# Astronomy:Lightning

Short description: Weather phenomenon involving electrostatic discharge
Strokes of cloud-to-ground lightning during a thunderstorm in the town of Oradea.

Lightning is a naturally occurring electrostatic discharge during which two electrically charged regions, both in the atmosphere or with one on the ground, temporarily neutralize themselves, causing the instantaneous release of an average of one gigajoule of energy.[1][2][3] This discharge may produce a wide range of electromagnetic radiation, from heat created by the rapid movement of electrons, to brilliant flashes of visible light in the form of black-body radiation. Lightning causes thunder, a sound from the shock wave which develops as gases in the vicinity of the discharge experience a sudden increase in pressure. Lightning occurs commonly during thunderstorms as well as other types of energetic weather systems, but volcanic lightning can also occur during volcanic eruptions.

The three main kinds of lightning are distinguished by where they occur: either inside a single thundercloud, between two different clouds, or between a cloud and the ground. Many other observational variants are recognized, including "heat lightning", which can be seen from a great distance but not heard; dry lightning, which can cause forest fires; and ball lightning, which is rarely observed scientifically.

Humans have deified lightning for millennia. Idiomatic expressions derived from lightning, such as the English expression "bolt from the blue", are common across languages. At all times people have been fascinated by the sight and difference of lightning. The fear of lightning is called astraphobia.

The first known photograph of lightning is from 1847, by Thomas Martin Easterly. The first surviving photograph is from 1882, by William Nicholson Jennings,[4] a photographer who spent half his life capturing pictures of lightning and proving its diversity.

## Electrification

(Figure 1) The main charging area in a thunderstorm occurs in the central part of the storm where the air is moving upward rapidly (updraft) and temperatures range from −15 to −25 °C (5 to −13 °F).

The details of the charging process are still being studied by scientists, but there is general agreement on some of the basic concepts of thunderstorm electrification. Electrification can be by the triboelectric effect as a result of ion transfer between colliding bodies. Uncharged, colliding water-drops can become charged because of charge transfer between them (as aqueous ions) in an electric field as would exist in a thunder cloud.[5] The main charging area in a thunderstorm occurs in the central part of the storm where air is moving upward rapidly (updraft) and temperatures range from −15 to −25 °C (5 to −13 °F); see Figure 1. In that area, the combination of temperature and rapid upward air movement produces a mixture of super-cooled cloud droplets (small water droplets below freezing), small ice crystals, and graupel (soft hail). The updraft carries the super-cooled cloud droplets and very small ice crystals upward. At the same time, the graupel, which is considerably larger and denser, tends to fall or be suspended in the rising air.[6]

(Figure 2) When the rising ice crystals collide with graupel, the ice crystals become positively charged and the graupel becomes negatively charged.

The differences in the movement of the precipitation cause collisions to occur. When the rising ice crystals collide with graupel, the ice crystals become positively charged and the graupel becomes negatively charged; see Figure 2. The updraft carries the positively charged ice crystals upward toward the top of the storm cloud. The larger and denser graupel is either suspended in the middle of the thunderstorm cloud or falls toward the lower part of the storm.[6]

The upper part of the thunderstorm cloud becomes positively charged while the middle to the lower part of the thunderstorm cloud becomes negatively charged.

The result is that the upper part of the thunderstorm cloud becomes positively charged while the middle to lower part of the thunderstorm cloud becomes negatively charged.[6]

The upward motions within the storm and winds at higher levels in the atmosphere tend to cause the small ice crystals (and positive charge) in the upper part of the thunderstorm cloud to spread out horizontally some distance from the thunderstorm cloud base. This part of the thunderstorm cloud is called the anvil. While this is the main charging process for the thunderstorm cloud, some of these charges can be redistributed by air movements within the storm (updrafts and downdrafts). In addition, there is a small but important positive charge buildup near the bottom of the thunderstorm cloud due to the precipitation and warmer temperatures.[6]

The induced separation of charge in pure liquid water has been known since the 1840s as has the electrification of pure liquid water by the tribo-electric effect.[7]

William Thomson (Lord Kelvin) demonstrated that charge separation in water occurs in the usual electric fields at the earth's surface and developed a continuous electric field measuring device using that knowledge.[8]

The physical separation of charge into different regions using liquid water was demonstrated by Kelvin with the Kelvin water dropper. The most likely charge-carrying species were considered to be the aqueous hydrogen ion and the aqueous hydroxide ion.[9]

The electrical charging of solid water ice has also been considered. The charged species were again considered to be the hydrogen ion and the hydroxide ion.[10][11]

An electron is not stable in liquid water with respect to a hydroxide ion plus dissolved hydrogen for the time scales involved in thunder storms.[12]

The charge carrier in lightning is mainly electrons in a plasma.[13] The process of going from charge as ions (positive hydrogen ion and negative hydroxide ion) associated with liquid water or solid water to charge as electrons associated with lightning must involve some form of electro-chemistry, that is, the oxidation and/or the reduction of chemical species.[14] As hydroxide functions as a base and carbon dioxide is an acidic gas, it is possible that charged water clouds in which the negative charge is in the form of the aqueous hydroxide ion, interact with atmospheric carbon dioxide to form aqueous carbonate ions and aqueous hydrogen carbonate ions.

## General considerations

The typical cloud-to-ground lightning flash culminates in the formation of an electrically conducting plasma channel through the air in excess of 5 km (3.1 mi) tall, from within the cloud to the ground's surface. The actual discharge is the final stage of a very complex process.[15] At its peak, a typical thunderstorm produces three or more strikes to the Earth per minute.[16] Lightning primarily occurs when warm air is mixed with colder air masses,[17] resulting in atmospheric disturbances necessary for polarizing the atmosphere. However, it can also occur during dust storms, forest fires, tornadoes, volcanic eruptions, and even in the cold of winter, where the lightning is known as thundersnow.[18][19] Hurricanes typically generate some lightning, mainly in the rainbands as much as 160 km (99 mi) from the center.[20][21][22]

## Distribution, frequency and extent

Main page: Physics:Distribution of lightning
World map showing the frequency of lightning strikes, in flashes per km² per year (equal-area projection), from combined 1995–2003 data from the Optical Transient Detector and 1998–2003 data from the Lightning Imaging Sensor.

Lightning is not distributed evenly around Earth, as shown in the map.

On Earth, the lightning frequency is approximately 44 (± 5) times per second, or nearly 1.4 billion flashes per year[23] and the average duration is 0.2 seconds made up from a number of much shorter flashes (strokes) of around 60 to 70 microseconds.[24]

Many factors affect the frequency, distribution, strength and physical properties of a typical lightning flash in a particular region of the world. These factors include ground elevation, latitude, prevailing wind currents, relative humidity, and proximity to warm and cold bodies of water. To a certain degree, the proportions of intra-cloud, cloud-to-cloud, and cloud-to-ground lightning may also vary by season in middle latitudes.

Because human beings are terrestrial and most of their possessions are on the Earth where lightning can damage or destroy them, cloud-to-ground (CG) lightning is the most studied and best understood of the three types, even though in-cloud (IC) and cloud-to-cloud (CC) are more common types of lightning. Lightning's relative unpredictability limits a complete explanation of how or why it occurs, even after hundreds of years of scientific investigation. About 70% of lightning occurs over land in the tropics[25] where atmospheric convection is the greatest.

This occurs from both the mixture of warmer and colder air masses, as well as differences in moisture concentrations, and it generally happens at the boundaries between them. The flow of warm ocean currents past drier land masses, such as the Gulf Stream, partially explains the elevated frequency of lightning in the Southeast United States. Because large bodies of water lack the topographic variation that would result in atmospheric mixing, lightning is notably less frequent over the world's oceans than over land. The North and South Poles are limited in their coverage of thunderstorms and therefore result in areas with the least lightning.[clarification needed]

In general, CG lightning flashes account for only 25% of all total lightning flashes worldwide. Since the base of a thunderstorm is usually negatively charged, this is where most CG lightning originates. This region is typically at the elevation where freezing occurs within the cloud. Freezing, combined with collisions between ice and water, appears to be a critical part of the initial charge development and separation process. During wind-driven collisions, ice crystals tend to develop a positive charge, while a heavier, slushy mixture of ice and water (called graupel) develops a negative charge. Updrafts within a storm cloud separate the lighter ice crystals from the heavier graupel, causing the top region of the cloud to accumulate a positive space charge while the lower level accumulates a negative space charge.

Lightning in Belfort, France

Because the concentrated charge within the cloud must exceed the insulating properties of air, and this increases proportionally to the distance between the cloud and the ground, the proportion of CG strikes (versus CC or IC discharges) becomes greater when the cloud is closer to the ground. In the tropics, where the freezing level is generally higher in the atmosphere, only 10% of lightning flashes are CG. At the latitude of Norway (around 60° North latitude), where the freezing elevation is lower, 50% of lightning is CG.[26][27]

Lightning is usually produced by cumulonimbus clouds, which have bases that are typically 1–2 km (0.62–1.24 mi) above the ground and tops up to 15 km (9.3 mi) in height.

