Rogue wave

Rogue waves (also known as freak waves, monster waves, episodic waves, killer waves, extreme waves, and abnormal waves) are unusually large, unexpected and suddenly appearing surface waves that can be extremely dangerous, even to large ships such as ocean liners.[2]

Rogue waves present considerable danger for several reasons: they are rare, are unpredictable, may appear suddenly or without warning, and can impact with tremendous force. A 12-metre (39 ft) wave in the usual "linear" wave model would have a breaking pressure of 6 metric tons per square metre [t/m2] (59 kPa; 8.5 psi). Although modern ships are designed to tolerate a breaking wave of 15 t/m2 (150 kPa; 21 psi), a rogue wave can dwarf both of these figures with a breaking pressure of 100 t/m2 (0.98 MPa; 140 psi).[3]

In oceanography, rogue waves are more precisely defined as waves whose height is more than twice the significant wave height (Hs or SWH), which is itself defined as the mean of the largest third of waves in a wave record. Therefore, rogue waves are not necessarily the biggest waves found on the water; they are, rather, unusually large waves for a given sea state. Rogue waves seem not to have a single distinct cause, but occur where physical factors such as high winds and strong currents cause waves to merge to create a single exceptionally large wave.[2]

Rogue waves can occur in media other than water. They appear to be ubiquitous in nature and have also been reported in liquid helium, in nonlinear optics and in microwave cavities. Recent research has focused on optical rogue waves which facilitate the study of the phenomenon in the laboratory. A 2015 paper studied the wave behavior around a rogue wave, including optical, and the Draupner wave, and concluded that "rogue events do not necessarily appear without a warning, but are often preceded by a short phase of relative order".[4] A 2012 study confirmed the existence of oceanic rogue holes, the inverse of rogue waves, where the depth of the hole can reach more than twice the significant wave height.


Rogue waves are an open water phenomenon, in which winds, currents, non-linear phenomena such as solitons, and other circumstances cause a wave to briefly form that is far larger than the "average" large occurring wave (the significant wave height or "SWH") of that time and place. The basic underlying physics that makes phenomena such as rogue waves possible is that different waves can travel at different speeds, and so they can "pile up" in certain circumstances, known as "constructive interference". (In deep ocean the speed of a gravity wave is proportional to the square root of its wavelength, i.e., the distance peak-to-peak between adjacent waves.) However, other situations can also give rise to rogue waves, particularly situations where non-linear effects or instability effects can cause energy to move between waves and be concentrated in one or very few extremely large waves before returning to "normal" conditions.

Once considered mythical and lacking hard evidence for their existence, rogue waves are now proven to exist and known to be a natural ocean phenomenon. Eyewitness accounts from mariners and damage inflicted on ships have long suggested they occurred. The first scientific evidence of the existence of rogue waves came with the recording of a rogue wave by the Gorm platform in the central North Sea in 1984. A stand-out wave was detected with a wave height of 11 metres (36 ft) in a relatively low sea state.[5] However, the wave that caught the attention of the scientific community was the digital measurement of the "Draupner wave", a rogue wave at the Draupner platform in the North Sea on January 1, 1995, with a maximum wave height of 25.6 metres (84 ft) with a peak elevation of 18.5 metres (61 ft). During that event, minor damage was also inflicted on the platform, far above sea level, confirming that the reading was valid.[1]

Their existence has also since been confirmed by video and photographs, and satellite imagery and radar of the ocean surface,[6] by stereo wave imaging systems,[7] by pressure transducers on the sea-floor and notably by oceanographic research vessels.[8] In February 2000, a British oceanographic research vessel, the RRS Discovery, sailing in the Rockall Trough west of Scotland encountered the largest waves ever recorded by scientific instruments in the open ocean, with a SWH of 18.5 metres (61 ft) and individual waves up to 29.1 metres (95 ft).[9] "In 2004 scientists using three weeks of radar images from European Space Agency satellites found ten rogue waves, each 25 metres (82 ft) or higher."[10]

A rogue wave is a natural ocean phenomenon that is not caused by land movement, only lasts briefly, occurs in a limited location, and most often happens far out at sea.[2] Rogue waves are considered rare but potentially very dangerous, since they can involve the spontaneous formation of massive waves far beyond the usual expectations of ship designers, and can overwhelm the usual capabilities of ocean-going vessels which are not designed for such encounters. Rogue waves are, therefore distinct from tsunamis.[2] Tsunamis are caused by massive displacement of water, often resulting, from sudden movement of the ocean floor, after which they propagate at high speed over a wide area. They are nearly unnoticeable in deep water and only become dangerous as they approach the shoreline and the ocean floor becomes shallower;[11] therefore, tsunamis do not present a threat to shipping at sea. (The only ships lost in the 2004 Asian tsunami were in port.) They are also distinct from megatsunamis, which are single massive waves caused by sudden impact, such as meteor impact or landslides within enclosed or limited bodies of water. They are also different from the waves described as "hundred-year waves", which is a purely statistical prediction of the highest wave likely to occur in a hundred-year period in a particular body of water.

Rogue waves have now been proven to be the cause of the sudden loss of some ocean-going vessels. Well-documented instances include the freighter MS München, lost in 1978[12] and the MV Derbyshire lost in 1980, the largest British ship ever lost at sea.[13][14] A rogue wave has been implicated in the loss of other vessels including the Ocean Ranger, which was a semi-submersible mobile offshore drilling unit that sank in Canadian waters on 15 February 1982.[15] In 2007 the United States National Oceanic and Atmospheric Administration compiled a catalogue of more than 50 historical incidents probably associated with rogue waves.[16]

History of rogue wave knowledge

Mythical status

In 1826, French scientist and naval officer Captain Jules Dumont d'Urville reported waves as high as 108 ft (33 m) in the Indian Ocean with three colleagues as witnesses, yet he was publicly ridiculed by fellow scientist François Arago. In that era it was widely held that no wave could exceed 30 ft (9 m).[17][18] Author Susan Casey wrote that much of that disbelief came because there were very few people who had seen a rogue wave, and until the advent of steel double-hulled ships of the 20th century "people who encountered 100-foot rogue waves generally weren't coming back to tell people about it."[19]

State of knowledge prior to the 1995 Draupner wave

Unusual waves have been studied scientifically for many years (for example, John Scott Russell's Wave of Translation, an 1834 study of a soliton wave), but these were not linked conceptually to sailors stories of encounters with giant rogue ocean waves, as the latter were believed to be scientifically implausible.

Since the 19th century, oceanographers, meteorologists, engineers and ship designers have used a statistical model known as the Gaussian function (or Gaussian Sea or standard linear model) to predict wave height, on the assumption that wave heights in any given sea are tightly grouped around a central (average) value, known as the 'significant wave height'.[20] In a storm sea with a significant wave height of 12 metres (39 ft), the model suggests there will hardly ever be a wave higher than 15 metres (49 ft). One of 30 metres (98 ft) could indeed happen – but only once in ten thousand years (of wave height of 12 metres [39 ft]). This basic assumption was well accepted (and acknowledged to be an approximation). The use of a Gaussian form to model waves has been the sole basis of virtually every text on that topic for the past 100 years.[20][21]

The first known scientific article on "Freak waves" was written by Professor Laurence Draper in 1964. In that paper which has been described as a 'seminal article' he documented the efforts of the National Institute of Oceanography in the early 1960s to record wave height and the highest wave recorded at that time which was about 20 m (67 ft). Draper also described freak wave holes.[22][23][24][25]

However, even as late as the mid 1990s, most popular texts on oceanography such as that by Pirie did not contain any mention of rogue or freak waves.[26] Even after the 1995 Draupner wave, the popular text on Oceanography by Gross (1996) only gave rogue waves a mention and simply stated that "Under extraordinary circumstances unusually large waves called rogue waves can form" without providing any further detail.[27]

Draupner Wave

It is of interest that far from ridiculing the old sailors' stories about enormous waves, modern research has confirmed that such monsters can occur, and that wave heights can exceed by an appreciable amount the maximum values which have been accepted in responsible circles.

