Radar

Radar
Radar is an object-detection system which uses radio waves to determine the range, altitude, direction, or speed of objects. It can be used to detect aircraft, ships, spacecraft, guided missiles, motor vehicles, weather formations, and terrain. The radar dish or antenna transmits pulses of radio waves or microwaves which bounce off any object in their path. The object returns a tiny part of the wave's energy to a dish or antenna which is usually located at the same site as the transmitter. Radar was developed in secret in nations across the world just before and during World War II. The term RADAR was coined in 1941 by the United States Navy as an acronym for radio detection and ranging.[1][2] The term radar has since entered English and other languages as the common noun radar, losing all capitalization. The modern uses of radar are highly diverse, including air traffic control, radar astronomy, air-defense systems, antimissile systems; marine radars to locate landmarks and other ships; aircraft anticollision systems; ocean surveillance systems, outer space surveillance and rendezvous systems; meteorological precipitation monitoring; altimetry and flight control systems; guided missile target locating systems; and ground-penetrating radar for geological observations. High tech radar systems are associated with digital signal processing and are capable of extracting objects from very high noise levels. Other systems similar to radar have been used in other parts of the electromagnetic spectrum. One example is "lidar", which uses visible light from lasers rather than radio waves.
A long-range radar antenna, known as ALTAIR, used to detect and track space objects in conjunction with ABM testing at the Ronald Reagan Test Site on Kwajalein Atoll.

History
As early as 1886, Heinrich Hertz showed that radio waves could be Israeli military radar is typical of the type of radar reflected from solid objects. In 1895 Alexander Popov, a physics used for air traffic control. The antenna rotates at instructor at the Imperial Russian Navy school in Kronstadt, developed a steady rate, sweeping the local airspace with a an apparatus using a coherer tube for detecting distant lightning strikes. narrow vertical fan-shaped beam, to detect aircraft at all altitudes. The next year, he added a spark-gap transmitter. In 1897, while testing this in communicating between two ships in the Baltic Sea, he took note of an interference beat caused by the passage of a third vessel. In his report, Popov wrote that this phenomenon might be used for detecting objects, but he did nothing more with this observation.[3] The German Christian Huelsmeyer was the first to use radio waves to detect "the presence of distant metallic objects". In 1904 he demonstrated the feasibility of detecting a ship in dense fog but not its distance.[4] He obtained a patent[5] for his detection device in April 1904 and later a patent[6] for a related amendment for determining the distance to the ship. He also got a British patent on September 23, 1904[7] for the first full radar application, which he called telemobiloscope.

Radar In August 1917 Nikola Tesla outlined a concept for primitive radar units.[8] He stated, "...by their [standing electromagnetic waves] use we may produce at will, from a sending station, an electrical effect in any particular region of the globe; [with which] we may determine the relative position or course of a moving object, such as a vessel at sea, the distance traversed by the same, or its speed." In 1922 A. Hoyt Taylor and Leo C. Young, researchers working with the U.S. Navy, discovered that when radio waves were broadcast at 60 MHz it was possible to determine the range and bearing of nearby ships in the Potomac River. Despite Taylor's suggestion that this method could be used in darkness and low visibility, the Navy did not immediately continue the work.[9] Serious investigation began eight years later after the discovery that radar could be used to track airplanes.[10] Before the Second World War, researchers in France, Germany, Italy, Japan, the A Chain Home tower in Great Netherlands, the Soviet Union, the United Kingdom, and the United States, Baddow, United Kingdom independently and in great secrecy, developed technologies that led to the modern version of radar. Australia, Canada, New Zealand, and South Africa followed prewar Great Britain, and Hungary had similar developments during the war.[11] In 1934 the Frenchman mile Girardeau stated he was building an obstacle-locating radio apparatus "conceived according to the principles stated by Tesla" and obtained a patent for a working system,[12][13][14] a part of which was installed on the Normandie liner in 1935.[15] During the same year, the Soviet military engineer P.K.Oschepkov, in collaboration with Leningrad Electrophysical Institute, produced an experimental apparatus, RAPID, capable of detecting an aircraft within 3km of a receiver.[16] The French and Soviet systems, however, had continuous-wave operation and could not give the full performance that was ultimately at the center of modern radar. Full radar evolved as a pulsed system, and the first such elementary apparatus was demonstrated in December 1934 by American Robert M. Page, working at the Naval Research Laboratory.[17] The following year, the United States Army successfully tested a primitive surface to surface radar to aim coastal battery search lights at night.[18] This was followed by a pulsed system demonstrated in May 1935 by Rudolf Khnhold and the firm GEMA in Germany and then one in June 1935 by an Air Ministry team led by Robert A. Watson Watt in Great Britain. Later, in 1943, Page greatly improved radar with the monopulse technique that was used for many years in most radar applications.[19] The British were the first to fully exploit radar as a defence against aircraft attack. This was spurred on by fears that the Germans were developing death rays.[20] The Air Ministry asked British scientists in 1934 to investigate the possibility of propagating electromagnetic energy and the likely effect. Following a study, they concluded that a death ray was impractical but that detection of aircraft appeared feasible.[20] Robert Watson Watt's team demonstrated to his superiors the capabilities of a working prototype and then patented the device.[14][21][22] It served as the basis for the Chain Home network of radars to defend Great Britain. In April 1940, Popular Science showed an example of a radar unit using the Watson-Watt patent in an article on air defence, but not knowing that the U.S. Army and U.S. Navy were working on radars with the same principle, stated under the illustration, "This is not U.S. Army equipment."[23] Also, in late 1941 Popular Mechanics had an article in which a U.S. scientist conjectured what he believed the British early warning system on the English east coast most likely looked like and was very close to what it actually was and how it worked in principle.[24]

Radar The war precipitated research to find better resolution, more portability, and more features for radar, including complementary navigation systems like Oboe used by the RAF's Pathfinder.

Applications
The information provided by radar includes the bearing and range (and therefore position) of the object from the radar scanner. It is thus used in many different fields where the need for such positioning is crucial. The first use of radar was for military purposes: to locate air, ground and sea targets. This evolved in the civilian field into applications for aircraft, ships, and roads. In aviation, aircraft are equipped with radar devices that warn of obstacles in or approaching their path and give accurate altitude readings. The first commercial device fitted to aircraft was a 1938 Bell Lab unit on some United Air Lines aircraft.[24] They can land in fog at airports equipped with radar-assisted ground-controlled approach systems, in which the plane's flight is observed on radar screens while operators radio landing directions to the pilot.

Commercial marine radar antenna. The rotating antenna radiates a vertical fan-shaped beam.