The place on Earth where lightning occurs most often is near the small village of Kifuka in the mountains of the eastern Democratic Republic of the Congo,[28] where the elevation is around 975 m (3,200 ft). On average, this region receives 158 lightning strikes per square kilometre per year (410/sq mi/yr).[29] Lake Maracaibo in Venezuela averages 297 days per year with lightning activity, an effect recognized as Catatumbo lightning.[30] Other lightning hotspots include Singapore[31] and Lightning Alley in Central Florida.[32][33]

The 477 mile megaflash from Texas to Louisiana.[34]

According to the United Nations' WMO, on April 29, 2020, a bolt 768 km (477.2 mi) long was observed in the southern U.S.—sixty km (37 mi) longer than the previous distance record (southern Brazil, October 31, 2018).[35] A single flash in Uruguay and northern Argentina on June 18, 2020 lasted for 17.1 seconds—0.37 seconds longer than the previous record (March 4, 2019, also in northern Argentina).[35] The most people killed by a single direct strike of lightning occurred when 21 people died as they huddled for safety in a hut that was hit (1975, Zimbabwe).[35] In an indirect strike, 469 people died when lightning struck a set of oil tanks in 1994, causing burning oil to flood a town (1994, Dronka, Egypt).[35]

## Necessary conditions

Main page: Physics:Thunderstorm

File:Thunder.ogg In order for an electrostatic discharge to occur, two preconditions are necessary: first, a sufficiently high potential difference between two regions of space must exist, and second, a high-resistance medium must obstruct the free, unimpeded equalization of the opposite charges. The atmosphere provides the electrical insulation, or barrier, that prevents free equalization between charged regions of opposite polarity.

It is well understood that during a thunderstorm there is charge separation and aggregation in certain regions of the cloud; however, the exact processes by which this occurs are not fully understood.[36]

### Electrical field generation

View of lightning from an airplane flying above a system.

As a thundercloud moves over the surface of the Earth, an equal electric charge, but of opposite polarity, is induced on the Earth's surface underneath the cloud. The induced positive surface charge, when measured against a fixed point, will be small as the thundercloud approaches, increasing as the center of the storm arrives and dropping as the thundercloud passes. The referential value of the induced surface charge could be roughly represented as a bell curve.

The oppositely charged regions create an electric field within the air between them. This electric field varies in relation to the strength of the surface charge on the base of the thundercloud – the greater the accumulated charge, the higher the electrical field.

## Flashes and strikes

Certain prominent structures often attract frequent lightning strikes. The CN Tower in Toronto is struck many times every summer.

The best-studied and understood form of lightning is cloud to ground (CG) lightning. Although more common, intra-cloud (IC) and cloud-to-cloud (CC) flashes are very difficult to study given there are no "physical" points to monitor inside the clouds. Also, given the very low probability of lightning striking the same point repeatedly and consistently, scientific inquiry is difficult even in areas of high CG frequency.

A lightning strike from cloud to ground in the Mojave Desert, California
An intra-cloud flash. A lightning flash within the cloud illuminates the entire cloud.

A downward leader travels towards earth, branching as it goes.
Lightning strike caused by the connection of two leaders, positive shown in blue and negative in red

In a process not well understood, a bidirectional channel of ionized air, called a "leader", is initiated between oppositely-charged regions in a thundercloud. Leaders are electrically conductive channels of ionized gas that propagate through, or are otherwise attracted to, regions with a charge opposite of that of the leader tip. The negative end of the bidirectional leader fills a positive charge region, also called a well, inside the cloud while the positive end fills a negative charge well. Leaders often split, forming branches in a tree-like pattern.[37] In addition, negative and some positive leaders travel in a discontinuous fashion, in a process called "stepping". The resulting jerky movement of the leaders can be readily observed in slow-motion videos of lightning flashes.

It is possible for one end of the leader to fill the oppositely-charged well entirely while the other end is still active. When this happens, the leader end which filled the well may propagate outside of the thundercloud and result in either a cloud-to-air flash or a cloud-to-ground flash. In a typical cloud-to-ground flash, a bidirectional leader initiates between the main negative and lower positive charge regions in a thundercloud. The weaker positive charge region is filled quickly by the negative leader which then propagates toward the inductively-charged ground.

The positively and negatively charged leaders proceed in opposite directions, positive upwards within the cloud and negative towards the earth. Both ionic channels proceed, in their respective directions, in a number of successive spurts. Each leader "pools" ions at the leading tips, shooting out one or more new leaders, momentarily pooling again to concentrate charged ions, then shooting out another leader. The negative leader continues to propagate and split as it heads downward, often speeding up as it gets closer to the Earth's surface.

About 90% of ionic channel lengths between "pools" are approximately 45 m (148 ft) in length.[38] The establishment of the ionic channel takes a comparatively long amount of time (hundreds of milliseconds) in comparison to the resulting discharge, which occurs within a few dozen microseconds. The electric current needed to establish the channel, measured in the tens or hundreds of amperes, is dwarfed by subsequent currents during the actual discharge.

Initiation of the lightning leader is not well understood. The electric field strength within the thundercloud is not typically large enough to initiate this process by itself.[39] Many hypotheses have been proposed. One hypothesis postulates that showers of relativistic electrons are created by cosmic rays and are then accelerated to higher velocities via a process called runaway breakdown. As these relativistic electrons collide and ionize neutral air molecules, they initiate leader formation. Another hypothesis involves locally enhanced electric fields being formed near elongated water droplets or ice crystals.[40] Percolation theory, especially for the case of biased percolation,[41] [clarification needed] describes random connectivity phenomena, which produce an evolution of connected structures similar to that of lightning strikes. A streamer avalanche model[42] has recently been favored by observational data taken by LOFAR during storms.[43][44]

### Upward streamers

When a stepped leader approaches the ground, the presence of opposite charges on the ground enhances the strength of the electric field. The electric field is strongest on grounded objects whose tops are closest to the base of the thundercloud, such as trees and tall buildings. If the electric field is strong enough, a positively charged ionic channel, called a positive or upward streamer, can develop from these points. This was first theorized by Heinz Kasemir.[45][46][47]

As negatively charged leaders approach, increasing the localized electric field strength, grounded objects already experiencing corona discharge will exceed a threshold and form upward streamers.

### Attachment

Once a downward leader connects to an available upward leader, a process referred to as attachment, a low-resistance path is formed and discharge may occur. Photographs have been taken in which unattached streamers are clearly visible. The unattached downward leaders are also visible in branched lightning, none of which are connected to the earth, although it may appear they are. High-speed videos can show the attachment process in progress.[48]

### Discharge

#### Return stroke

High-speed photography showing different parts of a lightning flash during the discharge process as seen in Toulouse, France.

Once a conductive channel bridges the air gap between the negative charge excess in the cloud and the positive surface charge excess below, there is a large drop in resistance across the lightning channel. Electrons accelerate rapidly as a result in a zone beginning at the point of attachment, which expands across the entire leader network at up to one third of the speed of light.[49] This is the "return stroke" and it is the most luminous and noticeable part of the lightning discharge.

A large electric charge flows along the plasma channel, from the cloud to the ground, neutralising the positive ground charge as electrons flow away from the strike point to the surrounding area. This huge surge of current creates large radial voltage differences along the surface of the ground. Called step potentials, they are responsible for more injuries and deaths in groups of people or of other animals than the strike itself.[50] Electricity takes every path available to it.[51] Such step potentials will often flow through one leg and out another, electrocuting an unlucky human or animal standing near the point where the lightning strikes.

The electric current of the return stroke averages 30 kiloamperes for a typical negative CG flash, often referred to as "negative CG" lightning. In some cases, a ground-to-cloud (GC) lightning flash may originate from a positively charged region on the ground below a storm. These discharges normally originate from the tops of very tall structures, such as communications antennas. The rate at which the return stroke current travels has been found to be around 100,000 km/s (one-third of the speed of light).[52]

The massive flow of electric current occurring during the return stroke combined with the rate at which it occurs (measured in microseconds) rapidly superheats the completed leader channel, forming a highly electrically conductive plasma channel. The core temperature of the plasma during the return stroke may exceed 50,000 K, causing it to radiate with a brilliant, blue-white color. Once the electric current stops flowing, the channel cools and dissipates over tens or hundreds of milliseconds, often disappearing as fragmented patches of glowing gas. The nearly instantaneous heating during the return stroke causes the air to expand explosively, producing a powerful shock wave which is heard as thunder.

#### Re-strike

High-speed videos (examined frame-by-frame) show that most negative CG lightning flashes are made up of 3 or 4 individual strokes, though there may be as many as 30.[53]

Each re-strike is separated by a relatively large amount of time, typically 40 to 50 milliseconds, as other charged regions in the cloud are discharged in subsequent strokes. Re-strikes often cause a noticeable "strobe light" effect.[54]

Each successive stroke is preceded by intermediate dart leader strokes that have a faster rise time but lower amplitude than the initial return stroke. Each subsequent stroke usually re-uses the discharge channel taken by the previous one, but the channel may be offset from its previous position as wind displaces the hot channel.[56]

Since recoil and dart leader processes do not occur on negative leaders, subsequent return strokes very seldom utilize the same channel on positive ground flashes which are explained later in the article.[55]

#### Transient currents during flash

The electric current within a typical negative CG lightning discharge rises very quickly to its peak value in 1–10 microseconds, then decays more slowly over 50–200 microseconds. The transient nature of the current within a lightning flash results in several phenomena that need to be addressed in the effective protection of ground-based structures. Rapidly changing currents tend to travel on the surface of a conductor, in what is called the skin effect, unlike direct currents, which "flow-through" the entire conductor like water through a hose. Hence, conductors used in the protection of facilities tend to be multi-stranded, with small wires woven together. This increases the total bundle surface area in inverse proportion to the individual strand radius, for a fixed total cross-sectional area.