Professor Laurence Draper (1971)[25]

In 1995, strong scientific evidence for the existence of rogue waves came with the recording of what has become known as the Draupner wave. The Draupner E is one structure in a gas pipeline support complex operated by Statoil about 160 kilometres (100 mi)58°11′19.30″N 2°28′0.00″E offshore and west by southwest from the southern tip of Norway.[28][29][30] The Draupner E platform is the first major oil platform of the jacket-type attached to the seabed with a bucket foundation instead of pilings and a suction anchoring system.[30] As a precaution, the operator (Statoil) fitted the platform with an extensive array of instrumentation. The instruments continuously check the platform's movements in particular any movement of the foundations during storm events. The state-of-the-art instrumentation fitted to the platform was able to continuously measure seven key parameters:[30]

  • wave height,
  • wave slope,
  • wave hold,
  • pressure of the bucket foundations,
  • tension in the platform pillars, and
  • acceleration on deck and foundations.

The rig was built to withstand a calculated 1-in-10,000 years wave with a predicted height of 20 m (64 ft) and was also fitted with a state-of-the-art laser wave recorder on the platform's underside. At 3 p.m. on 1 January 1995 it recorded a 26 m (85 ft) rogue wave i.e., 6 m [21 ft] taller than the predicted 10,000-year wave, that hit the rig at 72 km/h (45 mph). This was the first confirmed measurement of a freak wave, more than twice as tall and steep as its neighbors, with characteristics that fell outside any known wave model. The wave was recorded by all of the sensors fitted to the platform[30] and it caused enormous interest in the scientific community.[28][30]

Modern knowledge since 1995

Following the evidence of the Draupner wave, research in the area became widespread.

The first scientific study to comprehensively proved that freak waves exist that are clearly outside the range of Gaussian waves was published in 1997.[31] Some research confirms that observed wave height distribution in general follows well the Rayleigh distribution, but in shallow waters during high energy events, extremely high waves are more rare than this particular model predicts.[10] From about 1997 most leading authors acknowledged the existence of rogue waves with the caveat that wave models had been unable to replicate rogue waves.[17]

Statoil researchers presented a paper in 2000, collating evidence that freak waves were not the rare realizations of a typical or slightly non-gaussian sea surface population (classical extreme waves), but rather they were the typical realizations of a rare and strongly non-gaussian sea surface population of waves (freak extreme waves).[32] A workshop of leading researchers in the world attended the first Rogue Waves 2000 workshop held in Brest in November 2000.[33]

In 2000 the British oceanographic vessel RRS Discovery recorded a 29-metre (95 ft) wave off the coast of Scotland near Rockall. This was a scientific research vessel and was fitted with high quality instruments. The subsequent analysis determined that under severe gale force conditions with wind speeds averaging 21 metres per second (68.9 ft/s) a ship-borne wave recorder measured individual waves up to 29.1 metres (95.5 ft) from crest to trough, and a maximum significant wave height of 18.5 metres (60.7 ft). These were some of the largest waves recorded by scientific instruments up to that time. The authors noted that modern wave prediction models are known to significantly under-predict extreme sea states for waves with a significant height (Hs) above 12 metres (39.4 ft). The analysis of this event took a number of years, and noted that "none of the state-of-the-art weather forecasts and wave models — the information upon which all ships, oil rigs, fisheries, and passenger boats rely — had predicted these behemoths." Put simply, a scientific model (and also ship design method) to describe the waves encountered did not exist. This finding was widely reported in the press, which reported that "according to all of the theoretical models at the time under this particular set of weather conditions waves of this size should not have existed".[2][9][28][34][35]

In 2004 the ESA MaxWave project identified more than ten individual giant waves above 25 metres (82 ft) in height during a short survey period of three weeks in a limited area of the South Atlantic. The ESA's ERS satellites have helped to establish the widespread existence of these "rogue" waves.[36][37] By 2007, it was further proven via satellite radar studies that waves with crest to trough heights of 20 metres (66 ft) to 30 metres (98 ft), occur far more frequently than previously thought.[38] It is now known that rogue waves occur in all of the world's oceans many times each day.

Thus acknowledgement of the existence of rogue waves (despite the fact that they cannot plausibly be explained by reference to simple statistical models) is a very modern scientific paradigm.[39] It is now well accepted that rogue waves are a common phenomenon. Professor Akhmediev of the Australian National University, one of the world's leading researchers in this field, has stated that there are about 10 rogue waves in the world's oceans at any moment.[40] Some researchers have speculated that approximately three of every 10,000 waves on the oceans achieve rogue status, yet in certain spots — like coastal inlets and river mouths — these extreme waves can make up three out of every 1,000 waves, because wave energy can be focused.[41]

Rogue waves may also occur in lakes. A phenomenon known as the "Three Sisters" is said to occur in Lake Superior when a series of three large waves forms. The second wave hits the ship's deck before the first wave clears. The third incoming wave adds to the two accumulated backwashes and suddenly overloads the ship deck with tons of water. The phenomenon is one of various theories as to the cause of the sinking of the SS Edmund Fitzgerald on Lake Superior in November 1975.[42]

In reference to extreme events, rogue waves and soliton theory
These are considered to be the most important discoveries in the twentieth and twenty first centuries mathematical and experimental physics.

Optical sciences group, Australian National University[43]

Serious studies of the phenomenon of rogue waves only started about 20–30 years ago and have intensified since about 2005. One of the remarkable features of the rogue waves is that they always appear from nowhere and quickly disappear without a trace. Recent research has suggested that there could also be "super-rogue waves", which are up to five times the average sea-state. Rogue waves has now become a near universal term given by scientists to describe isolated large amplitude waves, that occur more frequently than expected for normal, Gaussian distributed, statistical events. Rogue waves appear to be ubiquitous in nature and are not limited to the oceans. They appear in other contexts and have recently been reported in liquid helium, in nonlinear optics and in microwave cavities. It is now universally accepted by marine researchers that these waves belong to a specific kind of sea wave, not taken into account by conventional models for sea wind waves.[44][45][46][47]

In 2012, researchers at the Australian National University proved the existence of rogue wave holes, an inverted profile of a rogue wave. Their research created rogue wave holes on the water surface, in a water wave tank.[48] In maritime folk-lore, stories of rogue holes are as common as stories of rogue waves. They follow from theoretical analysis but had never been proven experimentally.

In 2019, researchers succeeded in producing a wave with similar characteristics to the Draupner wave (steepness and breaking), and proportionately greater height, using multiple wavetrains meeting at an angle of 120 degrees. Previous research had strongly suggested that the wave resulted from interaction between waves from different directions ("crossing seas"). Their research also highlighted that wave-breaking behavior was not necessarily as expected. If waves met at an angle less than about 60 degrees, then the top of the wave "broke" sideways and downwards (a "plunging breaker"). But from about 60 degrees and greater, the wave began to break vertically upwards, creating a peak that did not reduce the wave height as usual, but instead increased it (a "vertical jet"). They also showed that the steepness of rogue waves could be reproduced in this manner. Finally, they observed that optical instruments such as the laser used for the Draupner wave might be somewhat confused by the spray at the top of the wave, if it broke, and this could lead to uncertainties of around 1–1.5 metres in the wave height. They concluded that "that the onset and type of wave breaking play a significant role and differ significantly for crossing and non-crossing waves. Crucially, breaking becomes less crest-amplitude limiting for sufficiently large crossing angles and involves the formation of near-vertical jets".[49][50]

Research efforts

There are a number of research programmes currently underway focussed on rogue waves including:


Because the phenomenon of rogue waves is still a matter of active research, it is premature to state clearly what the most common causes are or whether they vary from place to place. The areas of highest predictable risk appear to be where a strong current runs counter to the primary direction of travel of the waves; the area near Cape Agulhas off the southern tip of Africa is one such area; the warm Agulhas Current runs to the southwest, while the dominant winds are westerlies. However, since this thesis does not explain the existence of all waves that have been detected, several different mechanisms are likely, with localized variation. Suggested mechanisms for freak waves include the following:

Diffractive focusing 
According to this hypothesis, coast shape or seabed shape directs several small waves to meet in phase. Their crest heights combine to create a freak wave.[73]
Focusing by currents 
Waves from one current are driven into an opposing current. This results in shortening of wavelength, causing shoaling (i.e., increase in wave height), and oncoming wave trains to compress together into a rogue wave.[73] This happens off the South African coast, where the Agulhas Current is countered by westerlies.[64]
Nonlinear effects (modulational instability) 
It seems possible to have a rogue wave occur by natural, nonlinear processes from a random background of smaller waves.[12] In such a case, it is hypothesized, an unusual, unstable wave type may form which 'sucks' energy from other waves, growing to a near-vertical monster itself, before becoming too unstable and collapsing shortly after. One simple model for this is a wave equation known as the nonlinear Schrödinger equation (NLS), in which a normal and perfectly accountable (by the standard linear model) wave begins to 'soak' energy from the waves immediately fore and aft, reducing them to minor ripples compared to other waves. The NLS can be used in deep water conditions. In shallow water, waves are described by the Korteweg–de Vries equation or the Boussinesq equation. These equations also have non-linear contributions and show solitary-wave solutions. A small-scale rogue wave consistent with the nonlinear Schrödinger equation (the Peregrine Solution) was produced in a laboratory water tank in 2011.[74] In particular, the study of solitons, and especially Peregrine solitons, have supported the idea that non-linear effects could arise in bodies of water.[64][75][76][77]
Normal part of the wave spectrum 
Rogue waves are not freaks at all but are part of normal wave generation process, albeit a rare extremity.[73]
Constructive interference of elementary waves 
Rogue waves can result from the constructive interference (dispersive and directional focusing) of elementary 3D waves enhanced by nonlinear effects.[7][78]
Wind wave interactions 
While it is unlikely that wind alone can generate a rogue wave, its effect combined with other mechanisms may provide a fuller explanation of freak wave phenomena. As wind blows over the ocean, energy is transferred to the sea surface. When strong winds from a storm happen to blow in the opposing direction of the ocean current the forces might be strong enough to randomly generate rogue waves. Theories of instability mechanisms for the generation and growth of wind waves—although not on the causes of rogue waves—are provided by Phillips[79] and Miles.[64][80]
Thermal expansion 
When a stable wave group in a warm water column moves into a cold water column the size of the waves must change because energy must be conserved in the system. So each wave in the wave group become smaller because cold water holds more wave energy based on density. The waves are now spaced farther apart and because of gravity they will propagate into more waves to fill up the space and become a stable wave group. If a stable wave group exists in cold water and moves into a warm water column the waves will get larger and the wavelength will be shorter. The waves will seek equilibrium by attempting to displace the waves amplitude because of gravity. However, by starting with a stable wave group the wave energy can displace toward the center of the group. If both the front and back of the wave group are displacing energy toward the center it can become a rogue wave. This would happen only if the wave group is very large.

The spatio-temporal focusing seen in the NLS equation can also occur when the nonlinearity is removed. In this case, focusing is primarily due to different waves coming into phase, rather than any energy transfer processes. Further analysis of rogue waves using a fully nonlinear model by R. H. Gibbs (2005) brings this mode into question, as it is shown that a typical wavegroup focuses in such a way as to produce a significant wall of water, at the cost of a reduced height.

A rogue wave, and the deep trough commonly seen before and after it, may last only for some minutes before either breaking, or reducing in size again. Apart from one single rogue wave, the rogue wave may be part of a wave packet consisting of a few rogue waves. Such rogue wave groups have been observed in nature.[81]

There are three categories of freak waves:

  • "Walls of water" travelling up to 10 km (6 mi) through the ocean
  • "Three Sisters", groups of three waves[82]
  • Single, giant storm waves, building up to fourfold the storm's waves height and collapsing after some seconds[83]

Scientific applications

The possibility of the artificial stimulation of rogue wave phenomena has attracted research funding from DARPA, an agency of the United States Department of Defense. Bahram Jalali and other researchers at UCLA studied microstructured optical fibers near the threshold of soliton supercontinuum generation and observed rogue wave phenomena. After modelling the effect, the researchers announced that they had successfully characterized the proper initial conditions for generating rogue waves in any medium.[84] Additional works carried out in optics have pointed out the role played by a nonlinear structure called Peregrine soliton that may explain those waves that appear and disappear without leaving a trace.[85][86]

Reported encounters

Many of these encounters are only reported in the media, and are not examples of open ocean rogue waves. Often, in popular culture, an endangering huge wave is loosely denoted as a rogue wave, while it has not been (and most often cannot be) established that the reported event is a rogue wave in the scientific sense — i.e. of a very different nature in characteristics as the surrounding waves in that sea state and with very low probability of occurrence (according to a Gaussian process description as valid for linear wave theory).

This section lists a limited selection of notable incidents.

19th century

  • Eagle Island lighthouse (1861) – water broke the glass of the structure's east tower and flooded it, implying a wave that surmounted the 40 m (130 ft) cliff and overwhelmed the 26 m (85 ft) tower.[87]
  • Flannan Isles Lighthouse (1900) – three lighthouse keepers vanished after a storm that resulted in wave-damaged equipment being found 34 metres (112 ft) above sea level.[88][89]

20th century

  • SS Kronprinz Wilhelm, September 18, 1901 – The most modern German ocean liner of its time (winner of the Blue Riband) was damaged on its maiden voyage from Cherbourg to New York by a huge wave. The wave struck the ship head-on.[90]
  • SS Waratah (1909) – Left Durban, South Africa with 211 passengers and crew but did not reach Cape Town, South Africa.[2]
  • RMS Lusitania (1910) - On the night of 10 January 1910, a 23-metre (75 ft) wave struck the ship over the bow, damaging the forecastle deck and smashing the bridge windows.[91]
  • Voyage of the James Caird (1916) – Sir Ernest Shackleton encountered a wave he termed "gigantic" while piloting a lifeboat from Elephant Island to South Georgia Island.[92]
  • RMS Homeric (1924) - Hit by a 24-metre (80 ft) wave while sailing through a hurricane off the East Coast of the United States, injuring seven people, smashing numerous windows and portholes, carrying away one of the lifeboats, and snapping chairs and other fittings from their fastenings.[93]
  • USS Ramapo (AO-12) (1933) – Triangulated at 34 metres (112 ft).[94]
  • RMS Queen Mary (1942) – Broadsided by a 28-metre (92 ft) wave and listed briefly about 52 degrees before slowly righting.[17]
  • SS Flying Enterprise (1951) – Ripped apart amidships and eventually sank 64 kilometres (40 mi) from Falmouth, England.
  • SS Michelangelo (1966) – Hole torn in superstructure, heavy glass smashed 24 metres (80 ft) above the waterline, and three deaths.[94]
  • SS Edmund Fitzgerald (1975) – Lost on Lake Superior. A Coast Guard report blamed water entry to the hatches, which gradually filled the hold, or alternatively errors in navigation or charting causing damage from running onto shoals. However, another nearby ship, the SS Arthur M. Anderson, was hit at a similar time by two rogue waves and possibly a third, and this appeared to coincide with the sinking around ten minutes later.[42]
  • MS München (1978) – Lost at sea leaving only scattered wreckage and signs of sudden damage including extreme forces 20 metres (66 ft) above the water line. Although more than one wave was probably involved, this remains the most likely sinking due to a freak wave.[12]
  • Esso Languedoc (1980) – A 25-to-30-metre (80 to 100 ft) wave washed across the deck from the stern of the French supertanker near Durban, South Africa, and was photographed by the first mate, Philippe Lijour.[95][96]
  • Fastnet Lighthouse – Struck by a 48-metre (157 ft) wave in 1985 [97]
  • MV Derbyshire (1980) – A 91,655 GRT bulk freighter – the largest British ship ever lost at sea – disappeared without trace during Typhoon Orchid on 9 September 1980, with the loss of 44 lives. The wreck was located and extensively surveyed in 1994. One subsequent analysis (which won the 2001 Royal Institution of Naval Architects award for excellence) demonstrated that given the weather conditions pertaining, Derbyshire would almost certainly have encountered waves of at least 28 metres (92 ft), and that even a much smaller rogue wave would have easily destroyed one or more of Derbyshire's cargo hatch covers, leading to the rapid loss of the ship.[98]
  • Draupner wave (North Sea, 1995) – The first rogue wave confirmed with scientific evidence, it had a maximum height of 25.6 metres (84 ft).[99]
  • RMS Queen Elizabeth 2 (1995) – Encountered a 29-metre (95 ft) wave in the North Atlantic, during Hurricane Luis. The Master said it "came out of the darkness" and "looked like the White Cliffs of Dover."[3] Newspaper reports at the time described the cruise liner as attempting to "surf" the near-vertical wave in order not to be sunk.