Marine radars are used to measure the bearing and distance of ships to prevent collision with other ships, to navigate and to fix their position at sea when within range of shore or other fixed references such as islands, buoys, and lightships. In port or in harbour, vessel traffic service radar systems are used to monitor and regulate ship movements in busy waters. Police forces use radar guns to monitor vehicle speeds on the roads. Meteorologists use radar to monitor precipitation. It has become the primary tool for short-term weather forecasting and to watch for severe weather such as thunderstorms, tornadoes, winter storms, precipitation types, etc. Geologists use specialised ground-penetrating radars to map the composition of the Earth's crust.

Principles
A radar system has a transmitter that emits radio waves called radar signals in predetermined directions. When these come into contact with an object they are usually reflected or scattered in many directions. Radar signals are reflected especially well by materials of considerable electrical conductivityespecially by most metals, by seawater, by wet land, and by wetlands. Some of these make the use of radar altimeters possible. The radar signals that are reflected back towards the transmitter are the desirable ones that make radar work. If the object is moving either closer or farther away, there is a slight change in the frequency of the radio waves, caused by the Doppler effect. Radar receivers are usually, but not always, in the same location as the transmitter. Although the reflected radar signals captured by the receiving antenna are usually very weak, these signals can be strengthened by electronic amplifiers. More sophisticated methods of signal processing are also used in order to recover useful radar signals. The weak absorption of radio waves by the medium through which it passes is what enables radar sets to detect objects at relatively long rangesranges at which other electromagnetic wavelengths, such as visible light, infrared light, and ultraviolet light, are too strongly attenuated. Such things as fog, clouds, rain, falling snow, and sleet that block visible light are usually transparent to radio waves. Certain radio frequencies that are absorbed or scattered by water vapor, raindrops, or atmospheric gases (especially oxygen) are avoided in designing radars except when detection of these is intended. Radar relies on its own transmissions rather than light from the Sun or the Moon, or from electromagnetic waves emitted by the objects themselves, such as infrared wavelengths (heat). This process of directing artificial radio

Radar waves towards objects is called illumination, regardless of the fact that radio waves are invisible to the human eye or cameras.

Reflection
Electromagnetic waves reflect (scatter) from any large change in the dielectric constant or diamagnetic constants. This means that a solid object in air or a vacuum, or other significant change in atomic density between the object and what is surrounding it, will usually scatter radar (radio) waves. This is particularly true for electrically conductive materials, such as metal and carbon fiber, making radar well suited to the detection of aircraft and ships. Radar absorbing material, containing resistive and sometimes magnetic substances, is used on military vehicles to reduce radar reflection. This is the radio equivalent of painting something a dark color so that it cannot be seen through normal means. Radar waves scatter in a variety of ways depending on the size Brightness can indicate reflectivity as in this 1960 (wavelength) of the radio wave and the shape of the target. If the weather radar image (of Hurricane Abby). The wavelength is much shorter than the target's size, the wave will bounce radar's frequency, pulse form, polarization, signal off in a way similar to the way light is reflected by a mirror. If the processing, and antenna determine what it can observe. wavelength is much longer than the size of the target, the target may not be visible because of poor reflection. Low Frequency radar technology is dependent on resonances for detection, but not identification, of targets. This is described by Rayleigh scattering, an effect that creates the Earth's blue sky and red sunsets. When the two length scales are comparable, there may be resonances. Early radars used very long wavelengths that were larger than the targets and received a vague signal, whereas some modern systems use shorter wavelengths (a few centimeters or shorter) that can image objects as small as a loaf of bread. Short radio waves reflect from curves and corners, in a way similar to glint from a rounded piece of glass. The most reflective targets for short wavelengths have 90 angles between the reflective surfaces. A structure consisting of three flat surfaces meeting at a single corner, like the corner on a box, will reflect waves entering its opening directly back at the source. These so-called corner reflectors are commonly used as radar reflectors to make otherwise difficult-to-detect objects easier to detect and are often found on boats in order to improve their detection in a rescue situation and to reduce collisions. For similar reasons, objects attempting to avoid detection will angle their surfaces in a way to eliminate inside corners and avoid surfaces and edges perpendicular to likely detection directions, which leads to "odd" looking stealth aircraft. These precautions do not completely eliminate reflection because of diffraction, especially at longer wavelengths. Half wavelength long wires or strips of conducting material, such as chaff, are very reflective but do not direct the scattered energy back toward the source. The extent to which an object reflects or scatters radio waves is called its radar cross section.

Radar

Radar equation
The power Pr returning to the receiving antenna is given by the equation:

where Pt = transmitter power Gt = gain of the transmitting antenna Ar = effective aperture (area) of the receiving antenna = radar cross section, or scattering coefficient, of the target F = pattern propagation factor Rt = distance from the transmitter to the target Rr = distance from the target to the receiver.

In the common case where the transmitter and the receiver are at the same location, Rt = Rr and the term Rt Rr can be replaced by R4, where R is the range. This yields:

This shows that the received power declines as the fourth power of the range, which means that the reflected power from distant targets is very small. The equation above with F = 1 is a simplification for vacuum without interference. The propagation factor accounts for the effects of multipath and shadowing and depends on the details of the environment. In a real-world situation, pathloss effects should also be considered.

Doppler effect
Ground-based radar systems used for detecting speeds rely on the Doppler effect. The apparent frequency (f) of the wave changes with the relative position of the target. The doppler equation is stated as follows for (the radial speed of the observer) and (the radial speed of the target) and frequency of wave :

However, the change in phase of the return signal is often used instead of the change in frequency. Only the radial component of the speed is available. Hence when a target is moving at right angle to the radar beam, it has no relative velocity, while one parallel to it has maximum recorded speed even if both might have the same real absolute motion.

Polarization
In the transmitted radar signal, the electric field is perpendicular to the direction of propagation, and this direction of the electric field is the polarization of the wave. Radars use horizontal, vertical, linear and circular polarization to detect different types of reflections. For example, circular polarization is used to minimize the interference caused by rain. Linear polarization returns usually indicate metal surfaces. Random polarization returns usually indicate a fractal surface, such as rocks or soil, and are used by navigation radars.