The rapidly changing currents also create electromagnetic pulses (EMPs) that radiate outward from the ionic channel. This is a characteristic of all electrical discharges. The radiated pulses rapidly weaken as their distance from the origin increases. However, if they pass over conductive elements such as power lines, communication lines, or metallic pipes, they may induce a current which travels outward to its termination. The surge current is inversely related to the surge impedance: the higher in impedance, the lower the current.[57] This is the surge that, more often than not, results in the destruction of delicate electronics, electrical appliances, or electric motors. Devices known as surge protectors (SPD) or transient voltage surge suppressors (TVSS) attached in parallel with these lines can detect the lightning flash's transient irregular current, and, through alteration of its physical properties, route the spike to an attached earthing ground, thereby protecting the equipment from damage.

## Types

Three primary types of lightning are defined by the "starting" and "ending" points of a flash channel.

• Intra-cloud (IC) or in-cloud lightning occurs within a single thundercloud unit.
• Cloud-to-cloud (CC) or inter-cloud lightning starts and ends between two different "functional" thundercloud units.
• Cloud-to-ground (CG) lightning primarily originates in the thundercloud and terminates on an Earth surface, but may also occur in the reverse direction, that is ground to cloud.

There are variations of each type, such as "positive" versus "negative" CG flashes, that have different physical characteristics common to each which can be measured. Different common names used to describe a particular lightning event may be attributed to the same or to different events.

### Cloud to ground (CG)

Cloud-to-ground lightning

Cloud-to-ground (CG) lightning is a lightning discharge between a thundercloud and the ground. It is initiated by a stepped leader moving down from the cloud, which is met by a streamer moving up from the ground.

CG is the least common, but best understood of all types of lightning. It is easier to study scientifically because it terminates on a physical object, namely the Earth, and lends itself to being measured by instruments on the ground. Of the three primary types of lightning, it poses the greatest threat to life and property since it terminates on the Earth or "strikes".

The overall discharge, termed a flash, is composed of a number of processes such as preliminary breakdown, stepped leaders, connecting leaders, return strokes, dart leaders, and subsequent return strokes.[58] The conductivity of the ground, be it ground, fresh water or salt water, may affect the lightning discharge rate and thus visible characteristics.[59]

#### Positive and negative lightning

Cloud-to-ground (CG) lightning is either positive or negative, as defined by the direction of the conventional electric current between cloud and ground. Most CG lightning is negative, meaning that a negative charge is transferred to ground and electrons travel downward along the lightning channel (conventionally the current flows from the ground to the cloud). The reverse happens in a positive CG flash, where electrons travel upward along the lightning channel and a positive charge is transferred to the ground (conventionally the current flows from the cloud to the ground). Positive lightning is less common than negative lightning, and on average makes up less than 5% of all lightning strikes.[60]

A bolt from the blue lightning strike which appears to initiate from the clear, but the turbulent sky above the anvil cloud and drive a bolt of plasma through the cloud directly to the ground. They are commonly referred to as positive flashes, despite the fact that they are usually negative in polarity.

There are six different mechanisms theorized to result in the formation of positive lightning.[61]

• Vertical wind shear displacing the upper positive charge region of a thundercloud, exposing it to the ground below.
• The loss of lower charge regions in the dissipating stage of a thunderstorm, leaving the primary positive charge region.
• A complex arrangement of charge regions in a thundercloud, effectively resulting in an inverted dipole or inverted tripole in which the main negative charge region is above the main positive charge region instead of beneath it.
• An unusually large lower positive charge region in the thundercloud.
• Cutoff of an extended negative leader from its origin which creates a new bidirectional leader in which the positive end strikes the ground, commonly seen in anvil-crawler spider flashes.
• The initiation of a downward positive branch from an IC lightning flash.

Contrary to popular belief, positive lightning flashes do not necessarily originate from the anvil or the upper positive charge region and strike a rain-free area outside of the thunderstorm. This belief is based on the outdated idea that lightning leaders are unipolar and originate from their respective charge region.

Positive lightning strikes tend to be much more intense than their negative counterparts. An average bolt of negative lightning carries an electric current of 30,000 amperes (30 kA), and transfers 15 C (coulombs) of electric charge and 1 gigajoule of energy. Large bolts of positive lightning can carry up to 120 kA and 350 C.[62] The average positive ground flash has roughly double the peak current of a typical negative flash, and can produce peak currents up to 400 kA and charges of several hundred coulombs.[63][64] Furthermore, positive ground flashes with high peak currents are commonly followed by long continuing currents, a correlation not seen in negative ground flashes.[65]

As a result of their greater power, positive lightning strikes are considerably more dangerous than negative strikes. Positive lightning produces both higher peak currents and longer continuing currents, making them capable of heating surfaces to much higher levels which increases the likelihood of a fire being ignited. The long distances positive lightning can propagate through clear air explains why they are known as "bolts from the blue", giving no warning to observers.

Despite the popular misconception that these[clarification needed] are positive lightning strikes due to them seemingly originating from the positive charge region, observations have shown that these are in fact negative flashes. They begin as IC flashes within the cloud, the negative leader then exits the cloud from the positive charge region before propagating through clear air and striking the ground some distance away.[66][67]

Positive lightning has also been shown to trigger the occurrence of upward lightning flashes from the tops of tall structures and is largely responsible for the initiation of sprites several tens of km above ground level. Positive lightning tends to occur more frequently in winter storms, as with thundersnow, during intense tornadoes[68] and in the dissipation stage of a thunderstorm.[69] Huge quantities of extremely low frequency (ELF) and very low frequency (VLF) radio waves are also generated.[70]

### Cloud to cloud (CC) and intra-cloud (IC)

Lightning discharges may occur between areas of cloud without contacting the ground. When it occurs between two separate clouds, it is known as cloud-to-cloud (CC) or inter-cloud lightning; when it occurs between areas of differing electric potential within a single cloud, it is known as intra-cloud (IC) lightning. IC lightning is the most frequently occurring type.[69]

IC lightning most commonly occurs between the upper anvil portion and lower reaches of a given thunderstorm. This lightning can sometimes be observed at great distances at night as so-called "sheet lightning". In such instances, the observer may see only a flash of light without hearing any thunder.

Another term used for cloud–cloud or cloud–cloud–ground lightning is "Anvil Crawler", due to the habit of charge, typically originating beneath or within the anvil and scrambling through the upper cloud layers of a thunderstorm, often generating dramatic multiple branch strokes. These are usually seen as a thunderstorm passes over the observer or begins to decay. The most vivid crawler behavior occurs in well developed thunderstorms that feature extensive rear anvil shearing.

### Observational variations

Anvil Crawler over Lake Wright Patman south of Redwater, Texas on the backside of a large area of rain associated with a cold-front
• Anvil crawler lightning, sometimes called spider lightning is created when leaders propagate through horizontally-extensive charge regions in mature thunderstorms, usually the stratiform regions of mesoscale convective systems. These discharges usually begin as IC discharges originating within the convective region; the negative leader end then propagates well into the aforementioned charge regions in the stratiform area. If the leader becomes too long, it may separate into multiple bidirectional leaders. When this happens, the positive end of the separated leader may strike the ground as a positive CG flash or crawl on the underside of the cloud, creating a spectacular display of lightning crawling across the sky. Ground flashes produced in this manner tend to transfer high amounts of charge, and this can trigger upward lightning flashes and upper-atmospheric lightning.[55]
• Ball lightning may be an atmospheric electrical phenomenon, the physical nature of which is still controversial. The term refers to reports of luminous, usually spherical objects which vary from pea-sized to several metres in diameter.[71] It is sometimes associated with thunderstorms, but unlike lightning flashes, which last only a fraction of a second, ball lightning reportedly lasts many seconds. Ball lightning has been described by eyewitnesses but rarely recorded by meteorologists.[72][73] Scientific data on natural ball lightning is scarce owing to its infrequency and unpredictability. The presumption of its existence is based on reported public sightings, and has therefore produced somewhat inconsistent findings. Brett Porter,[74] a wildlife ranger, reported taking a photo in Queensland, Australia in 1987.

• Bead lightning, also known by the terms pearl lightning, chain lightning, perlschnurblitz and éclair en chapelet, to name a few [75] is the decaying stage of a lightning channel in which the luminosity of the channel breaks up into segments.[76] Nearly every lightning discharge will exhibit beading as the channel cools immediately after a return stroke, sometimes referred to as the lightning's 'bead-out' stage. 'Bead lightning' is more properly a stage of a normal lightning discharge rather than a type of lightning in itself. Beading of a lightning channel is usually a small-scale feature, and therefore is often only apparent when the observer/camera is close to the lightning.[77]
Gigantic jet as seen from the summit of Mauna Kea, Hawaii.

• Clear-air lightning describes lightning that occurs with no apparent cloud close enough to have produced it. In the U.S. and Canadian Rockies, a thunderstorm can be in an adjacent valley and not observable from the valley where the lightning bolt strikes, either visually or audibly. European and Asian mountainous areas experience similar events. Also in areas such as sounds, large lakes or open plains, when the storm cell is on the near horizon (within 26 km or 16 mi) there may be some distant activity, a strike can occur and as the storm is so far away, the strike is referred to as a bolt from the blue.[78] These flashes usually begin as normal IC lightning flashes before the negative leader exits the cloud and strikes the ground a considerable distance away.[66][67] Positive clear-air strikes can occur in highly sheared environments where the upper positive charge region becomes horizontally displaced from the precipitation area.[79]
• Cloud-to-air lightning is a lightning flash in which one end of a bidirectional leader exits the cloud, but does not result in a ground flash. Such flashes can sometimes be thought of as failed ground flashes. Blue jets and gigantic jets are a form of cloud-to-air or cloud-to-ionosphere lightning where a leader is launched from the top of a thunderstorm.
• Crown flash is a lightning flash accompanied by the brightening of the thunderhead crown followed by the emanation of aurora-like streamers into the clear atmosphere.
• Dry lightning is lightning that occurs with no precipitation at the surface and is the most common natural cause of wildfires.[80] Pyrocumulus clouds produce lightning for the same reason that it is produced by cumulonimbus clouds. This term is mainly used in Australia, Canada, and the United States.

