Mushroom cloud
A mushroom cloud is a distinctive
Mushroom clouds result from the sudden formation of a large volume of lower-density gases at any altitude, causing a
Early accounts and origins of term
Although the term appears to have been coined in the early 1950s, mushroom clouds generated by explosions were being described centuries before the
A contemporary aquatint by an unknown artist of the 1782 Franco-Spanish attack on Gibraltar shows one of the attacking force's floating batteries exploding with a mushroom cloud after the British defenders set it ablaze by firing heated shot.
In 1798, Gerhard Vieth published a detailed and illustrated account of a cloud in the neighborhood of Gotha that was "not unlike a mushroom in shape". The cloud had been observed by legation counselor Lichtenberg a few years earlier on a warm summer afternoon. It was interpreted as an irregular meteorological cloud and seemed to have caused a storm with rain and thunder from a new dark cloud that developed beneath it. Lichtenberg stated to have later observed somewhat similar clouds, but none as remarkable.[1]
The 1917 Halifax Explosion produced a mushroom cloud.
In 1930 Olaf Stapledon in his novel Last and First Men imagines the first demonstration of an atomic weapon "clouds of steam from the boiling sea.. a gigantic mushroom of steam and debris".
The Times published a report on 1 October 1937 of a Japanese attack on Shanghai, China, that generated "a great mushroom of smoke".
During World War II, the destruction of the Japanese battleship Yamato produced a mushroom cloud.[2]
The atomic bomb cloud over
In 1946, the
Physics
Mushroom clouds are formed by many sorts of large explosions under Earth's gravity, but they are best known for their appearance after
One way to analyze the motion, once the hot gas has cleared the ground sufficiently, is as a "spherical cap bubble",[5] as this gives agreement between the rate of rise and observed diameter.
As it rises, a
After the mass of hot gases reaches its equilibrium level, the ascent stops, and the cloud starts flattening to the characteristic mushroom shape, usually aided by surface growth due to the decaying turbulence.
Nuclear mushroom clouds
Nuclear detonations produced high above the ground might not create mushroom clouds with a stem. The heads of the clouds themselves consist of highly
Detonations significantly below ground level or deep below the water (for instance, nuclear depth charges) also do not produce mushroom clouds, as the explosion causes the vaporization of a huge amount of earth and water in these instances, creating a bubble which then collapses in on itself; in the case of a less deep underground explosion, this produces a
With surface and near-surface air bursts, the amount of debris lofted into the air decreases rapidly with increasing burst altitude. At burst altitudes of approximately 7 meters/kiloton1⁄3, a crater is not formed, and correspondingly lower amounts of dust and debris are produced. The fallout-reducing height, above which the primary radioactive particles consist mainly of the fine fireball condensation, is approximately 55 meters/kiloton0.4.[6] However, even at these burst altitudes, fallout may be formed by a number of mechanisms.
The distribution of radiation in the mushroom cloud varies with the yield of the explosion, type of weapon, fusion–fission ratio, burst altitude, terrain type, and weather. In general, lower-yield explosions have about 90% of their radioactivity in the mushroom head and 10% in the stem. In contrast, megaton-range explosions tend to have most of their radioactivity in the lower third of the mushroom cloud.[8]
At the moment of the explosion, the fireball is formed. The ascending, roughly spherical mass of hot,
If the size of the fireball is comparable to the atmospheric density scale height, the whole cloud rise will be ballistic, overshooting a large volume of overdense air to greater altitudes than the final stabilization altitude. Significantly smaller fireballs produce clouds with buoyancy-governed ascent.
After reaching the tropopause, the bottom of the region of strong static stability, the cloud tends to slow its ascent and spread out. If it contains sufficient energy, the central part of it may continue rising up into the stratosphere as an analog of a standard thunderstorm.[9] A mass of air ascending from the troposphere to the stratosphere leads to the formation of acoustic gravity waves, virtually identical to those created by intense stratosphere-penetrating thunderstorms. Smaller-scale explosions penetrating the tropopause generate waves of higher frequency, classified as infrasound.
The explosion raises a large amount of moisture-laden air from lower altitudes. As the air rises, its temperature drops, and its water vapour first condenses as water droplets, and later freezes as ice crystals. The phase changes release latent heat, heating the cloud and driving it to yet higher altitudes.
A mushroom cloud undergoes several phases of formation.[10]
- Early time, the first ≈20 seconds, when the fireball forms and the fission products mix with the material aspired from the ground or ejected from the crater. The condensation of evaporated ground occurs in first few seconds, most intensely during fireball temperatures between 3500 and 4100 K.[11]
- Rise and stabilization phase, 20 seconds to 10 minutes, when the hot gases rise up and early large fallout is deposited.
- Late time, until about 2 days later, when the airborne particles are being distributed by wind, deposited by gravity, and scavenged by precipitation.
The shape of the cloud is influenced by the local atmospheric conditions and wind patterns. The fallout distribution is predominantly a downwind
The initial color of some radioactive clouds can be colored red or reddish-brown, due to presence of nitrogen dioxide and nitric acid, formed from initially ionized nitrogen, oxygen, and atmospheric moisture. In the high-temperature, high-radiation environment of the blast, ozone is also formed. It is estimated that each megaton of yield produces about 5000 tons of nitrogen oxides.[12] Yellow and orange hues have also been described. This reddish hue is later obscured by the white colour of water/ice clouds, condensing out of the fast-flowing air as the fireball cools, and the dark colour of smoke and debris sucked into the updraft. The ozone gives the blast its characteristic corona discharge-like smell.[13]
The droplets of condensed water gradually evaporate, leading to the cloud's apparent disappearance. The radioactive particles, however, remain suspended in the air, and the now-invisible cloud continues depositing fallout along its path.
