Coastal ocean dynamics applications radar

Last updated
A CODAR source, detected in Atlanta, Georgia, on 14195 kHz, as seen from a software-defined radio's waterfall display. The sweeping, diagonal line is the CODAR signal. CODAR signal centered at ~14195 kHz.PNG
A CODAR source, detected in Atlanta, Georgia, on 14195 kHz, as seen from a software-defined radio's waterfall display. The sweeping, diagonal line is the CODAR signal.
Recording of CONDAR transmissions on 4.630mhz

Coastal ocean dynamics applications radar (CODAR) is a type of portable, land-based, high frequency (HF) radar developed between 1973 and 1983 at NOAA's Wave Propagation Laboratory in Boulder, Colorado. CODAR is a noninvasive system that can measure and map near-surface ocean currents in coastal waters. It is transportable and can produce ocean current maps on site in near real time. Moreover, using CODAR it is possible to measure wave heights and produce an indirect estimate of local wind direction.

Contents

Equipment

CODAR utilizes a compact antenna system that consists of crossed loops and a whip for receiving and a whip for transmitting radio pulses. [1] The system can be transported by vehicle and can operate from a portable power supply; for modern instrumentation a minimum capacity of 1050 Watts is recommended. [2] CODAR is capable of operating in virtually all weather conditions (it can tolerate temperatures from 0 °F (-18 °C) to 90 °F (32 °C) [3] ) and the relatively small dimensions of the antenna system allow CODAR deployment even in highly populated and rocky coastal areas. However, as the signal is rapidly attenuated by land, the antenna has to be mounted as close to the water surface as possible.

Modern equipment can operate from 3 to 50 MHz and can be programmed for unattended operation for periods of up to two weeks. [4]

The main equipment is cabled to the electronic segment, that is housed nearby in a sheltered environment and contains the system hardware, where information is stored. A minicomputer controls the radar and processes the signals and the operator can communicate with the system through a portable keyboard terminal.

The raw spectral data can be processed on-line to obtain real-time outputs and the final data products can be displayed on a graphics terminal or printed with a hardcopy plotter. Off-line processing at a later date can be accomplished as well.

Applications

The main purpose of CODAR is to measure surface current. The systems' range and resolution vary with environmental conditions and antenna placement. In general, however, in their long-range mode, modern CODAR can measure out to 100–200 km offshore with a resolution of 3–12 km. By increasing the frequency, resolutions as fine as 200–500 m can be obtained, but the observation range is shortened to 15–20 km. [5]

However, the actual range can be limited by radio interference, high-ocean states and ground conditions in the vicinity of the antennas. Wet and moist sandy soils enhance ground wave propagation, whereas dry and rocky grounds attenuate the signal. [6]

A single CODAR system can measure only the component of surface current travelling toward or away from the radar, so to determine the total surface current vectors, it is necessary to use at least a two-system setup. An array of CODAR sites can be employed to obtain regional coverage. In a multiple radar configuration, spacing between two radar systems should be approximately 15 to 40 km for long-range open ocean mode and 8 to 20 km in short-range mode. [7]

Typically, CODAR data are averaged over one hour to reduce the noisiness of the sea echo. Therefore, current maps can be produced every hour. This period can be reduced to approximately 20 minutes, however data collected over short periods may be noisy. [7]

CODAR's measurements are useful for both military and civil purposes. Main applications include coastal engineering and public safety projects, planning of navigational seaways, mitigation of ocean pollution, search and rescue operations, oil-spill mitigation in real time and larval population connectivity assessment. Also, data obtained from CODAR are used as inputs for global resource monitoring and weather forecasting models and are particularly helpful for tidal and storm-surge measurements. [8] Moreover, the direction of propagation of wave energy and the period of the most energetic waves, can be extracted from the measurements, which are important for many practical applications in design and operation of coastal and offshore structures.