• Forked lightning is cloud-to-ground lightning that exhibits branching of its path.
• Heat lightning is a lightning flash that appears to produce no discernible thunder because it occurs too far away for the thunder to be heard. The sound waves dissipate before they reach the observer.[81]

• Ribbon lightning occurs in thunderstorms with high cross winds and multiple return strokes. The wind will blow each successive return stroke slightly to one side of the previous return stroke, causing a ribbon effect.[82]

• Rocket lightning is a form of cloud discharge, generally horizontal and at cloud base, with a luminous channel appearing to advance through the air with visually resolvable speed, often intermittently.[83]

• Sheet lightning is cloud-to-cloud lightning that exhibits a diffuse brightening of the surface of a cloud, caused by the actual discharge path being hidden or too far away. The lightning itself cannot be seen by the spectator, so it appears as only a flash, or a sheet of light. The lightning may be too far away to discern individual flashes.

• Smooth channel lightning is an informal term referring to a type of cloud-to-ground lightning strike that has no visible branching and appears like a line with smooth curves as opposed to the jagged appearance of most lightning channels. They are a form of positive lightning generally observed in or near the convective regions of severe thunderstorms in the north central United States. It is theorized that severe thunderstorms in this region obtain an "inverted tripole" charge structure in which the main positive charge region is located below the main negative charge region instead of above it, and as a result these thunderstorms generate predominantly positive cloud-to-ground lightning. The term "smooth channel lightning" is also sometimes attributed to upward ground-to-cloud lightning flashes, which are generally negative flashes initiated by upward positive leaders from tall structures.

• Staccato lightning is a cloud-to-ground lightning (CG) strike which is a short-duration stroke that (often but not always) appears as a single very bright flash and often has considerable branching.[84] These are often found in the visual vault area near the mesocyclone of rotating thunderstorms and coincides with intensification of thunderstorm updrafts. A similar cloud-to-cloud strike consisting of a brief flash over a small area, appearing like a blip, also occurs in a similar area of rotating updrafts.[85]
This CG was of very short duration, exhibited highly branched channels and was very bright indicating that it was staccato lightning near New Boston, Texas.

• Superbolts are rather loosely defined as strikes with a source energy of more than 100 gigajoule [100 GJ] (most lightning strikes come in at around 1 gigajoule [1 GJ]). Events of this magnitude occur about as frequently as one in 240 strikes. They are not categorically distinct from ordinary lightning strikes, and simply represent the uppermost edge of a continuum. Contrary to popular misconception, superbolts can be either positively or negatively charged, and the charge ratio is comparable to that of "ordinary" lightning.[86][87][88]

• Sympathetic lightning is the tendency of lightning to be loosely coordinated across long distances. Discharges can appear in clusters when viewed from space.Cite error: Closing </ref> missing for <ref> tag The latter usually occurs during the cold season and may be the dominant lightning type in thundersnow events.[89]

## Effects

### Lightning strike

#### Effects on objects

Explosive steam pressure between trunk and bark from lightning strike blew away birch bark

thumb|Strike mark on trunk of an Oklahoma black walnut

Objects struck by lightning experience heat and magnetic forces of great magnitude. The heat created by lightning currents travelling through a tree may vaporize its sap, causing a steam explosion that bursts the trunk. As lightning travels through sandy soil, the soil surrounding the plasma channel may melt, forming tubular structures called fulgurites.

#### Effects on buildings and vehicles

Buildings or tall structures hit by lightning may be damaged as the lightning seeks unimpeded paths to the ground. By safely conducting a lightning strike to the ground, a lightning protection system, usually incorporating at least one lightning rod, can greatly reduce the probability of severe property damage.

Aircraft are highly susceptible to being struck due to their metallic fuselages, but lightning strikes are generally not dangerous to them.[90] Due to the conductive properties of aluminium alloy, the fuselage acts as a Faraday cage. Present day aircraft are built to be safe from a lightning strike and passengers will generally not even know that it has happened.

#### Effects on animals

Although 90 percent of people struck by lightning survive,[91] animals – including humans – struck by lightning may suffer severe injury due to internal organ and nervous system damage.

#### Other effects

Lightning serves an important role in the nitrogen cycle by oxidizing diatomic nitrogen in the air into nitrates which are deposited by rain and can fertilize the growth of plants and other organisms.[92][93]

### Thunder

Main page: Physics:Thunder

Because the electrostatic discharge of terrestrial lightning superheats the air to plasma temperatures along the length of the discharge channel in a short duration, kinetic theory dictates gaseous molecules undergo a rapid increase in pressure and thus expand outward from the lightning creating a shock wave audible as thunder. Since the sound waves propagate not from a single point source but along the length of the lightning's path, the sound origin's varying distances from the observer can generate a rolling or rumbling effect. Perception of the sonic characteristics is further complicated by factors such as the irregular and possibly branching geometry of the lightning channel, by acoustic echoing from terrain, and by the usually multiple-stroke characteristic of the lightning strike.

Light travels at about 300,000,000 m/s (980,000,000 ft/s), and sound travels through air at about 343 m/s (1,130 ft/s). An observer can approximate the distance to the strike by timing the interval between the visible lightning and the audible thunder it generates. A lightning flash preceding its thunder by one second would be approximately 343 m (1,125 ft) in distance; a delay of three seconds would indicate a distance of about 1 km or 0.62 mi (3 × 343 m). A flash preceding thunder by five seconds would indicate a distance of approximately 1.7 km or 1.1 mi (5 × 343 m). Consequently, a lightning strike observed at a very close distance will be accompanied by a sudden clap of thunder, with almost no perceptible time lapse, possibly accompanied by the smell of ozone (O3).

Lightning at a sufficient distance may be seen and not heard; there is data that a lightning storm can be seen at over 160 km (100 mi) whereas the thunder travels about 32 km (20 mi). Anecdotally, there are many examples of people saying 'the storm was directly overhead or all-around and yet there was no thunder'. Since thunderclouds can be up to 20 km high,[94] lightning occurring high up in the cloud may appear close but is actually too far away to produce noticeable thunder.

Lightning discharges generate radio-frequency pulses which can be received thousands of kilometres from their source as radio atmospheric signals and whistlers.

The production of X-rays by a bolt of lightning was theoretically predicted as early as 1925,[95] but no evidence was found until 2001/2002,[96][97][98] when researchers at the New Mexico Institute of Mining and Technology detected X-ray emissions from an induced lightning strike along a grounded wire trailed behind a rocket shot into a storm cloud. In the same year University of Florida and Florida Tech researchers used an array of electric field and X-ray detectors at a lightning research facility in North Florida to confirm that natural lightning makes X-rays in large quantities during the propagation of stepped leaders. The cause of the X-ray emissions is still a matter for research, as the temperature of lightning is too low to account for the X-rays observed.[99][100]

A number of observations by space-based telescopes have revealed even higher energy gamma ray emissions, the so-called terrestrial gamma-ray flashes (TGFs). These observations pose a challenge to current theories of lightning, especially with the recent discovery of the clear signatures of antimatter produced in lightning.[101] Recent research has shown that secondary species, produced by these TGFs, such as electrons, positrons, neutrons or protons, can gain energies of up to several tens of MeV.[102][103]

### Ozone and nitrogen oxides

The very high temperatures generated by lightning lead to significant local increases in ozone and oxides of nitrogen. Each lightning flash in temperate and sub-tropical areas produces 7 kg of NO
x
on average.[104] In the troposphere the effect of lightning can increase NO
x
by 90% and ozone by 30%.[105]

## Volcanic

Main page: Physics:Volcanic lightning
Volcanic material thrust high into the atmosphere can trigger lightning.

Volcanic activity produces lightning-friendly conditions in multiple ways. The enormous quantity of pulverized material and gases explosively ejected into the atmosphere creates a dense plume of particles. The ash density and constant motion within the volcanic plume produces charge by frictional interactions (triboelectrification), resulting in very powerful and very frequent flashes as the cloud attempts to neutralize itself. Due to the extensive solid material (ash) content, unlike the water rich charge generating zones of a normal thundercloud, it is often called a dirty thunderstorm.

• Powerful and frequent flashes have been witnessed in the volcanic plume as far back as the 79 AD eruption of Vesuvius by Pliny The Younger.[106]
• Likewise, vapors and ash originating from vents on the volcano's flanks may produce more localized and smaller flashes upwards of 2.9 km long.
• Small, short duration sparks, recently documented near newly extruded magma, attest to the material being highly charged prior to even entering the atmosphere.[107]

If the volcanic ash plume rises to freezing temperatures, ice particles form and collide with ash particles to cause electrification. Lightning can be detected in any explosion but the causation of additional electrification from ice particles in ash can lead to a stronger electrical field and a higher rate of detectable lightning. Lightning is also used as a volcano monitoring tool for detecting hazardous eruptions.[108]

## Fire lightning

Intense forest fires, such as those seen in the 2019–20 Australian bushfire season, can create their own weather systems that can produce lightning and other weather phenomena.[109] Intense heat from a fire causes air to rapidly rise within the smoke plume, causing the formation of pyrocumulonimbus clouds. Cooler air is drawn in by this turbulent, rising air, helping to cool the plume. The rising plume is further cooled by the lower atmospheric pressure at high altitude, allowing the moisture in it to condense into cloud. Pyrocumulonimbus clouds form in an unstable atmosphere. These weather systems can produce dry lightning, fire tornadoes, intense winds, and dirty hail.[109]

## Extraterrestrial

Lightning has been observed within the atmospheres of other planets, such as Jupiter and Saturn. Although in the minority on Earth, superbolts appear to be common on Jupiter.

