Corner reflector

Working principle of a corner reflector
Comparison of the effect of corner (1) and spherical (2) retroreflectors on three light rays. Reflective surfaces are drawn in dark blue.

A corner reflector is a retroreflector consisting of three mutually perpendicular, intersecting flat surfaces, which reflects waves back directly towards the source, but translated. The three intersecting surfaces often have square shapes. Radar corner reflectors made of metal are used to reflect radio waves from radar sets. Optical corner reflectors, called corner cubes, made of three-sided glass prisms, are used in surveying and laser rangefinding.

Principle

The incoming ray is reflected three times, once by each surface, which results in a reversal of direction.[1][2] To see this, the three corresponding normal vectors of the corner's perpendicular sides can be considered to form a basis (a rectangular coordinate system) (x, y, z) in which to represent the direction of an arbitrary incoming ray, [a, b, c]. When the ray reflects from the first side, say x, the ray's x component, a, is reversed to −a while the y and z components are unchanged, resulting in a direction of [−a, b, c]. Similarly, when reflected from side y and finally from side z, the b and c components are reversed. Therefore, the ray direction goes from [a, b, c] to [−a, b, c] to [−a, −b, c] to [−a, −b, −c], and it leaves the corner reflector with all three components of direction exactly reversed. The distance travelled, relative to a plane normal to the direction of the rays, is also equal for any ray entering the reflector, regardless of the location where it first reflects.

In diagram 1 the green ray is shown as reflecting from only one surface. This is a special case where the incoming ray is exactly normal (perpendicular) to one of the reflective faces. In the same diagram the orange and red rays are shown reflecting off of two surfaces. This is again a special case, the requirement being that the incoming ray is parallel to one of the reflecting planes. (In diagram 2, showing a retroreflective sphere, the incoming and outgoing rays are approximately parallel in special cases.)

In radar

(far left) A radar corner reflector (diamond-shaped object) on the mast of a yacht. Note that this one is improperly deployed; to best reflect surface radar it should be deployed in the so-called "rain-catching" configuration so as to present an inside corner as shown on the "radar testing" image.
(near left) Buoy in San Diego Harbor. Metal plates near the top form corner reflectors to reflect radar signals.
(near right) Corner reflector for radar testing
(far right) Multireflector at the Nevada Test Site used as radar target for simulated nuclear bombing

Radar corner reflectors are designed to reflect the microwave radio waves emitted by radar sets back toward the radar antenna. This causes them to show a strong "return" on radar screens. A simple corner reflector consists of three conducting sheet metal or screen surfaces at 90° angles to each other, attached to one another at the edges, forming a "corner". These reflect radio waves coming from in front of them back parallel to the incoming beam. To create a corner reflector that will reflect radar waves coming from any direction, 8 corner reflectors are placed back-to-back in an octahedron (diamond) shape. The reflecting surfaces must be larger than several wavelengths of the radio waves to function.[3]

In maritime navigation they are placed on bridge abutments, buoys, ships and, especially, lifeboats, to ensure that these show up strongly on ship radar screens. Corner reflectors are placed on the vessel's masts at a height of at least 4.6 meters (15 feet) above sea level (giving them an approximate minimum horizon distance of 8 kilometers or 4.5 nautical miles). Marine radar uses X-band microwaves with wavelengths of 2.5 - 3.75 cm, so small reflectors less than 30 cm across are used. In aircraft navigation, corner reflectors are installed on rural runways, to make them show up on aircraft radar.

In optics

Corner cube reflector
Apollo 15 Lunar Laser Ranging RetroReflector (LRRR) installed on the Moon

In optics, corner reflectors typically consist of three mirrors or reflective prism faces which return an incident light beam in the opposite direction. In surveying, retroreflector prisms are commonly used as targets for long-range electronic distance measurement using a total station.

Five arrays of optical corner reflectors have been placed on the Moon for use by Lunar Laser Ranging experiments observing a laser's time-of-flight to measure the Moon's orbit more precisely than was possible before. The three largest were placed by NASA as part of the Apollo program, and the Soviet Union's built two smaller ones into the Lunokhod rovers.

Automobile and bicycle tail lights are molded with arrays of small corner reflectors, with different sections oriented for viewing from different angles. Reflective paint for visibility at night usually contains retroreflective spherical beads. Thin plastic with microscopic corner reflector structures can be used as tape, on signs, or sewn or molded onto clothing.

Other examples

Corner reflectors can also occur accidentally. Tower blocks with balconies are often accidental corner reflectors for sound and return a distinctive echo to an observer making a sharp noise, such as a hand clap, nearby. Similarly, in radar interpretation, an object that has multiple reflections from smooth surfaces produces a radar return of greater magnitude than might be expected from the physical size of the object. This effect was put to use on the ADM-20 Quail, a small missile which had the same radar cross section as a B-52.

See also

References

  1. Newman, William I. (2012). Continuum Mechanics in the Earth Sciences. Cambridge University Press. pp. 6–7. ISBN 0521562899.
  2. Bernstein, Matt A.; William A. Friedman (2011). Thinking About Equations: A Practical Guide for Developing Mathematical Intuition in the Physical Sciences and Engineering. John Wiley and Sons. p. 193. ISBN 1118210646.
  3. Kraus, John &, Marhefka, Ronald (2002). Antennas for All Applications, 3rd ed. Mc Graw Hill. p. 365. ISBN 0-07-112240-0.
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