21st century

  • MS Bremen and Caledonian Star (South Atlantic, 2001) encountered 30-metre (98 ft) freak waves. Bridge windows on both ships were smashed, and all power and instrumentation lost.[3]
  • U.S. Naval Research Laboratory ocean-floor pressure sensors detected a freak wave caused by Hurricane Ivan in the Gulf of Mexico, 2004. The wave was around 27.7 metres (91 ft) high from peak to trough, and around 200 metres (660 ft) long.[100] Their computer models also indicated that waves may have exceeded 40 metres (130 ft) in the eyewall.[101]
  • Norwegian Dawn, (Georgia [US], 2005) On April 16, 2005, after sailing into rough weather off the coast of Georgia, Norwegian Dawn encountered a series of three 21-metre (70 ft) rogue waves. The third wave damaged several windows on the 9th and 10th decks and several decks were flooded. Damage, however, was not extensive and the ship was quickly repaired.[102] Four passengers were slightly injured in this incident.[103]
  • Aleutian Ballad, (Bering Sea, 2005) footage of what is identified as an 18-metre (60 ft) wave appears in an episode of Deadliest Catch. The wave strikes the ship at night and cripples the vessel, causing the boat to tip for a short period onto its side. This is one of the few video recordings of what might be a rogue wave.[104]
  • In 2006, researchers from U.S. Naval Institute theorise rogue waves may be responsible for the unexplained loss of low-flying aircraft, such as U.S. Coast Guard helicopters during Search and Rescue missions.[105]
  • On January 24, 2009 the Augusto González de Linares buoy, located 35 kilometres (22 mi) north of Santander, Spain reported a wave of 26.13 metres (85.7 ft), equivalent to eight floors high, during a storm.[106]
  • MS Louis Majesty (Mediterranean Sea, March 2010) was struck by three successive 8-metre (26 ft) waves while crossing the Gulf of Lion on a Mediterranean cruise between Cartagena and Marseille. Two passengers were killed by flying glass when a lounge window was shattered by the second and third waves. The waves, which struck without warning, were all abnormally high in respect to the sea swell at the time of the incident.[107][108]
  • In 2011, during the filming of Whale Wars the Sea Shepherd Conservation Society patrol vessel MV Brigitte Bardot was hit by a rogue wave on her way back to Fremantle. The wave snapped the pontoons requiring the crew to tie the damaged side down with straps. The vessel was escorted back to Fremantle by the MY Steve Irwin and the MV Shōnan Maru 2 and repaired.[109]
  • The Spanish Deepwater Buoys Network, in January 2014, measured a wave height of 27.81 metres (91.2 ft). The data was taken at the buoy Vilán-Sisargas (Cape Vilan) in Galicia (Spain) during the winter storms, which were particularly severe in Atlantic waters.[110]
  • MS Marco Polo was struck by a rogue wave on the English Channel (February 2014). An 85-year-old man was killed and a woman in her 70s injured.[111]
  • In 2019, Hurricane Dorian's extratropical remnant generated a 100 feet (30 m) rogue wave off the coast of Newfoundland.[112]

Quantifying the impact of rogue waves on ships

The loss of the MS München in 1978 provided some of the first physical evidence of the existence of rogue waves. The MS München was a state-of-the-art cargo ship with multiple water-tight compartments, an expert crew and was considered unsinkable. She was lost with all crew and the wreck has never been found. The only evidence found was the starboard lifeboat which was recovered from floating wreckage some time later. The lifeboats hung from forward and aft blocks 20 metres (66 ft) above the waterline. The pins had been bent back from forward to aft, indicating the lifeboat hanging below it had been struck by a wave that had run from fore to aft of the ship which had torn the lifeboat from the ship. To exert such force the wave must have been considerably higher than 20 metres (66 ft). At the time of the inquiry, the existence of rogue waves was considered so statistically unlikely as to be near impossible. Consequently, the Maritime Court investigation concluded that the severe weather had somehow created an 'unusual event' that had led to the sinking of the München.[12][113]

In 1980 the MV Derbyshire was lost during Typhoon Orchid south of Japan along with all of her crew. The Derbyshire was an ore-bulk-oil combination carrier built in 1976. At 91,655 gross register tons, she was—and remains—the largest British ship ever to have been lost at sea. The wreck was found in June 1994. The survey team deployed a remotely operated vehicle to photograph the wreck. A private report was published in 1998 which prompted the British government to reopen a formal investigation into the sinking. The British government investigation included a comprehensive survey by the Woods Hole Oceanographic Institution which took 135,774 pictures of the wreck during two surveys. The formal forensic investigation concluded that the ship sank because of structural failure and absolved the crew of any responsibility. Most notably, the report determined the detailed sequence of events that led to the structural failure of the vessel. A third comprehensive analysis was subsequently done by Douglas Faulkner, professor of marine architecture and ocean engineering at the University of Glasgow. His 2001 report linked the loss of the MV Derbyshire with the emerging science on freak waves, concluding that the Derbyshire was almost certainly destroyed by a rogue wave.[13][14][114][115][116]

In 2004 an extreme wave was recorded impacting the Admiralty Breakwater, Alderney in the Channel Islands. This breakwater is exposed to the Atlantic Ocean. The peak pressure recorded by a shore-mounted transducer was 745 kilopascals [kPa] (108.1 psi). This pressure far exceeds almost any design criteria for modern ships and this wave would have destroyed almost any merchant vessel.[5]

Work by Smith in 2007 confirmed prior forensic work by Faulkner in 1998 and determined that the MV Derbyshire was exposed to a hydrostatic pressure of a static head of water of about 20 metres (66 ft) with a resultant static pressure of 201 kilopascals (18.7 kN/sq ft).[nb 1] This is in effect 20 metres (66 ft) of green water (possibly a super rogue wave)[nb 2] flowing over the vessel. The deck cargo hatches on the Derbyshire were determined to be the key point of failure when the rogue wave washed over the ship. The design of the hatches only allowed for a static pressure of less than 2 metres (6.6 ft) of water or 17.1 kilopascals (1.59 kN/sq ft),[nb 3] in other words the typhoon load on the hatches was more than ten times the design load. The forensic structural analysis of the wreck of the Derbyshire is now widely regarded as irrefutable.[38]

In addition fast moving waves are now known to also exert extremely high dynamic pressure. It is known that plunging or breaking waves can cause short-lived impulse pressure spikes called Gifle peaks. These can reach pressures of 200 kilopascals (19 kN/sq ft) (or more) for milliseconds, which is sufficient pressure to lead to brittle fracture of mild steel. Evidence of failure by this mechanism was also found on the Derbyshire.[13] Smith has documented scenarios where hydrodynamic pressure of up to 5,650 kilopascals (525 kN/sq ft) or over 500 metric tonnes per 1 square metre (11 sq ft) could occur.[nb 4][38]