Lightning on Venus has been a controversial subject after decades of study. During the Soviet Venera and U.S. Pioneer missions of the 1970s and 1980s, signals suggesting lightning may be present in the upper atmosphere were detected.[110] Although the Cassini–Huygens mission fly-by of Venus in 1999 detected no signs of lightning, the observation window lasted mere hours. Radio pulses recorded by the spacecraft Venus Express (which began orbiting Venus in April 2006) may originate from lightning on Venus.

## Human-related phenomena

• Airplane contrails have also been observed to influence lightning to a small degree. The water vapor-dense contrails of airplanes may provide a lower resistance pathway through the atmosphere having some influence upon the establishment of an ionic pathway for a lightning flash to follow.[111]
• Rocket exhaust plumes provided a pathway for lightning when it was witnessed striking the Apollo 12 rocket shortly after takeoff.
• Thermonuclear explosions, by providing extra material for electrical conduction and a very turbulent localized atmosphere, have been seen triggering lightning flashes within the mushroom cloud. In addition, intense gamma radiation from large nuclear explosions may develop intensely charged regions in the surrounding air through Compton scattering. The intensely charged space charge regions create multiple clear-air lightning discharges shortly after the device detonates.[112]

## Scientific study

The science of lightning is called fulminology.

### Properties

Thunder is heard as a rolling, gradually dissipating rumble because the sound from different portions of a long stroke arrives at slightly different times.[113]

When the local electric field exceeds the dielectric strength of damp air (about 3 MV/m), electrical discharge results in a strike, often followed by commensurate discharges branching from the same path. Mechanisms that cause the charges to build up to lightning are still a matter of scientific investigation.[114][115] A 2016 study confirmed dielectric breakdown is involved.[116] Lightning may be caused by the circulation of warm moisture-filled air through electric fields.[117] Ice or water particles then accumulate charge as in a Van de Graaff generator.[118]

Researchers at the University of Florida found that the final one-dimensional speeds of 10 flashes observed were between 1.0×105 and 1.4×106 m/s, with an average of 4.4×105 m/s.[119]

### Detection and monitoring

Main page: Physics:Lightning detection
Lightning strike counter in a museum

The earliest detector invented to warn of the approach of a thunderstorm was the lightning bell. Benjamin Franklin installed one such device in his house.[120][121] The detector was based on an electrostatic device called the 'electric chimes' invented by Andrew Gordon in 1742.

Lightning discharges generate a wide range of electromagnetic radiations, including radio-frequency pulses. The times at which a pulse from a given lightning discharge arrives at several receivers can be used to locate the source of the discharge with a precision on the order of metres. The United States federal government has constructed a nationwide grid of such lightning detectors, allowing lightning discharges to be tracked in real time throughout the continental U.S.[122][123] In addition, a private global detection system that consists of over 500 detection stations owned and operated by hobbyists/volunteers provides near real-time lightning maps at blitzortung.org

The Earth-ionosphere waveguide traps electromagnetic VLF- and ELF waves. Electromagnetic pulses transmitted by lightning strikes propagate within that waveguide. The waveguide is dispersive, which means that their group velocity depends on frequency. The difference of the group time delay of a lightning pulse at adjacent frequencies is proportional to the distance between transmitter and receiver. Together with direction-finding methods, this allows locating lightning strikes up to distances of 10,000 km from their origin. Moreover, the eigenfrequencies of the Earth-ionospheric waveguide, the Schumann resonances at about 7.5 Hz, are used to determine the global thunderstorm activity.[124]

In addition to ground-based lightning detection, several instruments aboard satellites have been constructed to observe lightning distribution. These include the Optical Transient Detector (OTD), aboard the OrbView-1 satellite launched on April 3, 1995, and the subsequent Lightning Imaging Sensor (LIS) aboard TRMM launched on November 28, 1997.[125][126][127]

Starting in 2016, the National Oceanic and Atmospheric Administration launched Geostationary Operational Environmental Satellite–R Series (GOES-R) weather satellites outfitted with Geostationary Lightning Mapper (GLM) instruments which are near-infrared optical transient detectors that can detect the momentary changes in an optical scene, indicating the presence of lightning.[128][129] The lighting detection data can be converted into a real-time map of lightning activity across the Western Hemisphere; this mapping technique has been implemented by the United States National Weather Service.[130]

### Artificially triggered

• Rocket-triggered lightning can be "triggered" by launching specially designed rockets trailing spools of wire into thunderstorms. The wire unwinds as the rocket ascends, creating an elevated ground that can attract descending leaders. If a leader attaches, the wire provides a low-resistance pathway for a lightning flash to occur. The wire is vaporized by the return current flow, creating a straight lightning plasma channel in its place. This method allows for scientific research of lightning to occur under a more controlled and predictable manner.[131]
The International Center for Lightning Research and Testing (ICLRT) at Camp Blanding, Florida typically uses rocket triggered lightning in their research studies.
• Laser-triggered
Since the 1970s,[132] researchers have attempted to trigger lightning strikes by means of infrared or ultraviolet lasers, which create a channel of ionized gas through which the lightning would be conducted to ground. Such triggering of lightning is intended to protect rocket launching pads, electric power facilities, and other sensitive targets.[133][134][135][136][137]
In New Mexico, U.S., scientists tested a new terawatt laser which provoked lightning. Scientists fired ultra-fast pulses from an extremely powerful laser thus sending several terawatts into the clouds to call down electrical discharges in storm clouds over the region. The laser beams sent from the laser make channels of ionized molecules known as filaments. Before the lightning strikes earth, the filaments lead electricity through the clouds, playing the role of lightning rods. Researchers generated filaments that lived a period too short to trigger a real lightning strike. Nevertheless, a boost in electrical activity within the clouds was registered. According to the French and German scientists who ran the experiment, the fast pulses sent from the laser will be able to provoke lightning strikes on demand.[138] Statistical analysis showed that their laser pulses indeed enhanced the electrical activity in the thundercloud where it was aimed—in effect they generated small local discharges located at the position of the plasma channels.[139]

### Physical manifestations

Lightning-induced remanent magnetization (LIRM) mapped during a magnetic field gradient survey of an archaeological site located in Wyoming, United States.

#### Magnetism

The movement of electrical charges produces a magnetic field (see electromagnetism). The intense currents of a lightning discharge create a fleeting but very strong magnetic field. Where the lightning current path passes through rock, soil, or metal these materials can become permanently magnetized. This effect is known as lightning-induced remanent magnetism, or LIRM. These currents follow the least resistive path, often horizontally near the surface[140][141] but sometimes vertically, where faults, ore bodies, or ground water offers a less resistive path.[142] One theory suggests that lodestones, natural magnets encountered in ancient times, were created in this manner.[143]

Lightning-induced magnetic anomalies can be mapped in the ground,[144][145] and analysis of magnetized materials can confirm lightning was the source of the magnetization[146] and provide an estimate of the peak current of the lightning discharge.[147]

Research at the University of Innsbruck has found that magnetic fields generated by plasma may induce hallucinations in subjects located within 200 m (660 ft) of a severe lightning storm.[148]

### Solar wind and cosmic rays

Some high energy cosmic rays produced by supernovas as well as solar particles from the solar wind, enter the atmosphere and electrify the air, which may create pathways for lightning bolts.[149]

### Lightning and climate change

Due to the low resolution of global climate models, accurately representing lightning in these climate models is difficult, largely due to their inability to simulate the convection and cloud ice imperative which are fundamental to lightning formation. Research from the Future Climate for Africa programme demonstrates that using a convection-permitting model over Africa can more accurately capture convective thunderstorms and the distribution of ice particles. This research indicates climate change may increase the total amount of lightning only slightly: the total number of lightning days per year decreases, while more cloud ice and stronger convection leads to more lightning strikes occurring on days when lightning does occur.[150]

A study from the University of Washington looked at lightning activity in the Arctic from 2010 to 2020. The ratio of Arctic summertime strokes was compared to total global strokes and was observed to be increasing with time, indicating that the region is becoming more influenced by lightning. The fraction of strokes above 65 degrees north was found to be increasing linearly with the NOAA global temperature anomaly and grew by a factor of 3 as the anomaly increased from 0.65 to 0.95 °C [151]

## In culture and religion

### Religion and mythology

Lightning by Mikalojus Konstantinas Ciurlionis (1909)

In many cultures, lightning has been viewed as part of a deity or a deity in and of itself. These include the Greek god Zeus, the Aztec god Tlaloc, the Mayan God K, Slavic mythology's Perun, the Baltic Pērkons/Perkūnas, Thor in Norse mythology, Ukko in Finnish mythology, the Hindu god Indra, the Yoruba god Sango, Illapa in Inca mythology and the Shinto god Raijin.[152] In the traditional religion of the African Bantu tribes, lightning is a sign of the ire of the gods. Scriptures in Judaism, Islam and Christianity also ascribe supernatural importance to lightning. In Christianity, the Second Coming of Jesus is compared to lightning.[Matthew 24:27][Luke 17:24]

### Expressions and sayings

The expression "Lightning never strikes twice (in the same place)" is similar to "Opportunity never knocks twice" in the vein of a "once in a lifetime" opportunity, i.e., something that is generally considered improbable. Lightning occurs frequently and more so in specific areas. Since various factors alter the probability of strikes at any given location, repeat lightning strikes have a very low probability (but are not impossible).[153][154] Similarly, "A bolt from the blue" refers to something totally unexpected, and "A person being struck by lightning" is an imaginative or comedic metaphor for someone to experience a once in a lifetime, striking, sudden lightning-speed revelation, similar to an epiphany or an enlightenment.

