements are steered for with a regular phase moving and the main direction of the beam therefore is changed. E.g. the antenna of the RRP 117 consists of 1584 radiating elements arranged in an analog beamforming architecture. More sophsticated radar sets use the benefits of a Digital Beamforming architecture.

  • high gain width los side lobes
  • Ability to permit the beam to jump from one target to the next in a few microseconds
  • Ability to provide an agile beam under computer control
  • arbitrarily modes of surveillance and tracking
  • free eligible Dwell Time
  • multifunction operation by emitting several beams simultaneously
  • Fault of single components reduces the capability and beam sharpness, but the system remains operational
  • the coverage is limited to a 120 degree sector in azimuth and elevation
  • deformation of the beam while the deflection
  • low frequency agility
  • very complex structure (processor, phase shifters)
  • still high costs

Possible Arrangements

Linear Arrays

Figure 3: linear array of a phased-array antenna

Figure 3: linear array of a phased-array antenna

These antennae consist of lines whose elements are fed about a common phase shifter. A number of vertically about each other mounted linear arrays form a flat antenna.

This kind of the phased-array antenna is commonly used, if the beam-deflection is required in a single plane only because a turn of the complete antenna is anyway carried out ( RRP-117).

Figure 4: planar array of a phased-array antenna

Figure 4: planar array of a phased-array antenna

Planar Arrays

These antenna arrays completely consist of singles radiating elements and each of it gets an own phase shifter. The elements are ordered in a matrix array. The planar arrangement of all elements forms the complete phased-array antenna.

Figure 5: frequency scanning array

Figure 5: frequency scanning array

Frequency Scanning Array

Frequency scanning is a special case of the phased array antenna where the main beam steering occurs by the frequency scanning of the exciter. The beam stearing is a function of the transmitted frequency. This type of antenna is called a frequency scanning array. The normal arrangement is to feed the different radiating elements from one folded waveguide. The frequency scanning array is a special case of serial feeding type of a phased array antenna and is based on a particular property of wave propagation in waveguides. The phase difference between two radiating elements is n·360° at the normal frequency.

By changing the frequency, the angle Θs between the axis of the main beam and the normal on the array antenna changes. Height information is generated using the following philosophy:

As frequency is varied, the beam axis will change, and scanning can be accomplished in elevation. The radar set is designed so that it keeps track of the frequencies as they are transmitted and then detects and converts the returned frequencies into 3D display data.

Note that frequency scanning reduces the value of using frequency change as a means of achieving other valuable effects (benefits of pulse compression).

recommendation Feed systems

Phase-increment Calculating

The phase shift Δφ between two successive elements is constant and is called phase-increment. How large is this phase shift to reach a certain value of the beam steering?

A linear arrangement by isotropic radiating elements is looked at.

Die Grafik zeigt mehrere Strahler, die mit einer jeweiligen Phasendifferenz abstrahlen und einer grafischen Herleitung der Phasenverschiebung.

Figure 6: grafic derivation of the formula

x = d · sin Θs (1)

360° = λ Δφ = phase shift between two successive elements
d = distance between the radiating elements
Θs = beam steering
Δφ x

Δφ = 360° · d · sin Θs (3)

Example given:

  • A radar set works with a wavelength of λ=10 cm.
  • The distance between the radiating elements is 15 cm.
  • We can neglect the propagation time differences by the feeder.
  • The beam steering shall be Θs= 40°.
  • Which value shall have to have the phase shifter no. 8 (on the left side) to get this beam steering?

We start with the calculation of the phase-increment.
Because of the trigonometrical function we need a calculator anyway: Δφ =(360°·15 cm/10 cm)·sin(40°) = 347.1°.

This means the radiating element no. 8 needs the phase shift value φ = 7 · 347.1 = 2429.7°.
On reason of the periodicity of the sine function a phase shifting of n·360° is the same as 0°. Therefore we can as long as deduct 360° till there is a angle between 0° and 360° of the result. We get therefore for the phase shifter number 8 (left corner) a phase shift value of φ= 269.7°.

A part of this phase shift is realized by the delay in the feeding line yet.