Theory of operation

CODAR operates using sky transmission of waves in the high frequency (HF) band (3–30 MHz), as electromagnetic waves in this band have wavelengths commensurate with wind-driven gravity waves on the ocean surface. [9] As the customer needs, it can be used in single or multi-frequency mode. As the ocean has a rough surface, when a high frequency signal reaches the ocean surface, a portion of the incident energy is scattered back towards the source and the receiver measures the reflected signal. This backscattering (or reflection) produces an energy spectrum at the receiver, even if the energy source is single-frequency, because of the shape and motion of the sea surface. Interpreting the spectral returns for various transmit frequencies is the key to extracting information about the ocean [10] and, specifically, to measure surface currents.

As a consequence of Bragg’s Scattering Law, the strongest received return comes from ocean waves traveling directly toward or away from the radar source and whose physical wavelength is exactly one-half as long as the transmitted radar wave. The return signal is processed and its spectral analysis provides the sea-echo Doppler spectrum, where two dominant peaks at different frequencies can be recognized.

Displacement of these peaks away from their known frequencies is called the “echo Doppler shift” and allows one to assess the radial velocity of a surface current. That is; the scatter velocity along the line between the hit surface and the radar. In fact, the magnitude of this component of the velocity is proportional to the degree of signal-shift. Therefore, CODAR measures the Doppler-induced frequency-shift (along with the distance from the radar to the sector and directional angle) to provide an estimate of the radial-component of wave-speed in the sector of sea surface of interest.

Measuring surface currents

In order to measure currents, the CODAR equipment computes three components:

Computation of the radial velocity of currents

The signal sent from the CODAR antenna has a known frequency and it moves at the speed of light. Therefore, the wavelength of the signal is known (wavelength = speed of light / frequency). Exploiting Bragg’s Law, CODAR maximizes the scattered HF signal, given that the resonance will only occur for the given wavelength:

λs = λt / (2 * cos(φ) )

where λs is the wavelength of surface ocean wave, λt is the wavelength of transmitted signal and φ is the angle of incidence between the signal and the ocean surface

As the CODAR antennas are usually placed at sea level, the angle of incidence theta can be assumed to be zero. Therefore, the equation reduces to:

λs = λt / 2

This means that when the emitted signal hits waves with wavelength equal to one-half of the transmitted signal, the signal that is scattered back to the antenna will be in phase. Therefore, these waves will produce a scattered signal “stronger” and thus easily identifiable, which is measured by the CODAR system. Thus, the current speed is extracted by determining the Doppler Shift of the waves. [11]

However, the above equations represent a simplified model, as they assume that the reflecting waves are not moving. This is of course untrue and, because of the motion, the frequency of the scattered signal (and therefore its wavelength) is not the same as the one of the transmitted signal. In fact, “waves moving toward the receiver increase the return frequency, while waves moving away decrease the return frequency”. [11]

Then a further Doppler shift (Δf) is observed and, by measuring it, it is possible to determine the radial velocity νs component of the surface current by using the Doppler formula:

Δf = νs / λs

Computation of the distance to target

The range to target is calculated starting from the time delay, which is obtained by subtracting the return signal time from the transmitted signal one.

Computation of the angular direction to target

CODAR is a "direction finding system". The signal is received by two loop antennas and a monopole. Whereas the signal the monopole receives does not vary with the direction of the incoming signal, the signal received by the two loop antennas (positioned at a 90° angle) does vary with direction. [11] This information permits a software to determine the direction of the signal.

Once calculated the radial velocity of currents, distance to target, and the angular direction to target it is possible to determine the current vector and to construct current vector maps. In fact, for the area in which vector data from two CODAR sites overlap, it is possible to calculate the velocity and direction of the current and comparisons with surface drifters and error analysis made in 1979 indicate that CODAR measures surface currents with at least 10 cm/s accuracy. [12] In 2010, retailers of modern CODAR equipments guarantee an accuracy typically < 7 cm/s of the total current velocity and 1–2 cm of the tidal component, in normal environment condition. [13] However, the accuracy of the system depends on several factors, such as signal-to-noise ratios, geometry and pointing errors.