In French and Italian, the expression for "Love at first sight" is coup de foudre and colpo di fulmine, respectively, which literally translated means "lightning strike". Some European languages have a separate word for lightning which strikes the ground (as opposed to lightning in general); often it is a cognate of the English word "rays". The name of Australia's most celebrated thoroughbred horse, Phar Lap, derives from the shared Zhuang and Thai word for lightning.[155]

### Political and military culture

Two lightning bolts pictured in the former coat of arms of the Yli-Ii municipality

The bolt of lightning in heraldry is called a thunderbolt and is shown as a zigzag with non-pointed ends. This symbol usually represents power and speed.

Some political parties use lightning flashes as a symbol of power, such as the People's Action Party in Singapore, the British Union of Fascists during the 1930s, and the National States' Rights Party in the United States during the 1950s.[156] The Schutzstaffel, the paramilitary wing of the Nazi Party, used the Sig rune in their logo which symbolizes lightning. The German word Blitzkrieg, which means "lightning war", was a major offensive strategy of the German army during World War II.

The lightning bolt is a common insignia for military communications units throughout the world. A lightning bolt is also the NATO symbol for a signal asset.

## References

### Notes

1. Maggio, Christopher R.; Marshall, Thomas C.; Stolzenburg, Maribeth (2009). "Estimations of charge transferred and energy released by lightning flashes in short bursts" (in en). Journal of Geophysical Research: Atmospheres and Formed Through Several Layers 114 (D14): D14203. doi:10.1029/2008JD011506. ISSN 2156-2202. Bibcode2009JGRD..11414203M.
2. Jennings, S. G. & Latham, J. "The charging of water drops falling and colliding in an electric field". Proc. 3rd Conf. Static Electrification Paper 10. pp.84-92 (1971) Jennings, S. G. & Latham, J. "The charging of water drops falling and colliding in an electric field" or "Die Aufladung von Wassertropfen, die beim Fallen in einem elektrischen Feld kollidieren". Archiv für Meteorologie, Geophysik und Bioklimatologie, Serie A volume 21, pages 299–306 (1972)
3.   This article incorporates text from this source, which is in the public domain.
4. Francis, G. W., "Electrostatic Experiments" Oleg D. Jefimenko, Editor, Electret Scientific Company, Star City, 2005
5. Aplin, K. L.; Harrison, R. G. (3 September 2013). "Lord Kelvin's atmospheric electricity measurements". History of Geo- and Space Sciences 4 (2): 83–95. doi:10.5194/hgss-4-83-2013. Bibcode2013HGSS....4...83A.
6. Desmet, S; Orban, F; Grandjean, F (1 April 1989). "On the Kelvin electrostatic generator". European Journal of Physics 10 (2): 118–122. doi:10.1088/0143-0807/10/2/008. Bibcode1989EJPh...10..118D.
7. Dash, J G; Wettlaufer, J S (1 January 2003). "The surface physics of ice in thunderstorms". Canadian Journal of Physics 81 (1–2): 201–207. doi:10.1139/P03-011. Bibcode2003CaJPh..81..201D.
8. Dash, J. G.; Mason, B. L.; Wettlaufer, J. S. (16 September 2001). "Theory of charge and mass transfer in ice-ice collisions". Journal of Geophysical Research: Atmospheres 106 (D17): 20395–20402. doi:10.1029/2001JD900109. Bibcode2001JGR...10620395D.
9. Buxton, G. V., Greenstock, C. L., Helman, W. P. and Ross, A. B. "Critical Review of rate constants for reactions of hydrated electrons, hydrogen atoms and hydroxyl radicals (OH/O in aqueous solution." J. Phys. Chem. Ref. Data 17, 513–886 (1988).
10. Uman, Martin (1986). All About Lightning. New York: Dover. pp. 74. ISBN 978-0-486-25237-7.
11. Witzke, Megan; Rumbach, Paul; Go, David B; Sankaran, R Mohan (7 November 2012). "Evidence for the electrolysis of water by atmospheric-pressure plasmas formed at the surface of aqueous solutions". Journal of Physics D 45 (44): 442001. doi:10.1088/0022-3727/45/44/442001. Bibcode2012JPhD...45R2001W.
12. Uman (1986) p. 81.
13. Uman (1986) p. 55.
14. Füllekrug, Martin; Mareev, Eugene A.; Rycroft, Michael J. (2006-05-01) (in en). Sprites, Elves and Intense Lightning Discharges. Springer Science & Business Media. ISBN 9781402046285. Bibcode2006seil.book.....F.
15. New Lightning Type Found Over Volcano? . News.nationalgeographic.com (February 2010). Retrieved on June 23, 2012.
16. "Bench collapse sparks lightning, roiling clouds". Volcano Watch. United States Geological Survey. June 11, 1998.
17. Pardo-Rodriguez, Lumari (Summer 2009) Lightning Activity in Atlantic Tropical Cyclones: Using the Long-Range Lightning Detection Network (LLDN) . MA Climate and Society, Columbia University Significant Opportunities in Atmospheric Research and Science Program.
18. Hurricane Lightning , NASA, January 9, 2006.
19. The Promise of Long-Range Lightning Detection in Better Understanding, Nowcasting, and Forecasting of Maritime Storms . Long Range Lightning Detection Network
20. Oliver, John E. (2005). Encyclopedia of World Climatology. National Oceanic and Atmospheric Administration. ISBN 978-1-4020-3264-6. Retrieved February 8, 2009.
21. Holton, James R.; Curry, Judith A.; Pyle, J. A. (2003) (in en). Encyclopedia of atmospheric sciences. Academic Press. ISBN 9780122270901.
22. "Where LightningStrikes". NASA Science. Science News.. December 5, 2001.
23. Uman (1986) Ch. 8, p. 68.
24. "Annual Lightning Flash Rate". National Oceanic and Atmospheric Administration.
25. Fischetti, M. (2016) Lightning Hotspots, Scientific American 314: 76 (May 2016)
26. "Lightning Activity in Singapore". National Environmental Agency. 2002.
27. "Staying Safe in Lightning Alley". NASA. January 3, 2007.
28. Pierce, Kevin (2000). "Summer Lightning Ahead". Florida Environment.com.
29. Randall Cerveny (1 February 2022), "New WMO Certified Megaflash Lightning Extremes for Flash Distance (768 km) and Duration (17.01 seconds) Recorded from Space", Bulletin of the American Meteorological Society, doi:10.1175/BAMS-D-21-0254.1
30. Larson, Nina (1 February 2022). "770-km US megaflash sets new lightning record".
31. Saunders, C. P. R. (1993). "A Review of Thunderstorm Electrification Processes". Journal of Applied Meteorology 32 (4): 642–55. doi:10.1175/1520-0450(1993)032<0642:AROTEP>2.0.CO;2. Bibcode1993JApMe..32..642S.
32. Ultraslow-motion video of stepped leader propagation: ztresearch.com
33. Goulde, R.H. (1977) "The lightning conductor", pp. 545–576 in Lightning Protection, R.H. Golde, Ed., Lightning, Vol. 2, Academic Press.
34. Stolzenburg, Maribeth; Marshall, Thomas C. (2008). "Charge Structure and Dynamics in Thunderstorms". Space Science Reviews 137 (1–4): 355. doi:10.1007/s11214-008-9338-z. Bibcode2008SSRv..137..355S.
35. Petersen, Danyal; Bailey, Matthew; Beasley, William H.; Hallett, John (2008). "A brief review of the problem of lightning initiation and a hypothesis of initial lightning leader formation". Journal of Geophysical Research 113 (D17): D17205. doi:10.1029/2007JD009036. Bibcode2008JGRD..11317205P.
36. Hooyberghs, Hans; Van Schaeybroeck, Bert; Moreira, André A.; Andrade, José S.; Herrmann, Hans J.; Indekeu, Joseph O. (2010). "Biased percolation on scale-free networks". Physical Review E 81 (1): 011102. doi:10.1103/PhysRevE.81.011102. PMID 20365318. Bibcode2010PhRvE..81a1102H.
37. Griffiths, R. F.; Phelps, C. T. (1976). "A model for lightning initiation arising from positive corona streamer development" (in en). Journal of Geophysical Research 81 (21): 3671–3676. doi:10.1029/JC081i021p03671. ISSN 2156-2202. Bibcode1976JGR....81.3671G.
38. Sterpka, Christopher; Dwyer, J; Liu, N; Hare, B M; Scholten, O; Buitink, S; Ter Veen, S; Nelles, A (2021-11-24) (in en). The Spontaneous Nature of Lightning Initiation Revealed. doi:10.1002/essoar.10508882.1.
39. Lewton, Thomas (2021-12-20). "Detailed Footage Finally Reveals What Triggers Lightning" (in en).