Radar

Limiting factors
Beam path and range The radar beam would follow a linear path in vacuum, but it really follows a somewhat curved path in the atmosphere because of the variation of the refractive index of air, that is the radar horizon. Even when the beam is emitted parallel to the ground, it will rise above it as the Earth curvature sinks below the horizon. Furthermore, the signal is attenuated by the medium it crosses, and the beam disperses. The maximum range of a conventional radar can be limited by a number of factors: Line of sight, which depends on height above ground. Echo heights above ground The maximum non-ambiguous range which is determined by the pulse repetition frequency. The maximum non-ambiguous range is the distance the pulse could travel and return before the next pulse is emitted. Radar sensitivity and power of the return signal as computed in the radar equation. This includes factors such as environmentals and the size (or radar cross section) of the target. Noise Signal noise is an internal source of random variations in the signal, which is generated by all electronic components. Noise typically appears as random variations superimposed on the desired echo signal received in the radar receiver. The lower the power of the desired signal, the more difficult it is to discern it from the noise. Noise figure is a measure of the noise produced by a receiver compared to an ideal receiver, and this needs to be minimized. Noise is also generated by external sources, most importantly the natural thermal radiation of the background scene surrounding the target of interest. In modern radar systems, the internal noise is typically about equal to or lower than the external scene noise. An exception is if the radar is aimed upwards at clear sky, where the scene is so "cold" that it generates very little thermal noise. The thermal noise is given by kB T B, where T is temperature, B is bandwidth (post matched filter) and kB is Boltzman's constant. There is an appealing intuitive interpretation of this relationship in a radar. Matched filtering allows us to compress the entire energy received from a target into a single bin (be it a range, Doppler,elevation, or azimuth bin). On the surface it would appear then that within a fixed interval of time one could obtain perfect, error free, detection. To do this one simply compresses all energy into an infinitesimal time slice. What limits this approach in the real world is that, while time is arbitrarily divisible, current is not. The quanta of electrical energy is an electron, and so the best one can do is match filter all energy into a single electron. Since the electron is moving at a certain temperature (Plank spectrum) this noise source cannot be further eroded. We see then that radar,like indeed all macro-scale entities, is profoundly inmpacted by quantum theory. There will be also flicker noise caused by electrons transit, but depending on 1/f, flicker noise will be much lower than thermal noise when the frequency is high. Hence, in pulse radar, the system will be heterodyne. Another reason for heterodyne processing is that for fixed fractional bandwidth, the instantaneous bandwidth increases linearly in frequency. This allows improved range resolution. The one notable exception to heterodyne (downconversion) radar systems is ultra-wideband radar. Here a single cycle, or transient wave, is used similar to UWB communications, see List of UWB channels.

Radar Interference Radar systems must overcome unwanted signals in order to focus only on the actual targets of interest. These unwanted signals may originate from internal and external sources, both passive and active. The ability of the radar system to overcome these unwanted signals defines its signal-to-noise ratio (SNR). SNR is defined as the ratio of a signal power to the noise power within the desired signal. In less technical terms, SNR compares the level of a desired signal (such as targets) to the level of background noise. The higher a system's SNR, the better it is in isolating actual targets from the surrounding noise signals. Clutter Clutter refers to radio frequency (RF) echoes returned from targets which are uninteresting to the radar operators. Such targets include natural objects such as ground, sea, precipitation (such as rain, snow or hail), sand storms, animals (especially birds), atmospheric turbulence, and other atmospheric effects, such as ionosphere reflections, meteor trails, and three body scatter spike. Clutter may also be returned from man-made objects such as buildings and, intentionally, by radar countermeasures such as chaff. Some clutter may also be caused by a long radar waveguide between the radar transceiver and the antenna. In a typical plan position indicator (PPI) radar with a rotating antenna, this will usually be seen as a "sun" or "sunburst" in the centre of the display as the receiver responds to echoes from dust particles and misguided RF in the waveguide. Adjusting the timing between when the transmitter sends a pulse and when the receiver stage is enabled will generally reduce the sunburst without affecting the accuracy of the range, since most sunburst is caused by a diffused transmit pulse reflected before it leaves the antenna. Clutter is considered a passive interference source, since it only appears in response to radar signals sent by the radar. There are several methods of detecting and neutralizing clutter. Many of these methods rely on the fact that clutter tends to appear static between radar scans. Therefore, when comparing subsequent scan echoes, desirable targets will appear to move, and all stationary echoes can be eliminated. Sea clutter can be reduced by using horizontal polarization, while rain is reduced with circular polarization (note that meteorological radars wish for the opposite effect, therefore using linear polarization to detect precipitation). Other methods attempt to increase the signal-to-clutter ratio. The most effective clutter reduction technique is pulse-Doppler radar. Doppler separates clutter from aircraft and spacecraft using a frequency spectrum, so individual signals can be separated from multiple reflectors located in the same volume using velocity differences. This requires a coherent transmitter. Another technique is moving target indicator that subtracts the receive signal from two successive pulses using phase to reduce signals from slow moving objects. This can be adapted for systems that lack a coherent transmitter, such as time-domain pulse-amplitude radar. Constant False Alarm Rate, a form of Automatic Gain Control (AGC), is a method relying on the fact that clutter returns far outnumber echoes from targets of interest. The receiver's gain is automatically adjusted to maintain a constant level of overall visible clutter. While this does not help detect targets masked by stronger surrounding clutter, it does help to distinguish strong target sources. In the past, radar AGC was electronically controlled and affected the gain of the entire radar receiver. As radars evolved, AGC became computer-software controlled and affected the gain with greater granularity in specific detection cells.

Radar

Clutter may also originate from multipath echoes from valid targets caused by ground reflection, atmospheric ducting or ionospheric reflection/refraction (e.g. Anomalous propagation). This clutter type is especially bothersome since it appears to move and behave like other normal (point) targets of interest. In a typical scenario, an aircraft echo is reflected from the ground below, appearing to the receiver as an identical target below the correct one. The radar may try to unify the targets, reporting the target at an incorrect height, or eliminating it on the basis of jitter or a physical impossibility. These problems can be Radar multipath echoes from a target cause ghosts to appear. overcome by incorporating a ground map of the radar's surroundings and eliminating all echoes which appear to originate below ground or above a certain height. In newer Air Traffic Control radar equipment, algorithms are used to identify the false targets by comparing the current pulse returns, to those adjacent, as well as calculating return improbabilities. Jamming Radar jamming refers to radio frequency signals originating from sources outside the radar, transmitting in the radar's frequency and thereby masking targets of interest. Jamming may be intentional, as with an electronic warfare tactic, or unintentional, as with friendly forces operating equipment that transmits using the same frequency range. Jamming is considered an active interference source, since it is initiated by elements outside the radar and in general unrelated to the radar signals. Jamming is problematic to radar since the jamming signal only needs to travel one way (from the jammer to the radar receiver) whereas the radar echoes travel two ways (radar-target-radar) and are therefore significantly reduced in power by the time they return to the radar receiver. Jammers therefore can be much less powerful than their jammed radars and still effectively mask targets along the line of sight from the jammer to the radar (mainlobe jamming). Jammers have an added effect of affecting radars along other lines of sight through the radar receiver's sidelobes (sidelobe jamming). Mainlobe jamming can generally only be reduced by narrowing the mainlobe solid angle and cannot fully be eliminated when directly facing a jammer which uses the same frequency and polarization as the radar. Sidelobe jamming can be overcome by reducing receiving sidelobes in the radar antenna design and by using an omnidirectional antenna to detect and disregard non-mainlobe signals. Other anti-jamming techniques are frequency hopping and polarization.