Limitations

There are some limitations inherent to the system that do not permit certain applications. Here are presented the main practical limitations:

As discussed before, for a given look angle, a single CODAR station can detect only the component of flow traveling toward or away from its location. Radial currents from two or more sites should be combined to obtain vector surface current estimates. Moreover, when using two CODAR stations the so-called "baseline problem" can affect the measurement. This occurs when both the instruments measure the same component of velocity. To avoid this problem and resolve properly the current vector, generally two radials must have an angle between 30° and 150°. [14]

See also

Related Research Articles

The Doppler effect is the change in the frequency of a wave in relation to an observer who is moving relative to the source of the wave. The Doppler effect is named after the physicist Christian Doppler, who described the phenomenon in 1842. A common example of Doppler shift is the change of pitch heard when a vehicle sounding a horn approaches and recedes from an observer. Compared to the emitted frequency, the received frequency is higher during the approach, identical at the instant of passing by, and lower during the recession.

<span class="mw-page-title-main">Radar</span> Object detection system using radio waves

Radar is a radiolocation system that uses radio waves to determine the distance (ranging), angle (azimuth), and radial velocity of objects relative to the site. It is used to detect and track aircraft, ships, spacecraft, guided missiles, motor vehicles, map weather formations, and terrain. A radar system consists of a transmitter producing electromagnetic waves in the radio or microwaves domain, a transmitting antenna, a receiving antenna and a receiver and processor to determine properties of the objects. Radio waves from the transmitter reflect off the objects and return to the receiver, giving information about the objects' locations and speeds.

<span class="mw-page-title-main">Doppler radar</span> Type of radar equipment

A Doppler radar is a specialized radar that uses the Doppler effect to produce velocity data about objects at a distance. It does this by bouncing a microwave signal off a desired target and analyzing how the object's motion has altered the frequency of the returned signal. This variation gives direct and highly accurate measurements of the radial component of a target's velocity relative to the radar. The term applies to radar systems in many domains like aviation, police radar detectors, navigation, meteorology, etc.

<span class="mw-page-title-main">Millimeter cloud radar</span> Weather radar tuned to cloud detection

Millimeter-wave cloud radars, also denominated cloud radars, are radar systems designed to monitor clouds with operating frequencies between 24 and 110 GHz. Accordingly, their wavelengths range from 1 mm to 1.11 cm, about ten times shorter than those used in conventional S band radars such as NEXRAD.

<span class="mw-page-title-main">Synthetic-aperture radar</span> Form of radar used to create images of landscapes

Synthetic-aperture radar (SAR) is a form of radar that is used to create two-dimensional images or three-dimensional reconstructions of objects, such as landscapes. SAR uses the motion of the radar antenna over a target region to provide finer spatial resolution than conventional stationary beam-scanning radars. SAR is typically mounted on a moving platform, such as an aircraft or spacecraft, and has its origins in an advanced form of side looking airborne radar (SLAR). The distance the SAR device travels over a target during the period when the target scene is illuminated creates the large synthetic antenna aperture. Typically, the larger the aperture, the higher the image resolution will be, regardless of whether the aperture is physical or synthetic – this allows SAR to create high-resolution images with comparatively small physical antennas. For a fixed antenna size and orientation, objects which are further away remain illuminated longer – therefore SAR has the property of creating larger synthetic apertures for more distant objects, which results in a consistent spatial resolution over a range of viewing distances.

<span class="mw-page-title-main">Direction finding</span> Measurement of the direction from which a received signal was transmitted

Direction finding (DF), or radio direction finding (RDF), is the use of radio waves to determine the direction to a radio wave source. The source may be a cooperating radio transmitter or may be an inadvertant source, a naturally-occurring radio source, or an illicit or enemy system. Radio direction finding differs from radar in that only the direction is determined by any one receiver; a radar system usually also gives a distance to the object of interest, as well as direction. By triangulation, the location of a radio source can be determined by measuring its direction from two or more locations. Radio direction finding is used in radio navigation for ships and aircraft, to locate emergency transmitters for search and rescue, for tracking wildlife, and to locate illegal or interfering transmitters. During the Second World War, radio direction finding was used by both sides to locate and direct aircraft, surface ships, and submarines.