40. Kasemir, H. W. (1950) "Qualitative Übersicht über Potential-, Feld- und Ladungsverhaltnisse Bei einer Blitzentladung in der Gewitterwolke" (Qualitative survey of the potential, field and charge conditions during a lightning discharge in the thunderstorm cloud) in Das Gewitter (The Thunderstorm), H. Israel, ed., Leipzig, Germany: Akademische Verlagsgesellschaft.
41. Ruhnke, Lothar H. (June 7, 2007) Death notice: Heinz Wolfram Kasemir. physicstoday.org
42. Stephan, Karl (March 3, 2016). "The Man Who Understood Lightning". Scientific American.
43. Saba, M. M. F.; Paiva, A. R.; Schumann, C.; Ferro, M. A. S.; Naccarato, K. P.; Silva, J. C. O.; Siqueira, F. V. C.; Custódio, D. M. (2017). "Lightning attachment process to common buildings". Geophysical Research Letters 44 (9): 4368–4375. doi:10.1002/2017GL072796. Bibcode2017GeoRL..44.4368S.
44. Uman, M. A. (2001). The lightning discharge. Courier Corporation. ISBN 9780486151984. Retrieved September 1, 2020.
45. See, for example, here
46. Idone, V. P.; Orville, R. E.; Mach, D. M.; Rust, W. D. (1987). "The propagation speed of a positive lightning return stroke". Geophysical Research Letters 14 (11): 1150. doi:10.1029/GL014i011p01150. Bibcode1987GeoRL..14.1150I.
47. Uman (1986) Ch. 5, p. 41.
48. Uman (1986) pp. 103–110.
49. Warner, Tom (2017-05-06). "Ground Flashes".
50. Uman (1986) Ch. 9, p. 78.
51. Lightning Protection and Transient Overvoltage | VERDOLIN SOLUTIONS INC. | HIGH VOLTAGE POWER ENGINEERING SERVICES
52. V. Cooray, Mechanism of the Lightning Flash, in The Lightning Flash, 2nd ed., V. Cooray (Ed.), The Institution of Engineering and Technology, London, United Kingdom, 2014, pp. 119–229
53. Jones, Nicola (4 January 2021). "Salty Seas Make Lightning Brighter". Smithsonian.
54. Nag, Amitabh; Rakov, Vladimir A (2012). "Positive lightning: An overview, new observations, and inferences". Journal of Geophysical Research: Atmospheres 117 (D8): n/a. doi:10.1029/2012JD017545. Bibcode2012JGRD..117.8109N.
55. Hasbrouck, Richard. Mitigating Lightning Hazards , Science & Technology Review May 1996. Retrieved on April 26, 2009.
56. V.A. Rakov, M.A. Uman, Positive and bipolar lightning discharges to ground, in: Light. Phys. Eff., Cambridge University Press, 2003: pp. 214–240
57. U.A.Bakshi; M.V.Bakshi (1 January 2009). Power System – II. Technical Publications. p. 12. ISBN 978-81-8431-536-3.
58. Saba, Marcelo M. F; Schulz, Wolfgang; Warner, Tom A; Campos, Leandro Z. S; Schumann, Carina; Krider, E. Philip; Cummins, Kenneth L; Orville, Richard E (2010). "High-speed video observations of positive lightning flashes to ground". Journal of Geophysical Research: Atmospheres 115 (D24): D24201. doi:10.1029/2010JD014330. Bibcode2010JGRD..11524201S.
59. Lu, Gaopeng; Cummer, Steven A; Blakeslee, Richard J; Weiss, Stephanie; Beasley, William H (2012). "Lightning morphology and impulse charge moment change of high peak current negative strokes". Journal of Geophysical Research: Atmospheres 117 (D4): n/a. doi:10.1029/2011JD016890. Bibcode2012JGRD..117.4212L.
60. Krehbiel, Paul R; Riousset, Jeremy A; Pasko, Victor P; Thomas, Ronald J; Rison, William; Stanley, Mark A; Edens, Harald E (2008). "Upward electrical discharges from thunderstorms". Nature Geoscience 1 (4): 233. doi:10.1038/ngeo162. Bibcode2008NatGe...1..233K.
61. Antony H. Perez; Louis J. Wicker; Richard E. Orville (1997). "Characteristics of Cloud-to-Ground Lightning Associated with Violent Tornadoes". Weather Forecast. 12 (3): 428–37. doi:10.1175/1520-0434(1997)012<0428:COCTGL>2.0.CO;2. Bibcode1997WtFor..12..428P.
62. Boccippio, DJ; Williams, ER; Heckman, SJ; Lyons, WA; Baker, IT; Boldi, R (August 1995). "Sprites, ELF Transients, and Positive Ground Strokes". Science 269 (5227): 1088–1091. doi:10.1126/science.269.5227.1088. PMID 17755531. Bibcode1995Sci...269.1088B.
63. Singer, Stanley (1971). The Nature of Ball Lightning. New York: Plenum Press. ISBN 978-0-306-30494-1.
64. Ball, Philip (January 17, 2014). "Focus:First Spectrum of Ball Lightning". Physics 7: 5. doi:10.1103/physics.7.5. Bibcode2014PhyOJ...7....5B. Retrieved January 18, 2014.
65. Tennakone, Kirthi (2007). "Ball Lightning". Georgia State University.
66. Barry, James (1980), Ball Lightning and Bead Lightning, Springer, Boston, MA, doi:10.1007/978-1-4757-1710-5, ISBN 978-1-4757-1710-5
67. Minin, V. F.; Baibulatov, F. Kh. (1969). "On the nature of beaded lightning". Dokl. Akad. Nauk SSSR 188 (4): 795–798.
68. Scott, A (2000). "The Pre-Quaternary history of fire". Palaeogeography, Palaeoclimatology, Palaeoecology 164 (1–4): 281. doi:10.1016/S0031-0182(00)00192-9. Bibcode2000PPP...164..281S.
69. Haby, Jeff. "What is heat lightning?". theweatherprediction.com.
70. "Glossary". National Oceanic and Atmospheric Administration. National Weather Service.
71. Marshall, Tim; David Hoadley (illustrator) (May 1995). Storm Talk. Texas.
72. Turman, B. N. (1977). "Detection of lightning superbolts". Journal of Geophysical Research 82 (18): 2566–2568. doi:10.1029/JC082i018p02566. Bibcode1977JGR....82.2566T.
73. Holzworth, R. H. (2019). "Global Distribution of Superbolts". Journal of Geophysical Research: Atmospheres 124 (17–18): 9996–10005. doi:10.1029/2019JD030975. Bibcode2019JGRD..124.9996H.
74. Warner, Tom A.; Lang, Timothy J.; Lyons, Walter A. (2014). "Synoptic scale outbreak of self-initiated upward lightning (SIUL) from tall structures during the central U.S. Blizzard of 1-2 February 2011". Journal of Geophysical Research: Atmospheres 119 (15): 9530–9548. doi:10.1002/2014JD021691. Bibcode2014JGRD..119.9530W.
75. Jabr, Ferris (22 September 2014). "Lightning-Strike Survivors Tell Their Stories". Outside.
76. Bond, D.W.; Steiger, S.; Zhang, R.; Tie, X.; Orville, R.E. (2002). "The importance of NOx production by lightning in the tropics". Atmospheric Environment 36 (9): 1509–1519. doi:10.1016/s1352-2310(01)00553-2. Bibcode2002AtmEn..36.1509B.
77. Pickering, K.E., Bucsela, E., Allen, D, Cummings, K., Li, Y., MacGorman, D., Bruning, E. 2014. Estimates of Lightning NOx Production Per Flash from OMI NO2 and Lightning Observations. XV International Conference on Atmospheric Electricity, 15–20, June 2014.
78. Wilson, C.T.R. (1925). "The acceleration of beta-particles in strong electric fields such as those of thunderclouds". Proceedings of the Cambridge Philosophical Society 22 (4): 534–538. doi:10.1017/S0305004100003236. Bibcode1925PCPS...22..534W.
79. Moore, C. B.; Eack, K. B.; Aulich, G. D.; Rison, W. (2001). "Energetic radiation associated with lightning stepped-leaders". Geophysical Research Letters 28 (11): 2141. doi:10.1029/2001GL013140. Bibcode2001GeoRL..28.2141M.
80. Dwyer, J. R.; Uman, M. A.; Rassoul, H. K.; Al-Dayeh, M.; Caraway, L.; Jerauld, J.; Rakov, V. A.; Jordan, D. M. et al. (2003). "Energetic Radiation Produced During Rocket-Triggered Lightning". Science 299 (5607): 694–697. doi:10.1126/science.1078940. PMID 12560549. Bibcode2003Sci...299..694D. Retrieved August 28, 2015.
81. Newitz, A. (September 2007) "Educated Destruction 101", Popular Science, p. 61.
82. Scientists close in on source of X-rays in lightning , Physorg.com, July 15, 2008. Retrieved July 2008.
83. Prostak, Sergio (April 11, 2013). "Scientists Explain Invisible 'Dark Lightning'".
84. Signature Of Antimatter Detected In Lightning – Science News . Sciencenews.org (December 5, 2009). Retrieved on June 23, 2012.
85. Köhn, C.; Ebert, U. (2015). "Calculation of beams of positrons, neutrons and protons associated with terrestrial gamma-ray flashes". J. Geophys. Res. Atmos. 23 (4): 1620–1635. doi:10.1002/2014JD022229. Bibcode2015JGRD..120.1620K.
86. Köhn, C.; Diniz, G.; Harakeh, Muhsin (2017). "Production mechanisms of leptons, photons, and hadrons and their possible feedback close to lightning leaders". J. Geophys. Res. Atmos. 122 (2): 1365–1383. doi:10.1002/2016JD025445. PMID 28357174. Bibcode2017JGRD..122.1365K.