Radar signal processing

Distance measurement
Transit time One way to measure the distance to an object is to transmit a short pulse of radio signal (electromagnetic radiation) and measure the time it takes for the reflection to return. The distance is one-half the product of the round trip time (because the signal has to travel to the target and then back to the receiver) and the speed of the signal. Since radio waves travel at the speed of light, accurate distance measurement requires high-performance electronics. In most cases, the receiver does

Pulse radar: The round-trip time for the radar pulse to get to the target and return is measured. The distance is proportional to this time.

Radar

not detect the return while the signal is being transmitted. Through the use of a duplexer, the radar switches between transmitting and receiving at a predetermined rate. A similar effect imposes a maximum range as well. In order to maximize range, longer times between pulses should be used, referred to as a pulse repetition time, or its reciprocal, pulse repetition frequency. These two effects tend to be at odds with each other, and it is not easy Continuous wave (CW) radar to combine both good short range and good long range in a single radar. This is because the short pulses needed for a good minimum range broadcast have less total energy, making the returns much smaller and the target harder to detect. This could be offset by using more pulses, but this would shorten the maximum range. So each radar uses a particular type of signal. Long-range radars tend to use long pulses with long delays between them, and short range radars use smaller pulses with less time between them. As electronics have improved many radars now can change their pulse repetition frequency, thereby changing their range. The newest radars fire two pulses during one cell, one for short range (10km / 6miles) and a separate signal for longer ranges (100km /60miles). The distance resolution and the characteristics of the received signal as compared to noise depends on the shape of the pulse. The pulse is often modulated to achieve better performance using a technique known as pulse compression. Distance may also be measured as a function of time. The radar mile is the amount of time it takes for a radar pulse to travel one nautical mile, reflect off a target, and return to the radar antenna. Since a nautical mile is defined as 1,852meters, then dividing this distance by the speed of light (299,792,458meters per second), and then multiplying the result by 2 yields a result of 12.36 microseconds in duration. Frequency modulation Another form of distance measuring radar is based on frequency modulation. Frequency comparison between two signals is considerably more accurate, even with older electronics, than timing the signal. By measuring the frequency of the returned signal and comparing that with the original, the difference can be easily measured. This technique can be used in continuous wave radar and is often found in aircraft radar altimeters. In these systems a "carrier" radar signal is frequency modulated in a predictable way, typically varying up and down with a sine wave or sawtooth pattern at audio frequencies. The signal is then sent out from one antenna and received on another, typically located on the bottom of the aircraft, and the signal can be continuously compared using a simple beat frequency modulator that produces an audio frequency tone from the returned signal and a portion of the transmitted signal. Since the signal frequency is changing, by the time the signal returns to the aircraft the transmit frequency has changed. The amount of frequency shift is used to measure distance. The modulation index riding on the receive signal is proportional to the time delay between the radar and the reflector. The amount of that frequency shift becomes greater with greater time delay. The measure of the amount of frequency shift is directly proportional to the distance traveled. That distance can be displayed on an instrument, and it may also be available via the transponder. This signal processing is similar to that used in speed detecting Doppler radar. Example systems using this approach are AZUSA, MISTRAM, and UDOP. A further advantage is that the radar can operate effectively at relatively low frequencies. This was important in the early development of this type when high frequency signal generation was difficult or expensive. Terrestrial radar uses low-power FM signals that cover a larger frequency range. The multiple reflections are analyzed mathematically for pattern changes with multiple passes creating a computerized synthetic image. Doppler effects are used which allows slow moving objects to be detected as well as largely eliminating "noise" from the

Radar surfaces of bodies of water.

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Speed measurement
Speed is the change in distance to an object with respect to time. Thus the existing system for measuring distance, combined with a memory capacity to see where the target last was, is enough to measure speed. At one time the memory consisted of a user making grease pencil marks on the radar screen and then calculating the speed using a slide rule. Modern radar systems perform the equivalent operation faster and more accurately using computers. If the transmitter's output is coherent (phase synchronized), there is another effect that can be used to make almost instant speed measurements (no memory is required), known as the Doppler effect. Most modern radar systems use this principle into doppler radar and pulse-doppler radar systems (weather radar, military radar, etc...). The Doppler effect is only able to determine the relative speed of the target along the line of sight from the radar to the target. Any component of target velocity perpendicular to the line of sight cannot be determined by using the Doppler effect alone, but it can be determined by tracking the target's azimuth over time. It is possible to make a doppler radar without any pulsing, known as a continuous-wave radar (CW radar), by sending out a very pure signal of a known frequency. CW radar is ideal for determining the radial component of a target's velocity. CW radar is typically used by traffic enforcement to measure vehicle speed quickly and accurately where range is not important. When using a pulsed radar, the variation between the phase of successive returns gives the distance the target has moved between pulses, and thus its speed can be calculated. Other mathematical developments in radar signal processing include time-frequency analysis (Weyl Heisenberg or wavelet), as well as the chirplet transform which makes use of the fact that radar returns from moving targets typically "chirp" (change their frequency as a function of time).

Pulse-Doppler signal processing

Pulse-Doppler signal processing includes frequency filtering in the detection process. The space between each transmit pulse is divided into range cells or range gates. Each cell is filtered independently much like the process used by a spectrum analyzer to produce the display showing different frequencies. Each different distance produces a different spectrum. These spectra are used to perform the detection process. This is required to achieve acceptable performance in hostile environments involving weather, terrain, and electronic countermeasures. The primary purpose is to measure both the amplitude and frequency of the aggregate reflected signal from multiple distances. This is used with weather radar to measure radial wind velocity and precipitation rate in each different volume of air. This is linked with computing systems to produce a real-time electronic weather map. Aircraft safety depends upon continuous access to accurate weather radar information that is used to prevent injuries and accidents. Weather radar uses a low PRF. Coherency requirements are not as strict as those for military systems because individual signals ordinarily do not need to be separated. Less sophisticated filtering is required, and range ambiguity processing is not normally needed with weather radar in comparison with military radar intended to track air vehicles.

Pulse-Doppler signal processing. The Range Sample axis represents individual samples taken in between each transmit pulse. The Range Interval axis represents each successive transmit pulse interval during which samples are taken. The Fast Fourier Transform process converts time-domain samples into frequency domain spectra. This is sometimes called the bed of nails.