Ship failure mechanism

Very few ship-wrecks have ever been fully investigated. The most recent bulk-carrier loss on the open seas to have been subjected to thorough investigation (as at March 2011) was the UK-owned M.V. Derbyshire, which sank in 1980. Its entire crew of forty-four, all British citizens, perished. It took 14 years of pressure from the British public and a privately funded expedition to locate the wreck before a formal remote-camera search and investigation was done by the British government. At least a couple of hundred bulk carriers have been lost since 1980 and none have been properly investigated. A survey of 125 bulk carriers that sank between 1963 and 1996 found that seventy-six probably flooded, another four because of hatch-cover failure, the rest from unidentified causes. Nine other vessels broke completely in two. Causes of the remaining forty losses are unknown.[117] Montgomery-Swan has outlined the generic mechanism of ship failure when encountering a rogue wave:

The scenario is very simple: the weight of the ship accelerates her down the back slope of the previous wave, the bow sticks into the lower part of the front of the giant incoming wave, and thousands of tons of green water fall onto the fore part of the ship. What happens next depends on the structure of the vessel.[23]

Professor Faulkner who did the forensic independent analysis of the loss of the M.V. Derbyshire explains why this is such a problem for bulk carriers. He states that "It is quite possible that some of the many unexplained heavy weather losses (of bulk carriers) may have been caused by hatch cover or coaming failures because fore end plunging due to flooding of large holds can be rapid." He noted in his report that "because of their high inertias and natural pitch periods, these large ships do not rise to the waves, as appropriately experienced masters have confirmed. They tend to bury into them." Faulkner concluded that "beyond any reasonable doubt, the direct cause of the loss of the M.V. Derbyshire was the quite inadequate strength of her cargo hatch covers to withstand the forces of Typhoon Orchid." He also noted that "It is not possible to say which of the eighteen covers failed first, or from which direction the waves came; but evidence and other arguments suggest that the no. 1 hatch covers were probably the first to yield, probably from waves over the bow with the ship hove-to."[13]

Design standards

In November 1997 the International Maritime Organization (IMO) adopted new rules covering survivability and structural requirements for bulk carriers of 150 metres (490 ft) and upwards. The bulkhead and double bottom must be strong enough to allow the ship to survive flooding in hold one unless loading is restricted.[118]

It is now widely held that rogue waves present considerable danger for several reasons: they are rare, unpredictable, may appear suddenly or without warning, and can impact with tremendous force. A 12-metre (39 ft) wave in the usual "linear" model would have a breaking force of 6 metric tons per square metre [t/m2] (8.5 psi). Although modern ships are designed to (typically) tolerate a breaking wave of 15 MT/m2, a rogue wave can dwarf both of these figures with a breaking force far exceeding 100 MT/m2.[3][nb 5] Smith has presented calculations using the International Association of Classification Societies (IACS) Common Structural Rules (CSR) for a typical bulk carrier which are consistent.[nb 6][38]

Peter Challenor, a leading scientist in this field from the National Oceanography Centre in the United Kingdom was quoted in Casey's book in 2010 that "We don’t have that random messy theory for nonlinear waves. At all", he says. "People have been working actively on this for the past 50 years at least. We don’t even have the start of a theory".[28][34]

In 2006 Smith proposed that the International Association of Classification Societies (IACS) recommendation 34 pertaining to standard wave data be modified so that the minimum design wave height be increased to 65 feet (19.8 m). He presented analysis that there was sufficient evidence to conclude that 66 feet (20.1 m) high waves can be experienced in the 25-year lifetime of oceangoing vessels, and that 98 feet (29.9 m) high waves are less likely, but not out of the question. Therefore, a design criterion based on 36 feet (11.0 m) high waves seems inadequate when the risk of losing crew and cargo is considered. Smith has also proposed that the dynamic force of wave impacts should be included in the structural analysis.[119] The Norwegian offshore standards now take into account extreme severe wave conditions and require that a 10,000-year wave does not endanger the ships integrity.[120] Rosenthal notes that as at 2005 rogue waves were not explicitly accounted for in Classification Societies’ Rules for ships’ design.[120] As an example, DNV GL, one of the world's largest international certification body and classification society with main expertise in technical assessment, advisory, and risk management publishes their Structure Design Load Principles which remain largely based on the 'Significant Wave height' and as at January 2016 still has not included any allowance for rogue waves.[121]

The U.S. Navy historically took the design position that the largest wave likely to be encountered was 21.4 m (70 ft). Smith observed in 2007 that the navy now believes that larger waves can occur and the possibility of extreme waves that are steeper (i.e. do not have longer wavelengths) is now recognized. The navy has not had to make any fundamental changes in ship design as a consequence of new knowledge of waves greater than 21.4 m (70 ft) because they build to higher standards.[38]

A characteristic of the shipping industry is that there are no uniform codes or international standards. There are more than 50 classification societies worldwide, each has different rules. Ship design has historically largely been led by the ship insurers who inspected, classified and insured vessels. Hence the widespread adoption of new rules to allow for the existence of rogue waves is likely to take many years.[38]

See also


  1. A failure load pressure of 201 kN/m2 is the same as 20,500 kgf/m2 or 20.5 Mt/m2 (metric tonnes per square metre).
  2. Note that the term super rogue wave had not yet been coined by ANU researchers at that time.
  3. A design load pressure (of the hatches) of 17.1 kN/m2 is the same as 1,744 kgf/m2 or 1.7 Mt/m2 (metric tonnes per square metre).
  4. A hydrostatic pressure of 5,650 kN/m2 is the same as 576,100 kgf/m2 or 576.1 Mt/m2 (metric tonnes per square metre).
  5. Note that MT/m refers to metric tonnes per square metre.
  6. Smith has presented calculations for a hypothetical bulk carrier with a length of 275m and a displacement of 161,000 metric tonnes, the design Hydrostatic pressure, 8.75 m below waterline is 88 kN/m2 or 88 kPa or 8.9 MT/m2 (metric tonnes per square metre). For the same carrier the design Hydrodynamic pressure is 122 kN/m2 or 122 kPa or 12,440 kgf/m2 (kilograms of force per square metre) or 12.44 Mt/m2 (metric tonnes per square metre).