<span class="mw-page-title-main">Imaging radar</span> Application of radar which is used to create two-dimensional images

Imaging radar is an application of radar which is used to create two-dimensional images, typically of landscapes. Imaging radar provides its light to illuminate an area on the ground and take a picture at radio wavelengths. It uses an antenna and digital computer storage to record its images. In a radar image, one can see only the energy that was reflected back towards the radar antenna. The radar moves along a flight path and the area illuminated by the radar, or footprint, is moved along the surface in a swath, building the image as it does so.

<span class="mw-page-title-main">Satellite geodesy</span> Measurement of the Earth using satellites

Satellite geodesy is geodesy by means of artificial satellites—the measurement of the form and dimensions of Earth, the location of objects on its surface and the figure of the Earth's gravity field by means of artificial satellite techniques. It belongs to the broader field of space geodesy. Traditional astronomical geodesy is not commonly considered a part of satellite geodesy, although there is considerable overlap between the techniques.

<span class="mw-page-title-main">Pulse-Doppler radar</span> Type of radar system

A pulse-Doppler radar is a radar system that determines the range to a target using pulse-timing techniques, and uses the Doppler effect of the returned signal to determine the target object's velocity. It combines the features of pulse radars and continuous-wave radars, which were formerly separate due to the complexity of the electronics.

<span class="mw-page-title-main">Continuous-wave radar</span>

Continuous-wave radar is a type of radar system where a known stable frequency continuous wave radio energy is transmitted and then received from any reflecting objects. Individual objects can be detected using the Doppler effect, which causes the received signal to have a different frequency from the transmitted signal, allowing it to be detected by filtering out the transmitted frequency.

<span class="mw-page-title-main">TOPEX/Poseidon</span> Satellite mission to map ocean surface topography

TOPEX/Poseidon was a joint satellite altimeter mission between NASA, the U.S. space agency; and CNES, the French space agency, to map ocean surface topography. Launched on August 10, 1992, it was the first major oceanographic research satellite. TOPEX/Poseidon helped revolutionize oceanography by providing data previously impossible to obtain. Oceanographer Walter Munk described TOPEX/Poseidon as "the most successful ocean experiment of all time." A malfunction ended normal satellite operations in January 2006.

An acoustic doppler current profiler (ADCP) is a hydroacoustic current meter similar to a sonar, used to measure water current velocities over a depth range using the Doppler effect of sound waves scattered back from particles within the water column. The term ADCP is a generic term for all acoustic current profilers, although the abbreviation originates from an instrument series introduced by RD Instruments in the 1980s. The working frequencies range of ADCPs range from 38 kHz to several megahertz.

<span class="mw-page-title-main">Wind profiler</span>

A wind profiler is a type of weather observing equipment that uses radar or sound waves (SODAR) to detect the wind speed and direction at various elevations above the ground. Readings are made at each kilometer above sea level, up to the extent of the troposphere. Above this level there is inadequate water vapor present to produce a radar "bounce." The data synthesized from wind direction and speed is very useful to meteorological forecasting and timely reporting for flight planning. A twelve-hour history of data is available through NOAA websites.

<span class="mw-page-title-main">Sodar</span> Meteorological instrument

Sodar, an acronym of sonic detection and ranging, is a meteorological instrument used as a wind profiler based on the scattering of sound waves by atmospheric turbulence. Sodar equipment is used to measure wind speed at various heights above the ground, and the thermodynamic structure of the lower layer of the atmosphere.

<span class="mw-page-title-main">Wave radar</span> Technology for measuring surface waves on water

Wave radar is a type of radar for measuring wind waves. Several instruments based on a variety of different concepts and techniques are available, and these are all often called. This article, gives a brief description of the most common ground-based radar remote sensing techniques.

Moving target indication (MTI) is a mode of operation of a radar to discriminate a target against the clutter. It describes a variety of techniques used for finding moving objects, like an aircraft, and filter out unmoving ones, like hills or trees. It contrasts with the modern stationary target indication (STI) technique, which uses details of the signal to directly determine the mechanical properties of the reflecting objects and thereby find targets whether they are moving or not.