Radar The alternate purpose is "look-down/shoot-down" capability required to improve military air combat survivability. Pulse-Doppler is also used for ground based surveillance radar required to defend personnel and vehicles.[25][26] Pulse-Doppler signal processing increases the maximum detection distance using less radiation in close proximity to aircraft pilots, shipboard personnel, infantry, and artillery. Reflections from terrain, water, and weather produce signals much larger than aircraft and missiles, which allows fast moving vehicles to hide using nap-of-the-earth flying techniques and stealth technology to avoid detection until an attack vehicle is too close to destroy. Pulse-Doppler signal processing incorporates more sophisticated electronic filtering that safely eliminates this kind of weakness. This requires the use of medium pulse-repetition frequency with phase coherent hardware that has a large dynamic range. Military applications require medium PRF which prevents range from being determined directly, and range ambiguity resolution processing is required to identify the true range of all reflected signals. Radial movement is usually linked with Doppler frequency to produce a lock signal that cannot be produced by radar jamming signals. Pulse-Doppler signal processing also produces audible signals that can be used for threat identification.[25]

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Reduction of interference effects

Signal processing is employed in radar systems to reduce the radar interference effects. Signal processing techniques include moving target indication, Pulse-Doppler signal processing, moving target detection processors, correlation with secondary surveillance radar targets, space-time adaptive processing, and track-before-detect. Constant false alarm rate and digital terrain model processing are also used in clutter environments.

Plot and track extraction

Radar video returns on aircraft can be subjected to a plot extraction process whereby spurious and interfering signals are discarded. A sequence of target returns can be monitored through a device known as a plot extractor. The non relevant real time returns can be removed from the displayed information and a single plot displayed. In some radar systems, or alternatively in the command and control system to which the radar is connected, a radar tracker is used to associate the sequence of plots belonging to individual targets and estimate the targets' headings and speeds.

Engineering
A radar's components are: A transmitter that generates the radio signal with an oscillator such as a klystron or a magnetron and controls its duration by a modulator. A waveguide that links the transmitter and the antenna. A duplexer that serves as a switch between the antenna and the transmitter or the receiver for the signal when the antenna is used in both situations. A receiver. Knowing the shape of the desired received signal (a pulse), an optimal receiver can be designed using a matched filter. An electronic section that controls all those devices and the antenna to perform the radar scan ordered by software. A link to end users.
Radar components

Radar

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Antenna design
Radio signals broadcast from a single antenna will spread out in all directions, and likewise a single antenna will receive signals equally from all directions. This leaves the radar with the problem of deciding where the target object is located. Early systems tended to use omnidirectional broadcast antennas, with directional receiver antennas which were pointed in various directions. For instance the first system to be deployed, Chain Home, used two straight antennas at right angles for reception, each on a different display. The maximum return would be detected with an antenna at right angles to the target, and a minimum with the antenna pointed directly at it (end on). The operator could determine the direction to a target by rotating the antenna so one display showed a maximum while the other shows a minimum. One serious limitation with this type of solution is that the broadcast is sent out in all directions, so the amount of energy in the direction being examined is a small part of that transmitted. To get a reasonable amount of power on the "target", the transmitting aerial should also be directional. Parabolic reflector More modern systems use a steerable parabolic "dish" to create a tight broadcast beam, typically using the same dish as the receiver. Such systems often combine two radar frequencies in the same antenna in order to allow automatic steering, or radar lock. Parabolic reflectors can be either symmetric parabolas or spoiled parabolas: Symmetric parabolic antennas produce a narrow "pencil" beam in both the X and Y dimensions and consequently have a higher gain. The NEXRAD Pulse-Doppler weather radar uses a symmetric antenna to perform detailed volumetric scans of the atmosphere. Spoiled parabolic antennas produce a narrow beam in one dimension and a relatively wide beam in the other. This feature is useful if target detection over a wide range of angles is more important than target location in three dimensions. Most 2D surveillance radars use a spoiled parabolic antenna with a narrow azimuthal beamwidth and wide vertical beamwidth. This beam configuration allows the radar operator to detect an aircraft at a specific azimuth but at an indeterminate height. Conversely, so-called "nodder" height finding radars use a dish with a narrow vertical beamwidth and wide azimuthal beamwidth to detect an aircraft at a specific height but with low azimuthal precision. Types of scan Primary Scan: A scanning technique where the main antenna aerial is moved to produce a scanning beam, examples include circular scan, sector scan etc. Secondary Scan: A scanning technique where the antenna feed is moved to produce a scanning beam, examples include conical scan, unidirectional sector scan, lobe switching etc. Palmer Scan: A scanning technique that produces a scanning beam by moving the main antenna and its feed. A Palmer Scan is a combination of a Primary Scan and a Secondary Scan.

Surveillance radar antenna

Radar Slotted waveguide Applied similarly to the parabolic reflector, the slotted waveguide is moved mechanically to scan and is particularly suitable for non-tracking surface scan systems, where the vertical pattern may remain constant. Owing to its lower cost and less wind exposure, shipboard, airport surface, and harbour surveillance radars now use this in preference to the parabolic antenna.

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Slotted waveguide antenna

Phased array Another method of steering is used in a phased array radar. This uses an array of similar aerials suitably spaced, the phase of the signal to each individual aerial being controlled so that the signal is reinforced in the desired direction and cancels in other directions. If the individual aerials are in one plane and the signal is fed to each aerial in phase with all others then the signal will reinforce in a direction perpendicular to that plane. By altering the relative phase of the signal fed to each aerial the direction of the beam can be moved because the direction of constructive interference will move. Because phased array radars require no physical movement the beam can scan at thousands of degrees per second, fast enough to irradiate and track many individual Phased array: Not all radar antennas must rotate to scan the sky. targets and still run a wide-ranging search periodically. By simply turning some of the antennas on or off, the beam can be spread for searching, narrowed for tracking, or even split into two or more virtual radars. However, the beam cannot be effectively steered at small angles to the plane of the array, so for full coverage multiple arrays are required, typically disposed on the faces of a triangular pyramid (see picture). Phased array radars have been in use since the earliest years of radar use in World War II, but limitations of the electronics led to fairly poor accuracy. Phased array radars were originally used for missile defense. They are the heart of the ship-borne Aegis combat system and the Patriot Missile System and are increasingly used in other areas because the lack of moving parts makes them more reliable, which sometimes permits a much larger effective antenna, useful in fighter aircraft applications that offer only confined space for mechanical scanning. As the price of electronics has fallen, phased array radars have become more common. Almost all modern military radar systems are based on phased arrays, where the small additional cost is offset by the improved reliability of a system with no moving parts. Traditional moving-antenna designs are still widely used in roles where cost is a significant factor such as air traffic surveillance, weather radars and similar systems. Phased array radars are valued for use in aircraft since they can track multiple targets. The first aircraft to use a phased array radar was the B-1B Lancer. The first aircraft fighter to use phased array radar was the Mikoyan MiG-31. The MiG-31M's SBI-16 Zaslon phased array radar is considered to be the world's most powerful fighter

Radar radar.[27] Phased-array interferometry or, aperture synthesis techniques, using an array of separate dishes that are phased into a single effective aperture, are not typically used for radar applications, although they are widely used in radio astronomy. Because of the thinned array curse, such arrays of multiple apertures, when used in transmitters, result in narrow beams at the expense of reducing the total power transmitted to the target. In principle, such techniques used could increase the spatial resolution, but the lower power means that this is generally not effective. Aperture synthesis by post-processing of motion data from a single moving source, on the other hand, is widely used in space and airborne radar systems.