87. "Lightning's 'NOx-ious' Impact On Pollution, Climate". Science News. Retrieved 4 August 2018.
88. Pliny the Younger. "Pliny the Younger's Observations". "Behind us were frightening dark clouds, rent by lightning twisted and hurled, opening to reveal huge figures of flame."
89. Dell'Amore, Christine (February 3, 2010) New Lightning Type Found Over Volcano? . National Geographic News.
90. Anonymous (2020-03-27). "Q&A: Monitoring Volcanic Eruptions Using Lightning" (in en). Physics 13: 44. doi:10.1103/Physics.13.44. Bibcode2020PhyOJ..13...44..
91. Ceranic, Irena (28 November 2020). "Fire tornadoes and dry lightning are just the start of the nightmare when a bushfire creates its own storm". ABC News (Australian Broadcasting Corporation).
92. Strangeway, Robert J. (1995). "Plasma Wave Evidence for Lightning on Venus". Journal of Atmospheric and Terrestrial Physics 57 (5): 537–556. doi:10.1016/0021-9169(94)00080-8. Bibcode1995JATP...57..537S. Retrieved September 24, 2007.
93. Uman (1986) Ch. 4, pp. 26–34.
94. Colvin, J. D.; Mitchell, C. K.; Greig, J. R.; Murphy, D. P.; Pechacek, R. E.; Raleigh, M. (1987). "An empirical study of the nuclear explosion-induced lightning seen on IVY-MIKE". Journal of Geophysical Research 92 (D5): 5696–5712. doi:10.1029/JD092iD05p05696. Bibcode1987JGR....92.5696C.
95. Uman (1986) pp. 103–110
96. Fink, Micah. "How Lightning Forms". PBS.org. Public Broadcasting System.
97. National Weather Service (2007). "Lightning Safety". National Weather Service.
98. Rison, William; Krehbiel, Paul R.; Stock, Michael G.; Edens, Harald E.; Shao, Xuan-Min; Thomas, Ronald J.; Stanley, Mark A.; Zhang, Yang (2016-02-15). "Observations of narrow bipolar events reveal how lightning is initiated in thunderstorms" (in en). Nature Communications 7 (1): 10721. doi:10.1038/ncomms10721. ISSN 2041-1723. PMID 26876654. Bibcode2016NatCo...710721R.
99. Uman (1986) p. 61.
100. Rakov and Uman, p. 84.
101. Thomson, E. M.; Uman, M. A.; Beasley, W. H. (January 1985). "Speed and current for lightning stepped leaders near ground as determined from electric field records". Journal of Geophysical Research 90 (D5): 8136. doi:10.1029/JD090iD05p08136. Bibcode1985JGR....90.8136T.
102. The Franklin Institute. Ben Franklin's Lightning Bells . Retrieved December 14, 2008.
103.   NOAA page on how the U.S. national lightning detection system operates
104.   Real-time map of lightning discharges in U.S.
105. Volland, H. (ed) (1995) Handbook of Atmospheric Electrodynamics, CRC Press, Boca Raton, ISBN:0849386470.
106. "NASA Dataset Information". NASA. 2007.
107. Sima, Richard (March 13, 2020). "Mapping Lightning Strikes from Space". Eos.
108. Bruning, Eric C.; Tillier, Clemens E.; Edgington, Samantha F.; Rudlosky, Scott D.; Zajic, Joe; Gravelle, Chad; Foster, Matt; Calhoun, Kristin M. et al. (2019). "Meteorological Imagery for the Geostationary Lightning Mapper" (in en). Journal of Geophysical Research: Atmospheres 124 (24): 14285–14309. doi:10.1029/2019JD030874. ISSN 2169-8996. Bibcode2019JGRD..12414285B.
109. Kridler, Chris (July 25, 2002). "Triggered lightning video" (video). requires QuickTime. Chris Kridler's Sky Diary.
110. "UNM researchers use lasers to guide lightning". Campus News, The University of New Mexico. January 29, 2001.
111. Khan, N.; Mariun, N.; Aris, I.; Yeak, J. (2002). "Laser-triggered lightning discharge". New Journal of Physics 4 (1): 61. doi:10.1088/1367-2630/4/1/361. Bibcode2002NJPh....4...61K.
112. Rambo, P.; Biegert, J.; Kubecek, V.; Schwarz, J.; Bernstein, A.; Diels, J.-C.; Bernstein, R.; Stahlkopf, K. (1999). "Laboratory tests of laser-induced lightning discharge". Journal of Optical Technology 66 (3): 194–198. doi:10.1364/JOT.66.000194. Bibcode1999JOptT..66..194R.
113. Ackermann, R.; Stelmaszczyk, K.; Rohwetter, P.; MéJean, G.; Salmon, E.; Yu, J.; Kasparian, J.; MéChain, G. et al. (2004). "Triggering and guiding of megavolt discharges by laser-induced filaments under rain conditions". Applied Physics Letters 85 (23): 5781. doi:10.1063/1.1829165. Bibcode2004ApPhL..85.5781A.
114. Wang, D.; Ushio, T.; Kawasaki, Z. -I.; Matsuura, K.; Shimada, Y.; Uchida, S.; Yamanaka, C.; Izawa, Y. et al. (1995). "A possible way to trigger lightning using a laser". Journal of Atmospheric and Terrestrial Physics 57 (5): 459. doi:10.1016/0021-9169(94)00073-W. Bibcode1995JATP...57..459W.
115.   News report based on: Kasparian, J.; Ackermann, R.; André, Y. B.; Méchain, G. G.; Méjean, G.; Prade, B.; Rohwetter, P.; Salmon, E. et al. (2008). "Electric events synchronized with laser filaments in thunderclouds". Optics Express 16 (8): 5757–63. doi:10.1364/OE.16.005757. PMID 18542684. Bibcode2008OExpr..16.5757K.
116.   News report based on Kasparian et al., pp. 5757–5763
117. Graham, K.W.T. (1961). "The Re-magnetization of a Surface Outcrop by Lightning Currents". Geophysical Journal International 6 (1): 85. doi:10.1111/j.1365-246X.1961.tb02963.x. Bibcode1961GeoJ....6...85G.
118. Cox A. (1961). Anomalous Remanent Magnetization of Basalt . U.S. Geological Survey Bulletin 1038-E, pp. 131–160.
119. Bevan B. (1995). "Magnetic Surveys and Lightning". Near Surface Views (newsletter of the Near Surface Geophysics section of the Society of Exploration Geophysics). October 1995, pp. 7–8.
120. Wasilewski, Peter; Günther Kletetschka (1999). "Lodestone: Nature's only permanent magnet – What it is and how it gets charged". Geophysical Research Letters 26 (15): 2275–78. doi:10.1029/1999GL900496. Bibcode1999GeoRL..26.2275W. Retrieved July 13, 2009.
121. Sakai, H. S.; Sunada, S.; Sakurano, H. (1998). "Study of Lightning Current by Remanent Magnetization". Electrical Engineering in Japan 123 (4): 41–47. doi:10.1002/(SICI)1520-6416(199806)123:4<41::AID-EEJ6>3.0.CO;2-O.
122. Archaeo-Physics, LLC | Lightning-induced magnetic anomalies on archaeological sites . Archaeophysics.com. Retrieved on June 23, 2012.
123. Maki, David (2005). "Lightning strikes and prehistoric ovens: Determining the source of magnetic anomalies using techniques of environmental magnetism". Geoarchaeology 20 (5): 449–459. doi:10.1002/gea.20059. Retrieved November 1, 2017.
124. Verrier, V.; Rochette, P. (2002). "Estimating Peak Currents at Ground Lightning Impacts Using Remanent Magnetization". Geophysical Research Letters 29 (18): 1867. doi:10.1029/2002GL015207. Bibcode2002GeoRL..29.1867V.
125. Finney, D. L.; Marsham, J. H.; Wilkinson, J. M.; Field, P. R.; Blyth, A. M.; Jackson, L. S.; Kendon, E. J.; Tucker, S. O. et al. (2020). "African Lightning and its Relation to Rainfall and Climate Change in a Convection-Permitting Model" (in en). Geophysical Research Letters 47 (23): e2020GL088163. doi:10.1029/2020GL088163. ISSN 1944-8007. Bibcode2020GeoRL..4788163F.
126. Holzworth, R. H.; Brundell, J. B.; McCarthy, M. P.; Jacobson, A. R.; Rodger, C. J.; Anderson, T. S. (2021). "Lightning in the Arctic". Geophysical Research Letters 48 (7). doi:10.1029/2020GL091366. Bibcode2021GeoRL..4891366H.
127. Gomes, Chandima; Gomes, Ashen (2014). "Lightning; Gods and sciences". 2014 International Conference on Lightning Protection (ICLP). pp. 1909–1918. doi:10.1109/ICLP.2014.6973441. ISBN 978-1-4799-3544-4.
128. Uman (1986) Ch. 6, p. 47.
129. "Jesus actor struck by lightning". BBC News. October 23, 2003.
130. "Lightning". Phar Lap: Australia's wonder horse. Museum Victoria.
131. Picture of John Kaspar of the National States Rights Party speaking in front of the party’s lightning bolt flag (the flag was red, white, and blue) . Mauryk2.com (November 6, 2010). Retrieved on April 9, 2013.

### Bibliography

This article incorporates public domain material from the National Oceanic and Atmospheric Administration document "Understanding Lightning: Thunderstorm Electrification".