  1. Haver, Sverre (2003). Freak wave event at Draupner jacket January 1 1995 (PDF) (Report). Statoil, Tech. Rep. PTT-KU-MA. Retrieved 2015-06-03.
  2. "Rogue Waves – Monsters of the deep: Huge, freak waves may not be as rare as once thought". Economist Magazine. September 17, 2009. Retrieved 2009-10-04.
  3. "Freak waves" (PDF). Archived from the original (PDF) on 2008-04-14. (1.07 MiB), Beacon #185, Skuld, June 2005
  4. Predictability of Rogue Events, Simon Birkholz, Carsten Brée, Ayhan Demircan, and Günter Steinmeyer, Physical Review Letters 114, 213901, 28 May 2015
  5. "Rogue Waves: The Fourteenth 'Aha Huliko'A Hawaiian Winter Workshop" (PDF). Oceanography. 3 September 2005. pp. 66–70. Retrieved April 16, 2016.
  6. "Freak waves spotted from space". BBC News. July 22, 2004. Retrieved May 22, 2010.
  7. Benetazzo, Alvise; Barbariol, Francesco; Bergamasco, Filippo; Torsello, Andrea; Carniel, Sandro; Sclavo, Mauro (2015-06-22). "Observation of Extreme Sea Waves in a Space–Time Ensemble". Journal of Physical Oceanography. 45 (9): 2261–2275. Bibcode:2015JPO....45.2261B. doi:10.1175/JPO-D-15-0017.1. ISSN 0022-3670.
  8. "Task Report – NOAA Great Lakes Environmental Research Laboratory – Ann Arbor, MI, USA". Retrieved April 16, 2016.
  9. Holliday, Naomi P. (March 2006). "Were extreme waves in the Rockall Trough the largest ever recorded?". Geophysical Research Letters. 33 (5): L05613. Bibcode:2006GeoRL..33.5613H. doi:10.1029/2005GL025238.
  10. Laird, Anne Marie (December 2006). "Observed Statistics of Extreme Waves". Doctoral Dissertation, Monterey, California Naval Postgraduate School: 2.
  11. "Physics of Tsunamis". United States Department of Commerce. 27 January 2016. Retrieved 29 January 2016. They cannot be felt aboard ships, nor can they be seen from the air in the open ocean.
  12. "Freak Wave – programme summary". BBC. 14 November 2002. Retrieved 15 January 2016.
  13. Faulkner, Douglas (1998). An Independent Assessment of the Sinking of the M.V. Derbyshire. SNAME Transactions, Royal Institution of Naval Architects. pp. 59–103. Archived from the original on 2016-04-18. The author's starting point therefore was to look for an extraordinary cause. He reasoned that nothing could be more extraordinary than the violence of a fully arisen and chaotic storm tossed sea. He therefore studied the meteorology of revolving tropical storms and freak waves and found that steep elevated waves of 25 m to 30 m or more were quite likely to have occurred during typhoon Orchid.
  14. Faulkner, Douglas (2000). Rogue Waves – Defining Their Characteristics for Marine Design (PDF). Rogue Waves 2000 Workshop. Brest: French Research Institute for Exploitation of the Sea. p. 16. Retrieved 15 January 2016. This paper introduces the need for a paradigm shift in thinking for the design of ships and offshore installations to include a Survival Design approach additional to current design requirements.
  15. Royal Commission on the Ocean Ranger Marine Disaster (Canada) (1985). Safety offshore Eastern Canada, summary of studies & seminars. The Commission.
  16. Liu, Paul C. (2007). "A Chronology of Freaque Wave Encounters" (PDF). Geofizika. 24 (1): 57–70. Retrieved October 8, 2012.
  17. Bruce Parker (13 March 2012). The Power of the Sea: Tsunamis, Storm Surges, Rogue Waves, and Our Quest to Predict Disasters. St. Martin's Press. ISBN 978-0-230-11224-7.
  18. Ian Jones; Joyce Jones (2008). Oceanography in the Days of Sail (PDF). Hale & Iremonger. p. 115. ISBN 978-0-9807445-1-4. Archived from the original (PDF) on 2016-03-02. Retrieved 2016-01-15. Dumont d'Urville, in his narrative, expressed the opinion that the waves reached a height of 'at least 80 to 100 feet'. In an era when opinions were being expressed that no wave would exceed 30 feet, Dumont d'Urville's estimations were received, it seemed, with some scepticism. No one was more outspoken in his rejection than François Arago, who, calling for a more scientific approach to the estimation of wave height in his instructions for the physical research on the voyage of the Bonité, suggested that imagination played a part in estimations as high as '33 metres' (108 feet). Later, in his 1841 report on the results of the Vénus expedition, Arago made further reference to the 'truly prodigious waves with which the lively imagination of certain navigators delights in covering the seas'
  19. ""The Wave": The growing danger of monster waves". 26 September 2010. Retrieved 26 March 2018.
  20. Carlos Guedes Soares; T.A. Santos (3 October 2014). Maritime Technology and Engineering. CRC Press. ISBN 978-1-315-73159-9.
  21. "US Army Engineer Waterways Experimental Station: Coastal Engineering Technical Note CETN I-60" (PDF). March 1995. Archived from the original (PDF) on February 21, 2013. Retrieved April 16, 2016.
  22. Draper, Laurence (July 1964). ""Freak" Ocean Waves" (PDF). Oceanus. 10 (4): 12–15.
  23. Hugo Montgomery-Swan (2010). Heavy Weather Powerboating. Adlard Coles Nautical. p. 33. ISBN 9780713688719.
  24. Michel Olagnon, Marc Prevosto (20 October 2004). Rogue Waves 2004: Proceedings of a Workshop Organized by Ifremer and Held in Brest, France, 20-21-22 October 2004, Within the Brest Sea Tech Week 2004. pp. VIII. ISBN 9782844331502.
  25. Draper, Laurence (July 1971). "Severe Wave Conditions at Sea" (PDF). Journal of the Institute of Navigation. 24 (3): 274–277. doi:10.1017/s0373463300048244.
  26. Robert Gordon Pirie (1996). Oceanography: Contemporary Readings in Ocean Sciences. Oxford University Press. ISBN 978-0-19-508768-0.
  27. M. Grant Gross (1 March 1996). Oceanography. Prentice Hall. ISBN 978-0-13-237454-5.
  28. "The last word: Terrors of the sea". 27 September 2010. Retrieved 15 January 2016.
  29. "Factpages, Norwegian Petroleum Directorate". Norwegian Petroleum Directorate. Retrieved 12 September 2016.
  30. Bjarne Røsjø, Kjell Hauge (2011-11-08). "Proof: Monster Waves are real". ScienceNordic. "Draupner E had only been operating in the North Sea for around half a year, when a huge wave struck the platform like a hammer. When we first saw the data, we were convinced it had to be a technological error," says Per Sparrevik. He is the head of the underwater technology, instrumentation and monitoring at the Norwegian NGI ... but the data were not wrong. When NGI looked over the measurements and calculated the effect of the wave that had hit the platform, the conclusion was clear: The wave that struck the unmanned platform Draupner E on 1 January 1995 was indeed extreme.
  31. Skourup, J; Hansen, N.-E. O.; Andreasen, K. K. (1997-08-01). "Non-Gaussian Extreme Waves in the Central North Sea". Journal of Offshore Mechanics and Arctic Engineering. 119 (3): 146. doi:10.1115/1.2829061. The area of the Central North Sea is notorious for the occurrence of very high waves in certain wave trains. The short-term distribution of these wave trains includes waves which are far steeper than predicted by the Rayleigh distribution. Such waves are often termed "extreme waves" or "freak waves". An analysis of the extreme statistical properties of these waves has been made. The analysis is based on more than 12 years of wave records from the Mærsk Olie og Gas AS operated Gorm Field, which is located in the Danish sector of the Central North Sea. From the wave recordings more than 400 freak wave candidates were found. The ratio between the extreme crest height and the significant wave height (20-min value) has been found to be about 1.8, and the ratio between extreme crest height and extreme wave height has been found to be 0.69. The latter ratio is clearly outside the range of Gaussian waves, and it is higher than the maximum value for steep nonlinear long-crested waves, thus indicating that freak waves are not of a permanent form, and probably of short-crested nature. The extreme statistical distribution is represented by a Weibull distribution with an upper bound, where the upper bound is the value for a depth-limited breaking wave. Based on the measured data, a procedure for determining the freak wave crest height with a given return period is proposed. A sensitivity analysis of the extreme value of the crest height is also made.