14

Frequency bands
The traditional band names originated as code-names during World War II and are still in military and aviation use throughout the world. They have been adopted in the United States by the Institute of Electrical and Electronics Engineers and internationally by the International Telecommunication Union. Most countries have additional regulations to control which parts of each band are available for civilian or military use. Other users of the radio spectrum, such as the broadcasting and electronic countermeasures industries, have replaced the traditional military designations with their own systems.

Radar frequency bands

Band name HF P VHF UHF Frequency range 330 MHz < 300MHz 30300MHz 3001000MHz Wavelength range 10100 m 1 m+ 110 m 0.31 m Notes

coastal radar systems, over-the-horizon radar (OTH) radars; 'high frequency' 'P' for 'previous', applied retrospectively to early radar systems Very long range, ground penetrating; 'very high frequency' Very long range (e.g. ballistic missile early warning), ground penetrating, foliage penetrating; 'ultra high frequency' Long range air traffic control and surveillance; 'L' for 'long' Moderate range surveillance, Terminal air traffic control, long-range weather, marine radar; 'S' for 'short' Satellite transponders; a compromise (hence 'C') between X and S bands; weather; long range tracking Missile guidance, marine radar, weather, medium-resolution mapping and ground surveillance; in the USA the narrow range 10.525GHz 25MHz is used for airport radar; short range tracking. Named X band because the frequency was a secret during WW2. high-resolution from German kurz, meaning 'short'; limited use due to absorption by water vapour, so Ku and Ka were used instead for surveillance. K-band is used for detecting clouds by meteorologists, and by police for detecting speeding motorists. K-band radar guns operate at 24.150 0.100GHz. mapping, short range, airport surveillance; frequency just above K band (hence 'a') Photo radar, used to trigger cameras which take pictures of license plates of cars running red lights, operates at 34.300 0.100GHz. millimetre band, subdivided as below. The frequency ranges depend on waveguide size. Multiple letters are assigned to these bands by different groups. These are from Baytron, a now defunct company that made test equipment. Very strongly absorbed by atmospheric oxygen, which resonates at 60GHz. used as a visual sensor for experimental autonomous vehicles, high-resolution meteorological observation, and imaging. used for through-the-wall radar and imaging systems.

L S

12 GHz 24GHz

1530 cm 7.515cm

C X

48GHz 812GHz

3.757.5cm 2.53.75cm

Ku K

1218GHz 1824GHz

1.672.5cm 1.111.67cm

Ka

2440GHz

0.751.11cm

mm

40300GHz

7.5mm 1mm

V W

4075GHz 75110GHz

4.07.5mm 2.74.0mm

UWB

1.610.5GHz

18.75cm 2.8cm

Radar

15

Radar modulators
Modulators act to provide the waveform of the RF-pulse. There are two different radar modulator designs: high voltage switch for non-coherent keyed power-oscillators[28] These modulators consist of a high voltage pulse generator formed from a high voltage supply, a pulse forming network, and a high voltage switch such as a thyratron. They generate short pulses of power to feed the e.g. magnetron, a special type of vacuum tube that converts DC (usually pulsed) into microwaves. This technology is known as pulsed power. In this way, the transmitted pulse of RF radiation is kept to a defined, and usually, very short duration. hybrid mixers,[29] fed by a waveform generator and an exciter for a complex but coherent waveform. This waveform can be generated by low power/low-voltage input signals. In this case the radar transmitter must be a power-amplifier, e.g. a klystron tube or a solid state transmitter. In this way, the transmitted pulse is intrapulse-modulated and the radar receiver must use pulse compression technique.

Radar coolant
Coolanol (silicate ester) was used in several military radars in the 1970s. However, it is hygroscopic, leading to formation of highly flammable alcohol. The loss of a U.S. Navy aircraft in 1978 was attributed to a silicate ester fire.[30] Coolanol is also expensive and toxic. The U.S. Navy has instituted a program named Pollution Prevention (P2) to reduce or eliminate the volume and toxicity of waste, air emissions, and effluent discharges. Because of this Coolanol is used less often today.

Notes
[1] Mark Maybury, the MITRE Corporation. "Social Radar for Smart Power" (http:/ / www. mitre. org/ work/ tech_papers/ 2010/ 10_0745/ 10_0745. pdf). . Retrieved 2012-01-24. [2] "Radar definition in multiple dictionaries" (http:/ / www. answers. com/ topic/ radar). Answers.com. . Retrieved 2008-10-09. [3] Kostenko, A. A., A. I. Nosich, and I. A. Tishchenko, "Radar Prehistory, Soviet Side," Proc. of IEEE APS International Symposium 2001, vol.4. p. 44, 2003 [4] Christian Hlsmeyer by Radar World (http:/ / www. radarworld. org/ huelsmeyer. html) [5] Patent DE165546; Verfahren, um metallische Gegenstnde mittels elektrischer Wellen einem Beobachter zu melden. [6] Verfahren zur Bestimmung der Entfernung von metallischen Gegenstnden (Schiffen o. dgl.), deren Gegenwart durch das Verfahren nach Patent 16556 festgestellt wird. [7] GB 13170 (http:/ / worldwide. espacenet. com/ textdoc?DB=EPODOC& IDX=GB13170) Telemobiloscope [8] The Electrical Experimenter, 1917 [9] Post-War Research and Development of Radio Communication Equipment (http:/ / earlyradiohistory. us/ 1963hw28. htm) [10] Radar (http:/ / earlyradiohistory. us/ 1963hw38. htm) [11] Watson, Raymond C., Jr. (2009-11-25). Radar Origins Worldwide: History of Its Evolution in 13 Nations Through World War II (http:/ / books. google. com/ ?id=g-rQQgAACAAJ). Trafford Publishing. ISBN978-1-4269-2111-7. . [12] http:/ / www. teslasociety. com/ time. jpg [13] FR 788795 (http:/ / worldwide. espacenet. com/ textdoc?DB=EPODOC& IDX=FR788795) Nouveau systme de reprage d'obstacles et ses applications [14] (French) Copy of Patents for the invention of radar (http:/ / www. radar-france. fr/ brevet radar1934. htm) on www.radar-france.fr [15] Hearst Magazines (1935-12). Popular Mechanics (http:/ / books. google. com/ ?id=x98DAAAAMBAJ& pg=PA844). Hearst Magazines. p.844. . [16] John Erickson. Radio-Location and the Air Defence Problem: The Design and Development of Soviet Radar. Science Studies, Vol. 2, No. 3 (Jul., 1972), pp. 241-263 [17] Page, Robert Morris, The Origin of Radar, Doubleday Anchor, New York, 1962, p. 66 [18] Bonnier Corporation (1935-10). Popular Science (http:/ / books. google. com/ ?id=bygDAAAAMBAJ& pg=PA29). Bonnier Corporation. p.29. . [19] Goebel, Greg (2007-01-01). "The Wizard War: WW2 & The Origins Of Radar" (http:/ / www. vectorsite. net/ ttwiz_01. html). . Retrieved 2007-03-24. [20] Alan Dower Blumlein (2002). "The story of RADAR Development" (http:/ / www. doramusic. com/ Radar. htm). . Retrieved 2011-05-06. [21] British man first to patent radar (http:/ / www. patent. gov. uk/ media/ pressrelease/ 2001/ 1009. htm) official site of the Patent Office [22] GB 593017 (http:/ / worldwide. espacenet. com/ textdoc?DB=EPODOC& IDX=GB593017) Improvements in or relating to wireless systems

