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Phased Array




In , 2006 . This technology was originally developed for Radio Astronomy , leading to Physics Nobel Prizes for Antony Hewish and Martin Ryle after several large phased arrays were developed at Cambridge University . The design is also used in Radar , and is generalized in Interferometric radio antennas.


USAGE

The relative Amplitude s of — and constructive and destructive Interference effects among — the signals radiated by the individual antennas determine the effective Radiation Pattern of the array. A phased array may be used to point a fixed radiation pattern, or to Scan rapidly in Azimuth or elevation. When phased arrays are used in Sonar it is called Beamforming .

The phased array is used for instance in Optical Communication as a wavelength selective splitter.

Phased arrays are required to be used by many AM Broadcast Stations to enhance signal coverage in the city of license, while minimizing interference to other areas. Due to the differences between daytime and nightime Ionospheric Propagation at AM broadcast frequencies, it is common for AM broadcast stations to change between day and night radiation patterns by switching the Phase and power levels supplied to the individual antenna elements daily at sunrise and sunset.


Naval usage

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Phased array radar systems are also used by Warships of several navies including the Japanese, Spanish and United States' navies in the Aegis combat system. Phased array radars allow a warship to use one Radar system for surface detection and tracking (finding ships), air detection and tracking (finding aircraft and missiles) and missile uplink capabilities. Prior to using these systems each Surface-to-air Missile in flight required a dedicated Fire-control Radar , which meant that ships could only engage a limited number of simultaneous targets. Phased array systems can be used to control missiles during the mid-course phase of the missile's flight. During the terminal portion of the flight, continuous-wave fire control directors provide the final guidance to the target. Because of the radar beam is electronically steered, phased array systems can direct radar beams fast enough to maintain a Fire Control Quality track on many targets simultaneously while also controlling several in-flight missiles. Modern U.S. guided missile Cruisers are capable of controlling more Missiles than could previous classes of warships.




Space usage

Recently, the MESSENGER spacecraft was launched. This is a mission to the planet Mercury (arrival 12 March 2011). This spacecraft is the first deep-space mission to use a phased-array antenna for communications. It communicates in the X-Band . The radiating elements are Circularly-polarized , slotted waveguides. The antenna can operate with 4 or 8 radiating elements.


Research usage

The , 2006 .


Optics

Within the visible or infrared spectrum of electromagnetic waves it is also possible to build phased arrays. They are used in wavelength multiplexers and filters for telecommunication purposesP. D. Trinh, S. Yegnanarayanan, F. Coppinger and B. Jalali Silicon-on-Insulator (SOI) Phased-Array Wavelength Multi/Demultiplexer with Extremely Low-Polarization Sensitivity IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 9, NO. 7, JULY 1997


MATHEMATICAL PERSPECTIVE AND FORMULAE

A phased array is an example of N-slit Diffraction . Since each individual antenna acts as a slit, emitting radio waves, their diffraction pattern can be calculated by adding the phase shift Φ to the fringing term.

We will begin from the N-slit diffraction pattern derived on the Diffraction page.

:
\psi ={\lambda } heta ight)}{ rac{\lambda }\sin heta} ight]\left[ rac{\sin
\left( rac{N}{2}{kd}\sin heta ight)}{\sin \left( rac{2}\sin heta ight)} ight]


Now, adding a Φ term to the \begin{matrix}kd\sin heta\,\end{matrix} fringe effect in the second term yields:

:\psi ={\lambda }\sin heta ight)}{ rac{\lambda }\sin heta} ight]\left[ rac{\sin
\left( rac{N}{2}\big( rac{\lambda }\sin heta + \phi \big) ight)}{\sin \left( rac{\lambda }\sin heta +\phi ight)} ight]


Taking the square of the wave function gives us the intensity of the wave.

:I = I_0{\lambda } \sin [ heta
]} ight]}^2}{\lambda
} \sin heta+\phi ight)} ight]}^2}


:
I =I_0{\lambda } \sin heta ight)}{ rac{\lambda }