<span class="mw-page-title-main">Terminal Doppler Weather Radar</span>

Terminal Doppler Weather Radar (TDWR) is a Doppler weather radar system with a three-dimensional "pencil beam" used primarily for the detection of hazardous wind shear conditions, precipitation, and winds aloft on and near major airports situated in climates with great exposure to thunderstorms in the United States. As of 2011, all were in-service with 45 operational radars, some covering multiple airports in major metropolitan locations, across the United States & Puerto Rico. Several similar weather radars have also been sold to other countries such as China (Hong Kong). Funded by the United States Federal Aviation Administration (FAA), TDWR technology was developed in the early 1990s at Lincoln Laboratory, part of the Massachusetts Institute of Technology, to assist air traffic controllers by providing real-time wind shear detection and high-resolution precipitation data.

A laser surface velocimeter (LSV) is a non-contact optical speed sensor measuring velocity and length on moving surfaces. Laser surface velocimeters use the laser Doppler principle to evaluate the laser light scattered back from a moving object. They are widely used for process and quality control in industrial production processes.

Lucy R. Wyatt is an English mathematician and a professor in the School of Mathematics and Statistics at the University of Sheffield, Yorkshire. She is a member of the Environmental Dynamics research group in the School of Mathematics.

Doppler radio direction finding, or Doppler DF for short, is a radio direction finding method that generates accurate bearing information with a minimum of electronics. It is best suited to VHF and UHF frequencies, and takes only a short time to indicate a direction. This makes it suitable for measuring the location of the vast majority of commercial, amateur and automated broadcasts. Doppler DF is one of the most widely used direction finding techniques. Other direction finding techniques are generally used only for fleeting signals, or longer or shorter wavelengths.

References

  1. Barrick et aL, Ocean Surface Currents Mapped by Radar - Science, New Series, Vol. 198, No. 4313 (Oct. 14, 1977), pp. 138-144, https://www.jstor.org/stable/1744926 1977
  2. see Technical Specification sheet 2010 at "Archived copy" (PDF). Archived from the original (PDF) on 2010-06-08. Retrieved 2012-11-02.{{cite web}}: CS1 maint: archived copy as title (link)
  3. "Archived copy" (PDF). Archived from the original (PDF) on 2010-06-08. Retrieved 2012-11-02.{{cite web}}: CS1 maint: archived copy as title (link)
  4. High Frequency Radar Measurements of Coastal Ocean Parameters, CETN-I-41 6/86, Coastal Engineering Research Centre, Technical Note. "Archived copy" (PDF). Archived from the original (PDF) on 2013-02-21. Retrieved 2012-11-02.{{cite web}}: CS1 maint: archived copy as title (link)
  5. http://www.codar.com/SeaSonde_gen_specs.shtml, Technical Specification sheet 2010, CODAR OCEAN SENSORS SeaSonde
  6. J. D. Paduan, H. C. Graber, Introduction to high-frequency radar: reality and myth, OCEANOGRAPHY Vol. 10, NO. 2, 1997, page 38
  7. 1 2 K. Andresen, S. Litvin - The Use of CODAR High Frequency Radar to Attain Wave Height Measurements (http://marine.rutgers.edu/mrs/codar/waves/project2.html
  8. B. J. Lipa, D. E. Barrick, Tidal and Storm-Surge Measurements with Single-Site CODAR, JOURNAL OF OCEANIC ENGINEERING, VOL. OE-11, NO. 2, APRIL 1986, pages 241-245
  9. J. D. Paduan, L. Washburn, High-Frequency Radar Observations of Ocean Surface Currents, Annual Review of Marine Science, 2012
  10. J. D. Paduan, L. Washburn, 2011 - High Frequency Radar Observations of Ocean Surface Currents
  11. 1 2 3 "Untitled".
  12. M. Evans, T. Georges, Coastal Ocean Dynamics Radar (CODAR): NOAA's Surface Current Mapping System, 1979
  13. "CODAR Ocean Sensors - Products - the SeaSonde®".
  14. J. D. Paduan, H. C. Graber, Introduction to high-frequency radar: reality and mith, OCEANOGRAPHY VoI. 10, NO. 2, 1997, page 37

Further reading