Radar
[23] Bonnier Corporation (1941-12). Popular Science (http:/ / books. google. com/ ?id=hCcDAAAAMBAJ& pg=PA56). Bonnier Corporation. p.56. . [24] Hearst Magazines (1941-09). Popular Mechanics (http:/ / books. google. com/ ?id=69kDAAAAMBAJ& pg=PA26). Hearst Magazines. p.26. . [25] "Ground Surveillance Radars and Military Intelligence" (http:/ / www. mit. edu/ ~lrv/ cornell/ publications/ Ground Surveillance Radars and Military Intelligence. pdf). Syracuse Research Corporation; Massachusetts Institute of Technology. . [26] "AN/PPS-5 Ground Surveillance Radar" (http:/ / www. youtube. com/ watch?v=B0q1Pgz6Cm8). You Tube; jaglavaksoldier's Channel. . [27] MiG-31 FOXHOUND (http:/ / www. globalsecurity. org/ military/ world/ russia/ mig-31. htm) [28] Radartutorial (http:/ / www. radartutorial. eu/ / 08. transmitters/ tx06. en. html) [29] Radartutorial (http:/ / www. radartutorial. eu/ / 08. transmitters/ tx10. en. html) [30] Stropki, Michael A. (1992). "Polyalphaolefins: A New Improved Cost Effective Aircraft Radar Coolant" (http:/ / www. dtic. mil/ cgi-bin/ GetTRDoc?AD=ADA250517& Location=U2& doc=GetTRDoc. pdf). Melbourne, Australia: Aeronautical Research Laboratory, Defense Science and Technology Organisation, Department of Defense. . Retrieved 2010-03-18.

16

References
Barrett, Dick, " All you ever wanted to know about British air defence radar (http://www.radarpages.co.uk/ index.htm)". The Radar Pages. (History and details of various British radar systems) Buderi, " Telephone History: Radar History (http://www.privateline.com/TelephoneHistory3/ radarhistorybuderi.html)". Privateline.com. (Anecdotal account of the carriage of the world's first high power cavity magnetron from Britain to the US during WW2.) Ekco Radar WW2 Shadow Factory (http://www.ekco-radar.co.uk/) The secret development of British radar. ES310 " Introduction to Naval Weapons Engineering.". (Radar fundamentals section) (http://www.fas.org/ man/dod-101/navy/docs/es310/syllabus.htm) Hollmann, Martin, " Radar Family Tree (http://www.radarworld.org/index.html)". Radar World (http:// www.radarworld.org/). Penley, Bill, and Jonathan Penley, " Early Radar History (http://www.penleyradararchives.org.uk/history/ introduction.htm)an Introduction". 2002. Pub 1310 Radar Navigation and Maneuvering Board Manual, National Imagery and Mapping Agency, Bethesda, MD 2001 (US govt publication '...intended to be used primarily as a manual of instruction in navigation schools and by naval and merchant marine personnel.') Swords, Sen S., Technical History of the Beginnings of Radar, IEE History of Technology Series, Vol. 6, London: Peter Peregrinus, 1986

Further reading
Reg Batt (1991). The radar army: winning the war of the airwaves. ISBN978-0-7090-4508-3. E. G. Bowen (1998-01-01). Radar Days. Taylor & Francis. ISBN978-0-7503-0586-0. Michael Bragg (2002-05-01). RDF1: The Location of Aircraft by Radio Methods 1935-1945. Twayne Publishers. ISBN978-0-9531544-0-1. Louis Brown (1999). A radar history of World War II: technical and military imperatives. Taylor & Francis. ISBN978-0-7503-0659-1. Robert Buderi (1996). The invention that changed the world: how a small group of radar pioneers won the Second World War and launched a technological revolution. ISBN978-0-684-81021-8. Burch, David F., Radar For Mariners, McGraw Hill, 2005, ISBN 978-0-07-139867-1. Ian Goult (2011). Secret Location: A witness to the Birth of Radar and its Postwar Influence. History Press. ISBN978-0-7524-5776-5. Peter S. Hall (1991-03). Radar. Potomac Books Inc. ISBN978-0-08-037711-7. Derek Howse; Naval Radar Trust (1993-02). Radar at sea: the royal Navy in World War 2. Naval Institute Press. ISBN978-1-55750-704-4. R. V. Jones (1998-08). Most Secret War. Wordsworth Editions Ltd. ISBN978-1-85326-699-7.

Radar Kaiser, Gerald, Chapter 10 in "A Friendly Guide to Wavelets", Birkhauser, Boston, 1994. Kouemou, Guy (Ed.): Radar Technology. InTech, 2010, ISBN 978-953-307-029-2, ( Radar Technology - Free Open Access Book | InTechOpen (http://www.intechopen.com/books/show/title/radar-technology)). Colin Latham; Anne Stobbs (1997-01). Radar: A Wartime Miracle. Sutton Pub Ltd. ISBN978-0-7509-1643-1. Franois Le Chevalier (2002). Principles of radar and sonar signal processing. Artech House Publishers. ISBN978-1-58053-338-6. David Pritchard (1989-08). The radar war: Germany's pioneering achievement 1904-45. Harpercollins. ISBN978-1-85260-246-8. Merrill Ivan Skolnik (1980-12-01). Introduction to radar systems. ISBN978-0-07-066572-9. Merrill Ivan Skolnik (1990). Radar handbook. McGraw-Hill Professional. ISBN978-0-07-057913-2. George W. Stimson (1998). Introduction to airborne radar. SciTech Publishing. ISBN978-1-891121-01-2. Younghusband, Eileen., Not an Ordinary Life. How Changing Times Brought Historical Events into my Life, Cardiff Centre for Lifelong Learning, Cardiff, 2009., ISBN 987-0-9561156-9-0 (Pages 3667 contain the experiences of a WAAF radar plotter in WWII.) Younghusband, Eileen., One Woman's War. Cardiff. Candy Jar Books. 2011. ISBN 978-0-9566826-2-8 David Zimmerman (2001-02). Britain's shield: radar and the defeat of the Luftwaffe. Sutton Pub Ltd. ISBN978-0-7509-1799-5.

