An optical fiber or optical fibre is really a flexible, SZ stranding line created by drawing glass (silica) or plastic into a diameter slightly thicker than that of a human hair.[1] Optical fibers are used in most cases as a method to deliver light involving the two ends of the fiber and look for wide usage in fiber-optic communications, where they permit transmission over longer distances as well as higher bandwidths (data rates) than wire cables. Fibers are employed as an alternative to metal wires because signals travel along these with lesser amounts of loss; moreover, fibers are also immune to electromagnetic interference, an issue from which metal wires suffer excessively. Fibers are also employed for illumination, and they are wrapped in bundles to make sure they may be used to carry images, thus allowing viewing in confined spaces, as in the case of a fiberscope. Specially engineered fibers are also used for a variety of other applications, many of them being fiber optic sensors and fiber lasers.

Optical fibers typically include a transparent core surrounded by a transparent cladding material by using a lower index of refraction. Light is saved in the core with the phenomenon of total internal reflection that causes the fiber to act like a waveguide. Fibers that support many propagation paths or transverse modes are known as multi-mode fibers (MMF), while those that support just one mode are called single-mode fibers (SMF). Multi-mode fibers normally have a wider core diameter and can be used for short-distance communication links as well as for applications where high power needs to be transmitted.[citation needed] Single-mode fibers can be used for most communication links over 1,000 meters (3,300 ft).[citation needed]

Having the capacity to join optical fibers with low loss is important in fiber optic communication. This can be more complex than joining electrical wire or cable and involves careful cleaving of your fibers, precise alignment in the fiber cores, and the coupling of such aligned cores. For applications that need to have a permanent connection a fusion splice is typical. In this particular technique, an electrical arc is utilized to melt the ends in the fibers together. Another common strategy is a mechanical splice, in which the ends from the fibers are kept in contact by mechanical force. Temporary or semi-permanent connections are produced by way of specialized optical fiber connectors.

The realm of applied science and engineering interested in the look and implementation of optical fibers is recognized as fiber optics. The word was coined by Indian physicist Narinder Singh Kapany who is widely acknowledged as being the father of fiber optics.

Daniel Colladon first described this “light fountain” or “light pipe” in a 1842 article titled In the reflections of your ray of light in a parabolic liquid stream. This type of illustration originates from a later article by Colladon, in 1884.

Guiding of light by refraction, the key that creates fiber optics possible, was first demonstrated by Daniel Colladon and Jacques Babinet in Paris in early 1840s. John Tyndall included a demonstration of it in their public lectures in London, 12 years later. Tyndall also wrote in regards to the property of total internal reflection within an introductory book regarding the nature of light in 1870:

If the light passes from air into water, the refracted ray is bent to the perpendicular… When the ray passes from water to air it is bent through the perpendicular… In the event the angle that the ray in water encloses with the perpendicular for the surface be greater than 48 degrees, the ray will not likely quit water in any way: it will probably be totally reflected at the surface…. The angle which marks the limit where total reflection begins is known as the limiting angle from the medium. For water this angle is 48°27′, for flint glass it can be 38°41′, while for diamond it can be 23°42′.

Within the late 19th and early 20th centuries, light was guided through bent glass rods to illuminate body cavities. Practical applications like close internal illumination during dentistry appeared at the beginning of the twentieth century. Image transmission through tubes was demonstrated independently from the radio experimenter Clarence Hansell and also the television pioneer John Logie Baird within the 1920s. Within the 1930s, Heinrich Lamm revealed that one could transmit images via a bundle of unclad optical fibers and tried it for internal medical examinations, but his work was largely forgotten.

In 1953, Dutch scientist Bram van Heel first demonstrated image transmission through bundles of optical fibers by using a transparent cladding. That same year, Harold Hopkins and Narinder Singh Kapany at Imperial College in London succeeded to make image-transmitting bundles with ten thousand fibers, and subsequently achieved image transmission by way of a 75 cm long bundle which combined several thousand fibers. Their article titled “An adaptable fibrescope, using static scanning” was published in the journal Nature in 1954. The 1st practical fiber optic semi-flexible gastroscope was patented by Basil Hirschowitz, C. Wilbur Peters, and Lawrence E. Curtiss, researchers on the University of Michigan, in 1956. At the same time of developing the gastroscope, Curtiss produced the very first glass-clad fibers; previous optical fiber ribbon machine had relied on air or impractical oils and waxes since the low-index cladding material. A number of other image transmission applications soon followed.

Kapany coined the word ‘fiber optics’ in an article in Scientific American in 1960, and wrote the very first book concerning the new field.

The initial working fiber-optical data transmission system was demonstrated by German physicist Manfred Börner at Telefunken Research Labs in Ulm in 1965, that has been followed by the initial patent application for this technology in 1966. NASA used fiber optics from the television cameras that were delivered to the moon. Back then, the utilization in the cameras was classified confidential, and employees handling the cameras must be supervised by someone having an appropriate security clearance.

Charles K. Kao and George A. Hockham from the British company Standard Telephones and Cables (STC) were the first, in 1965, to promote the concept that the attenuation in optical fibers may be reduced below 20 decibels per kilometer (dB/km), making fibers a practical communication medium.They proposed that this attenuation in fibers available at that time was due to impurities that could be removed, instead of by fundamental physical effects for example scattering. They correctly and systematically theorized the light-loss properties for optical fiber, and pointed out the best material for such fibers – silica glass with higher purity. This discovery earned Kao the Nobel Prize in Physics during 2009.

The crucial attenuation limit of 20 dB/km was basically achieved in 1970 by researchers Robert D. Maurer, Donald Keck, Peter C. Schultz, and Frank Zimar working for American glass maker Corning Glass Works. They demonstrated a fiber with 17 dB/km attenuation by doping silica glass with titanium. Many years later they produced a fiber with only 4 dB/km attenuation using germanium dioxide as the core dopant. In 1981, General Electric produced fused quartz ingots which can be drawn into strands 25 miles (40 km) long.

Initially high-quality optical fibers could basically be manufactured at 2 meters per second. Chemical engineer Thomas Mensah joined Corning in 1983 and increased the pace of manufacture to in excess of 50 meters per second, making optical fiber cables less expensive than traditional copper ones. These innovations ushered inside the era of optical dexopky04 telecommunication.

The Italian research center CSELT worked with Corning to build up practical optical fiber cables, resulting in the initial metropolitan fiber optic cable being deployed in Torino in 1977. CSELT also developed a young technique for SZ stranding line, called Springroove.

Attenuation in modern optical cables is much under in electrical copper cables, leading to long-haul fiber connections with repeater distances of 70-150 kilometers (43-93 mi). The erbium-doped fiber amplifier, which reduced the price of long-distance fiber systems by reduction of or eliminating optical-electrical-optical repeaters, was co-designed by teams led by David N. Payne from the University of Southampton and Emmanuel Desurvire at Bell Labs in 1986.

The emerging field of photonic crystals resulted in the development in 1991 of photonic-crystal fiber, which guides light by diffraction coming from a periodic structure, as opposed to by total internal reflection. The very first photonic crystal fibers became commercially available in 2000. Photonic crystal fibers can carry higher power than conventional fibers in addition to their wavelength-dependent properties can be manipulated to improve performance.