  32. Haver S and Andersen O J (2010). Freak waves: rare realizations of a typical population or typical realizations of a rare population? (PDF). Proc. 10th Conf. of Int. Society for Offshore and Polar Engineering (ISOPE). Seattle: ISOPE. pp. 123–130. Archived from the original (PDF) on 2016-05-12. Retrieved 18 April 2016.
  33. Rogue Waves 2000. Ifremer and IRCN organised a workshop on "Rogue waves", 29–30 November 2000, during SeaTechWeek 2000, Le Quartz, Brest, France. Brest: iFremer. 2000. Retrieved 18 April 2016.
  34. Susan Casey (2010). The Wave: In the Pursuit of the Rogues, Freaks and Giants of the Ocean. Doubleday Canada. ISBN 978-0-385-66667-1.
  35. Holliday, N.P.; Yelland, M.Y.; Pascal, R.; Swail, V.; Taylor, P.K.; Griffiths, C.R.; Kent, E.C. (2006). "Were extreme waves in the Rockall Trough the largest ever recorded?". Geophysical Research Letters. 33 (5): L05613. Bibcode:2006GeoRL..33.5613H. doi:10.1029/2005gl025238. In February 2000 those onboard a British oceanographic research vessel near Rockall, west of Scotland experienced the largest waves ever recorded by scientific instruments in the open ocean. Under severe gale force conditions with wind speeds averaging 21 ms1 a shipborne wave recorder measured individual waves up to 29.1 m from crest to trough, and a maximum significant wave height of 18.5 m. The fully formed sea developed in unusual conditions as westerly winds blew across the North Atlantic for two days, during which time a frontal system propagated at a speed close to the group velocity of the peak waves. The measurements are compared to a wave hindcast that successfully simulated the arrival of the wave group, but underestimated the most extreme waves.
  36. "Critical review on potential use of satellite date to find rogue waves" (PDF). European Space Agency SEASAR 2006 proceedings. April 2006. Retrieved February 23, 2008.
  37. "Observing the Earth: Ship-Sinking Monster Waves revealed by ESA Satellites". ESA. 21 July 2004. Retrieved 14 January 2016.
  38. Smith, Craig (2007). Extreme Waves and Ship Design (PDF). 10th International Symposium on Practical Design of Ships and Other Floating Structures. Houston: American Bureau of Shipping. p. 8. Retrieved 13 January 2016. Recent research has demonstrated that extreme waves, waves with crest to trough heights of 20 to 30 meters, occur more frequently than previously thought.
  39. John H. Steele; Steve A. Thorpe; Karl K. Turekian (26 August 2009). Elements of Physical Oceanography: A derivative of the Encyclopedia of Ocean Sciences. Academic Press. ISBN 978-0-12-375721-0.
  40. "Rogue wave theory to save ships". 29 July 2015. Retrieved April 16, 2016.
  41. Janssen, T. T.; Herbers, T. H. C. (2009). "Nonlinear Wave Statistics in a Focal Zone". Journal of Physical Oceanography. 39 (8): 1948–1964. Bibcode:2009JPO....39.1948J. doi:10.1175/2009jpo4124.1. ISSN 0022-3670.
  42. Wolff, Julius F. (1979). "Lake Superior Shipwrecks", p. 28. Lake Superior Marine Museum Association, Inc., Duluth, Minnesota, USA. ISBN 0-932212-18-8.
  43. "Optical sciences group – Theoretical Physics – ANU". Https. Retrieved April 16, 2016.
  44. Dysthe, K; Krogstad, H; Müller, P (2008). "Annual Review of Fluid Mechanics": 287–310. Cite journal requires |journal= (help)
  45. Kharif, C; Pelinovsky, E (2003). "Physical mechanisms of the rogue wave phenomenon". European Journal of Mechanics B. 22 (6): 603–634. Bibcode:2003EJMF...22..603K. CiteSeerX doi:10.1016/j.euromechflu.2003.09.002.
  46. Onorato, M; Residori, S; Bortolozzo, U; Montina, A; Arecchi, F (10 July 2013). "Rogue waves and their generating mechanisms in different physical contexts". Physics Reports. 528 (2): 47–89. Bibcode:2013PhR...528...47O. doi:10.1016/j.physrep.2013.03.001.
  47. Slunyaev, A; Didenkulova, I; Pelinovsky, E (November 2011). "Rogue waters". Contemporary Physics. 52 (6): 571–590. arXiv:1107.5818. Bibcode:2011ConPh..52..571S. doi:10.1080/00107514.2011.613256. Retrieved 16 April 2016.
  48. Chabchoub, A; Hoffmann, N.P.; Akhmediev, N (1 February 2012). "Observation of rogue wave holes in a water wave tank". Journal of Geophysical Research: Oceans. 117 (C11): C00J02. Bibcode:2012JGRC..117.0J02C. doi:10.1029/2011JC007636.
  49. [ Laboratory recreation of the Draupner wave and the role of breaking in crossing seas - McAllister et al - Journal of Fluid Mechanics, 2019, vol. 860, pp. 767-786, pub. Cambridge University Press, DOI 10.1017/jfm.2018.886
  51. "Freak waves spotted from space". BBC News Online. 22 July 2004. Retrieved May 8, 2006.
  52. "Lego pirate proves, survives, super rogue wave". Retrieved April 15, 2016.
  53. "Maritime security". Retrieved April 15, 2016.
  54. "Lego Pirate Proves, Survives, Super Rogue Wave". 2012-04-11. Retrieved April 15, 2016.
  55. Broad, William J. (July 11, 2006). "Rogue Giants at Sea". The New York Times. Retrieved April 15, 2016.
  56. "Scientists Model Rogue Waves". Retrieved April 15, 2016.
  57. "Mapping a strategy for rogue monsters of the seas". Archived from the original on April 24, 2016. Retrieved April 15, 2016.
  58. Katherine Noyes (25 February 2016). "A new algorithm from MIT could protect ships from 'rogue waves' at sea". Retrieved April 8, 2016.
  59. Will Cousins and Themistoklis P. Sapsis (5 January 2016). "Reduced-order precursors of rare events in unidirectional nonlinear water waves" (PDF). Journal of Fluid Mechanics. 790: 368–388. Bibcode:2016JFM...790..368C. doi:10.1017/jfm.2016.13. hdl:1721.1/101436. Retrieved April 8, 2016.
  60. Stuart Thornton (3 December 2012). "Rogue Waves – National Geographic Society". Retrieved April 16, 2016.
  61. "Introduction – Nobuhito Mori". Retrieved April 15, 2016.
  62. "Freak wave probability higher than thought ' News in Science (ABC Science)". 2011-10-05. Retrieved April 15, 2016.
  63. "'Freak' ocean waves hit without warning, new research shows – ScienceDaily". Https. Retrieved April 15, 2016.
  64. Thomas A A Adcock and Paul H Taylor (14 October 2014). "The physics of anomalous ('rogue') ocean waves". Reports on Progress in Physics. 77 (10): 105901. Bibcode:2014RPPh...77j5901A. doi:10.1088/0034-4885/77/10/105901. PMID 25313170.
  65. Mike McRae (January 23, 2019). "Scientists Recreated a Devastating 'Freak Wave' in The Lab, And It's Weirdly Familiar". Retrieved January 25, 2019.
  66. Stephen Ornes (11 Aug 2014). "Monster waves blamed for shipping disasters". Retrieved April 16, 2016.
  67. "European Commission : CORDIS : Projects & Results Service : Periodic Report Summary – EXTREME SEAS (Design for ship safety in extreme seas)". Retrieved April 16, 2016.
  68. P. K. Shukla, I. Kourakis, B. Eliasson, M. Marklund and L. Stenflo: "Instability and Evolution of Nonlinearly Interacting Water Waves" nlin.CD/0608012, Physical Review Letters (2006)
  69. "Mechanics – Department of Mathematics". University of Oslo, The Faculty of Mathematics and Natural Sciences. 27 January 2016. Retrieved April 17, 2016.
  70. Alex, Cattrell (2018). "Can Rogue Waves Be Predicted Using Characteristic Wave Parameters?" (PDF). Journal of Geophysical Research: Oceans. 123 (8): 5624–5636. Bibcode:2018JGRC..123.5624C. doi:10.1029/2018JC013958.
  71. Barnett, T. P.; Kenyon, K. E. (1975). "Recent advances in the study of wind waves". Reports on Progress in Physics. 38 (6): 667. Bibcode:1975RPPh...38..667B. doi:10.1088/0034-4885/38/6/001. ISSN 0034-4885.
  72. "The RITMARE flagship project". Retrieved October 11, 2017.
  73. "Rogue Waves". Ocean Prediction Center. National Weather Service. April 22, 2005. Retrieved May 8, 2006.
  74. Adrian Cho (13 May 2011). "Ship in Bottle, Meet Rogue Wave in Tub". Science Now. 332 (6031): 774. doi:10.1126/science.332.6031.774-b. Retrieved 2011-06-27.