17

External links
MIT Video Course: Introduction to Radar Systems (http://ocw.mit.edu/resources/ res-ll-001-introduction-to-radar-systems-spring-2007/) A set of 10 video lectures developed at Lincoln Laboratory to develop an understanding of radar systems and technologies. Popular Science, August 1943, What Are the Facts About RADAR (http://books.google.com/ books?id=_yYDAAAAMBAJ&pg=PA66&dq=popular+science+june+1941&hl=en& ei=cT2TTNqUB9Ofnwfn49ywCA&sa=X&oi=book_result&ct=result&resnum=4& ved=0CDwQ6AEwAw#v=onepage&q&f=true) one of the first detailed factual articles on radar history, principles and operation published in the US "The Great Detective", 1946. Story of the development of radar by the Chrysler Corporation (http:// imperialclub.com/Yr/1945/46Radar/Cover.htm) Christian Hlsmeyer and the early days of radar (http://www.xs4all.nl/~aobauer/Huelspart1def.pdf) Radar: The Canadian History of Radar - Canadian War Museum (http://www.warmuseum.ca/cwm/ exhibitions/radar/index_e.shtml) Radar technology principles (http://www.radartutorial.eu/index.en.html) History of radar (http://math.la.asu.edu/~kuang/LM/030902-Radar_History10.pdf) Radar invisibility with metamaterials (http://www.metamaterials.net) Radar Research Center-Italy (http://crr.sesm.it) Early radar development in the UK (http://www.purbeckradar.org.uk/) Principles of radar target acquisition and weapon guidance systems (http://ourworld.compuserve.com/ homepages/edperry/ewtutor1.htm) Cloaking and radar invisibility (http://www.radartechnology.eu/) The Secrets of Radar Museum (http://www.secretsofradar.com) 84th Radar Evaluation Squadron (http://www.rades.hill.af.mil/) Radar (http://www.skybrary.aero/index.php/Radar) EKCO WW II ASV radar units (http://www.ekco-radar.co.uk/ASV19/asv.php) RAF Air Defence Radar Museum (http://www.radarmuseum.co.uk/) Radar - A case study highlighting the vital contribution physics research has made to major technological development (http://www.iop.org/publications/iop/2011/page_47522.html)

Radar The short film Radar and Its Applications (1962) (http://www.archive.org/details/gov.archives.arc.892095) is available for free download at the Internet Archive [more]

18

Article Sources and Contributors

19

Article Sources and Contributors

Radar Source: http://en.wikipedia.org/w/index.php?oldid=477773470 Contributors: 119, 128.59.58.xxx, 209.239.196.xxx, 2over0, A. Carty, A.R., ADude, Aarchiba, AdjustShift, AeroPsico, Ahbushnell, Ahoerstemeier, Ahunt, Al Silonov, Alai, Alanbrowne, Alansohn, Alex.tan, Alexander.stohr, Alga, Allstarecho, Alphasinus, Altenmann, Altmany, Alvaro, Amalas, American Eagle, American2, Amoruso, Amorymeltzer, Andre Engels, Andrea105, Andux, Andyjsmith, Angusmclellan, Animum, Anna Lincoln, Annetna, Anttin, Apoc2400, Arch dude, Armstrong1113149, ArnoldReinhold, Arodin66, Arpingstone, Arz1969, Ashley Y, Astairefred, Astromahitis, Atif.t2, Atollinchi, Aude, Ausir, Avaragado, Average Earthman, Axlq, Aymatth2, B. 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Image Sources, Licenses and Contributors

File:Radar antenna.jpg Source: http://en.wikipedia.org/w/index.php?title=File:Radar_antenna.jpg License: Public Domain Contributors: Angeloleithold, Dual Freq, Get It, Huntster, Saperaud, Tony Wills, 1 anonymous edits File:Radar-hatzerim-1-1.jpg Source: http://en.wikipedia.org/w/index.php?title=File:Radar-hatzerim-1-1.jpg License: Creative Commons Attribution-Sharealike 3.0 Contributors: Bukvoed File:Chain home.jpg Source: http://en.wikipedia.org/w/index.php?title=File:Chain_home.jpg License: Public Domain Contributors: Original uploader was Stuart166axe at en.wikipedia File:Radar antennas on USS Theodore Roosevelt SPS-64.jpg Source: http://en.wikipedia.org/w/index.php?title=File:Radar_antennas_on_USS_Theodore_Roosevelt_SPS-64.jpg License: Public Domain Contributors: U.S. Navy File:weather radar.jpg Source: http://en.wikipedia.org/w/index.php?title=File:Weather_radar.jpg License: unknown Contributors: NOAA's National Weather Service File:Radar-height.PNG Source: http://en.wikipedia.org/w/index.php?title=File:Radar-height.PNG License: GNU Free Documentation License Contributors: Pierre cb File:Multipath propagation diagram en.svg Source: http://en.wikipedia.org/w/index.php?title=File:Multipath_propagation_diagram_en.svg License: Public Domain Contributors: Original image: Lithium57 English translation: MichaelBillington (talk) File:Radaroperation.gif Source: http://en.wikipedia.org/w/index.php?title=File:Radaroperation.gif License: Creative Commons Attribution-Sharealike 2.0 Contributors: Original uploader was Averse at de.wikipedia File:Sonar Principle EN.svg Source: http://en.wikipedia.org/w/index.php?title=File:Sonar_Principle_EN.svg License: Creative Commons Attribution-ShareAlike 3.0 Unported Contributors: Georg Wiora (Dr. Schorsch) File:Pulse doppler signal processing.png Source: http://en.wikipedia.org/w/index.php?title=File:Pulse_doppler_signal_processing.png License: Creative Commons Attribution-Sharealike 3.0 Contributors: User:Nanoatzin File:Radar composantes.svg Source: http://en.wikipedia.org/w/index.php?title=File:Radar_composantes.svg License: Creative Commons Attribution-Sharealike 3.0 Contributors: Pierre cb, Vanessaezekowitz, WikipediaMaster, 1 anonymous edits File:SPS-10 radar antenna on a Knox class frigate.jpg Source: http://en.wikipedia.org/w/index.php?title=File:SPS-10_radar_antenna_on_a_Knox_class_frigate.jpg License: unknown Contributors: DON S. MONTGOMERY File:PAVE PAWS Radar Clear AFS Alaska.jpg Source: http://en.wikipedia.org/w/index.php?title=File:PAVE_PAWS_Radar_Clear_AFS_Alaska.jpg License: Public Domain Contributors: AirBa, Avron, Chetvorno, Tony Wills

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