Radar engineering details

Radar engineering details are technical details pertaining to the components of a radar and their ability to detect the return energy from moving scatterers — determining an object's position or obstruction in the environment.[1][2][3] This includes field of view in terms of solid angle and maximum unambiguous range and velocity, as well as angular, range and velocity resolution. Radar sensors are classified by application, architecture, radar mode, platform, and propagation window.

Applications of radar include Autonomous cruise control system, autonomous landing guidance, radar altimeter, air traffic management, early-warning radar, fire-control radar, forward warning collision sensing, ground penetrating radar, surveillance, and weather forecasting.

Architecture choice

The angle of a target is detected by scanning the field of view with a highly directive beam. This is done electronically, with a phased array antenna, or mechanically by rotating a physical antenna. The emitter and the receiver can be in the same place, as with the monostatic radars, or be separated as in the bistatic radars. Finally, the radar wave emitted can be continuous or pulsed. The choice of the architecture depends on the sensors to be used.

Scanning antenna

Fig. 1: A passive electronically scanned array with a monopulse feed network.

An electronically scanned array (ESA), or a phased array, offers advantages over mechanically scanned antennas such as instantaneous beam scanning, the availability of multiple concurrent agile beams, and concurrently operating radar modes. Figures of merit of an ESA are the bandwidth, the effective isotropically radiated power (EIRP) and the GR/T quotient, the field of view. EIRP is the product of the transmit gain, GT, and the transmit power, PT. GR/T is the quotient of the receive gain and the antenna noise temperature. A high EIRP and GR/T are a prerequisite for long-range detection. Design choices are:

k \, d \, \cos{\theta} = \beta \left ( f \right ) = 2 \, \pi \, \frac{c}{\lambda_0} \, \Delta \tau
\theta = \arccos { \left ( \frac{c}{d} \, \Delta \tau \right )}

Note that \theta is not a function of frequency. A constant phase shift over frequency has important applications as well, albeit in wideband pattern synthesis. For example, the generation of wideband monopulse \Sigma/\Delta receive patterns depends on a feed network which combines two subarrays using a wideband hybrid coupler.

FMCW versus pulse-Doppler

The range and velocity of a target are detected through pulse delay ranging and the Doppler effect (pulse-Doppler), or through the frequency modulation (FM) ranging and range differentiation. The range resolution is limited by the instantaneous signal bandwidth of the radar sensor in both pulse-Doppler and FMCW radars. Monostatic monopulse-Doppler radar sensors offer advantages over FMCW radars, such as:

Bistatic versus monostatic

Bistatic radars have a spatially dislocated transmitter and receiver. In this case sensor in the transmitting antenna report back to the system the angular position of the scanning beam while the energy detecting ones are with the other antenna. A time synchronisation is crucial in interpreting the data as the receiver antenna is not moving.

Monostatic radars have a spatially co-located transmitter and receiver. It this case, the emission has to be insulated from the reception sensors as the energy emitted is far greater than the returned one.

Platform

Radar clutter is platform-dependent. Examples of platforms are airborne, car-borne, ship-borne, space-borne, and ground-based platforms.

Propagation window

The radar frequency is selected based on size and technology readiness level considerations. The radar frequency is also chosen in order to optimize the radar cross-section (RCS) of the envisioned target, which is frequency-dependent. Examples of progation windows are the 3 GHz (S), 10 GHz (X), 24 GHz (K), 35 GHz (Ka), 77 GHz (W), 94 GHz (W) propagation windows.

Radar Mode

Radar modes for point targets include search and track. Radar modes for distributed targets include ground mapping and imaging. The radar mode sets the radar waveform

See also

  1. Amplitude monopulse for amplitude-comparison monopulse
  2. Phase interferometry for phase-comparison monopulse

References

  1. G. W. Stimson: "Introduction to Airborne Radar, 2nd Ed.," SciTech Publishing, 1998
  2. P. Lacomme, J.-P. Hardange, J.-C. Marchais, E. Normant: "Air and Spaceborne Radar Systems: An Introduction," IEE, 2001
  3. M. I. Skolnik: "Introduction to Radar Systems, 3rd Ed.," McGraw-Hill, 2005
  4. R. J. Mailloux: "Phased Array Antenna Handbook," Artech House, 2005
  5. E. Brookner: "Practical Phased Array Antenna Systems," Artech House, 1991
  6. R. C. Hansen: "Phased Array Antennas," John Wiley & Sons, 1998
  7. A. Ludloff: "Praxiswissen Radar und Radarsignalverarbeitung, 2. Auflage," Viewegs Fachbücher der Technik, 1998
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