  75. "Math explains water disasters – ScienceAlert". 26 August 2010. Retrieved April 15, 2016.
  76. "Bristol University". 22 August 2010. Retrieved April 15, 2016.
  77. Akhmediev, N.; Soto-Crespo, J. M.; Ankiewicz, A. (2009). "How to excite a rogue wave". Physical Review A. 80 (4): 043818. Bibcode:2009PhRvA..80d3818A. doi:10.1103/PhysRevA.80.043818. hdl:10261/59738.
  78. Fedele, Francesco; Brennan, Joseph; Ponce de León, Sonia; Dudley, John; Dias, Frédéric (2016-06-21). "Real world ocean rogue waves explained without the modulational instability". Scientific Reports. 6: 27715. Bibcode:2016NatSR...627715F. doi:10.1038/srep27715. ISSN 2045-2322. PMC 4914928. PMID 27323897.
  79. Phillips 1957, Journal of Fluid Mechanics
  80. Miles, 1957, Journal of Fluid Mechanics
  81. Frederic-Moreau. The Glorious Three, translated by M. Olagnon and G.A. Chase / Rogue Waves-2004, Brest, France
  82. Endeavour or Caledonian Star report, March 2, 2001, 53°03′S 63°35′W
  83. MS Bremen report, February 22, 2001, 45°54′S 38°58′W
  84. R. Colin Johnson (December 24, 2007). "EEs Working With Optical Fibers Demystify 'Rogue Wave' Phenomenon". Electronic Engineering Times (1507): 14, 16.
  85. Kibler, B.; Fatome, J.; Finot, C.; Millot, G.; Dias, F.; Genty, G.; Akhmediev, N.; Dudley, J.M. (2010). "The Peregrine soliton in nonlinear fibre optics". Nature Physics. 6 (10): 790–795. Bibcode:2010NatPh...6..790K. CiteSeerX doi:10.1038/nphys1740.
  86. "Peregrine's 'Soliton' observed at last". Retrieved 2010-08-24.
  87. "Eagle Island Lighthouse". Commissioners of Irish Lights. Retrieved 28 October 2010.
  88. Haswell-Smith, Hamish (2004). The Scottish Islands. Edinburgh: Canongate. pp. 329–31. ISBN 978-1-84195-454-7.
  89. Munro, R.W. (1979) Scottish Lighthouses. Stornoway. Thule Press. ISBN 0-906191-32-7. Munro (1979) pages 170–1
  90. The New York Times, September 26, 1901, p. 16
  91. Freaquewaves (17 December 2009). "Freaque Waves: The encounter of RMS Lusitania". Retrieved 26 March 2018.
  92. "Archived copy" (PDF). Archived from the original (PDF) on 2009-01-06. Retrieved 2010-01-10.CS1 maint: archived copy as title (link), Müller, et al., "Rogue Waves," 2005
  93. Kerbrech, Richard De (2009). Ships of the White Star Line. Ian Allan Publishing. p. 190. ISBN 978-0-7110-3366-5.
  94. Rogue Giants at Sea, Broad, William J, New York Times, July 11, 2006
  95. "Ship-sinking monster waves revealed by ESA satellites", ESA News, July 21, 2004, accessed June 18, 2010
  96. Kastner, Jeffrey. "Sea Monsters". Cabinet Magazine. Retrieved 10 October 2017.
  97. "The Story of the Fastnet – The Economist Magazine December 18th 2008"
  98. Faulkner, Douglas. "An Independent Assessment of the Sinking of the MV DERBYSHIRE" (PDF). Royal Institution of Naval Architects. Retrieved 10 October 2017.
  99. esa. "Ship-sinking monster waves revealed by ESA satellites". Retrieved 26 March 2018.
  100. Hurricane Ivan prompts rogue wave rethink, The Register, 5 August 2005
  101. "NRL Measures Record Wave During Hurricane Ivan - U.S. Naval Research Laboratory". 2017-02-17. Retrieved 26 March 2018.
  102. Reuters (April 18, 2005). Freak wave pummels cruise ship.
  103. "NTSB – Brief MAB-05/03". Archived from the original on 2009-03-08. Retrieved 2009-03-08.
  104. Deadliest Catch Season 2, Episode 4 "Finish Line" Original airdate: April 28, 2006; approx time into episode: 0:40:00–0:42:00. Edited footage viewable online at Archived 2009-08-06 at the Wayback Machine
  105. "Monster waves threaten rescue helicopters" (PDF). (35.7 KiB), U.S. Naval Institute, December 15, 2006
  106. "Olas de récord en Cantabria". El Diario Montañés. 3 February 2009.
  107. "Dos muertos y 16 heridos por una ola gigante en un crucero con destino a Cartagena". La Vanguardia. 3 March 2010.
  108. "Giant rogue wave slams into ship off French coast, killing 2". FoxNews. 3 March 2010. Archived from the original on 2010-03-06. Retrieved 2010-03-04.
  109. "Sea Shepherd Vessel Suffers Serious Damage From Rouge Wave". ecorazzi. 28 December 2011.
  110. "Nuevo récord de altura de ola máxima registrada en España". Puertos del Estado. 21 October 2014.
  111. Jivanda, Tomas (15 February 2014). "UK weather: Man killed after huge wave breaks window of cruise ship Marco Polo in English Channel as storms set to continue". The Independent. Retrieved 17 February 2014.
  112. Matthew Cappucci (September 9, 2019). "Hurricane Dorian probably whipped up a 100-foot rogue wave near Newfoundland". The Washington Post. Retrieved September 10, 2019.
  113. Keith McCloskey (15 July 2014). The Lighthouse: The Mystery of the Eilean Mor Lighthouse Keepers. History Press Limited. ISBN 978-0-7509-5741-0.
  114. Brown, David (1998). "The Loss of the 'DERBYSHIRE'" (Technical Report). Crown.
  115. "Ships and Seafarers (Safety)". Parliamentary Debates (Hansard). House of Commons. 25 June 2002. col. 193WH–215WH. The MV Derbyshire was registered at Liverpool and, at the time, was the largest ship ever built: it was twice the size of the Titanic.
  116. Lerner, S.; Yoerger, D.; Crook, T. (May 1999). "Navigation for the Derbyshire Phase2 Survey" (Technical Report). Woods Hole Oceanographic Institution MA. p. 28. WHOI-99-11. In 1997, the Deep Submergence Operations Group of the Woods Hole Oceanographic Institution conducted an underwater forensic survey of the UK bulk carrier MV Derbyshire with a suite of underwater vehicles. This report describes the navigation systems and methodologies used to precisely position the vessel and vehicles. Precise navigation permits the survey team to control the path of the subsea vehicle in order to execute the survey plan, provides the ability to return to specific targets, and allows the assessment team to correlate observations made at different times from different vehicles. In this report, we summarize the techniques used to locate Argo as well as the repeatability of those navigation fixes. To determine repeatability, we selected a number of instances where the vehicle lines crossed. By registering two images from overlapping areas on different tracklines, we can determine the true position offset. By comparing the position offset derived from the images to the offsets obtained from navigation, we can determine the navigation error. The average error for 123 points across a single tie line was 3.1 meters, the average error for a more scattered selection of 18 points was 1.9 meters.
  117. "Inside the Lethal World of Bulk Carriers: Death Trips on the Seven Seas" (PDF). Retrieved April 17, 2016.
  118. "Improving the safety of bulk carriers" (PDF). IMO. Archived from the original (PDF) on 2009-07-07. Retrieved 2009-08-11.
  119. Smith, Craig (2006). Extreme Waves. Joseph Henry Press. ISBN 9780309100625. There is sufficient evidence to conclude that 66-foot high waves can be experienced in the 25-year lifetime of oceangoing vessels, and that 98-foot high waves are less likely, but not out of the question. Therefore a design criterion based on 36-foot high waves seems inadequate when the risk of losing creq and cargo is considered.
  120. Rosenthal, W (2005). "Results of the MAXWAVE project" (PDF). Retrieved 14 January 2016. The Norwegian offshore standards take into account extreme severe wave conditions by requiring that a 10,000-year wave does not endanger the structure’s integrity (Accidental Limit State, ALS).
  121. "Rules for Classification and Construction" (PDF). Hamburg, Germany: Germanischer Lloyd SE. 2011. Archived from the original (PDF) on 2014-09-12. Retrieved 13 January 2016. General Terms and Conditions of the respective latest edition will be applicable. See Rules for Classification and Construction, I – Ship Technology, Part 0 – Classification and Surveys.

Further reading

Extreme seas project

MaxWave report and WaveAtlas


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