Airbursts produce white, steamy stems, while groundbursts produce gray to brown stems as large amounts of dust, dirt, soil, and debris are sucked into the mushroom cloud. Groundbursts produce dark mushroom clouds containing irradiated material from the ground in addition to the bomb and its casing, and therefore produce more radioactive fallout, with larger particles that readily deposit locally.
A higher-yield detonation can carry the nitrogen oxides from the burst high enough in atmosphere to cause significant depletion of the ozone layer.
A double mushroom, with two levels, can be formed under certain conditions. For example, the
The fallout itself may appear as dry, ash-like flakes, or as particles too small to be visible; in the latter case, the particles are often deposited by rain. Large amounts of newer, more radioactive particles deposited on skin can cause
Cloud composition
The cloud contains three main classes of material: the remains of the weapon and its fission products, the material acquired from the ground (only significant for burst altitudes below the fallout-reducing altitude, which depends on the weapon yield), and water vapour. The bulk of the radiation contained in the cloud consists of the
Most of the radiation is created by the fission products. Thermonuclear weapons produce a significant part of their yield from nuclear fusion. Fusion products are typically non-radioactive. The degree of radiation fallout production is therefore measured in kilotons of fission. The Tsar Bomba, which produced 97% of its 50-megaton yield from fusion, was a very clean weapon compared to what would typically be expected of a weapon of its yield (although it still produced 1.5 megatons of its yield from fission), as its fusion tamper was made of lead instead of uranium-238; otherwise, its yield would have been 100 megatons with 51 of those from fission. Were it to be detonated at or near the surface, its fallout would comprise fully one-quarter of all the fallout from every nuclear weapon test, combined.
Initially, the fireball contains a highly ionized plasma consisting only of atoms of the weapon, its fission products, and atmospheric gases of adjacent air. As the plasma cools, the atoms react, forming fine droplets and then solid particles of oxides. The particles coalesce to larger ones, and deposit on surface of other particles. Larger particles usually originate from material aspired into the cloud. Particles aspired while the cloud is still hot enough to melt them mix with the fission products throughout their volume. Larger particles get molten radioactive materials deposited on their surface. Particles aspired into the cloud later, when its temperature is low enough, do not become significantly contaminated. Particles formed only from the weapon itself are fine enough to stay airborne for a long time and become widely dispersed and diluted to non-hazardous levels. Higher-altitude blasts which do not aspire ground debris, or which aspire dust only after cooling enough and where the radioactive fraction of the particles is therefore small, cause a much smaller degree of localized fallout than lower-altitude blasts with larger radioactive particles formed.
The concentration of condensation products is the same for the small particles and for the deposited surface layers of larger particles. About 100 kg of small particles are formed per kiloton of yield. The volume, and therefore activity, of the small particles is almost three orders of magnitude lower than the volume of the deposited surface layers on larger particles.
For higher-altitude blasts, the primary particle forming processes are condensation and subsequent coagulation. For lower-altitude and ground blasts, with involvement of soil particles, the primary process is deposition on the foreign particles.
A low-altitude detonation produces a cloud with a dust loading of 100 tons per megaton of yield. A ground detonation produces clouds with about three times as much dust. For a ground detonation, approximately 200 tons of soil per kiloton of yield is melted and comes in contact with radiation.[11]
The fireball volume is the same for a surface or an atmospheric detonation. In the first case, the fireball is a hemisphere instead of a sphere, with a correspondingly larger radius.[11]
The particle sizes range from submicrometer- and micrometer-sized (created by condensation of plasma in the fireball), through 10–500 micrometers (surface material agitated by the blast wave and raised by the afterwinds), to millimeter and above (crater ejecta). The size of particles together with the altitude they are carried to, determines the length of their stay in the atmosphere, as larger particles are subject to
Particles from air bursts are smaller than 10–25 micrometers, usually in the submicrometer range. They are composed mostly of
For ground and low-altitude bursts, the cloud contains also vaporized, melted and fused soil particles. The distribution of activity through the particles depends on their formation. Particles formed by vaporization-condensation have activity evenly distributed through volume as the air-burst particles. Larger molten particles have the fission products diffused through the outer layers, and fused and non-melted particles that were not heated sufficiently but came in contact with the vaporized material or scavenged droplets before their solidification have a relatively thin layer of high activity material deposited on their surface. The composition of such particles depends on the character of the soil, usually a glass-like material formed from
The elements undergo
The largest, and therefore the most radioactive particles, are deposited by fallout in the first few hours after the blast. Smaller particles are carried to higher altitudes and descend more slowly, reaching ground in a less radioactive state as the isotopes with the shortest half-lives decay the fastest. The smallest particles can reach the stratosphere and stay there for weeks, months, or even years, and cover an entire hemisphere of the planet via atmospheric currents. The higher danger, short-term, localized fallout is deposited primarily downwind from the blast site, in a cigar-shaped area, assuming a wind of constant strength and direction. Crosswinds, changes in wind direction, and precipitation are factors that can greatly alter the fallout pattern.[18]
The condensation of water droplets in the mushroom cloud depends on the amount of
Chemical reactivity of the elements and their oxides, ion adsorption properties, and compound solubility influence particle distribution in the environment after deposition from the atmosphere. Bioaccumulation influences the propagation of fallout radioisotopes in the biosphere.
Radioisotopes
The primary fallout hazard is
The neutron irradiation of the atmosphere itself produces a small amount of activation, mainly as long-lived carbon-14 and short-lived argon-41. The elements most important for induced radioactivity for sea water are sodium-24, chlorine, magnesium, and bromine. For ground bursts, the elements of concern are aluminium-28, silicon-31, sodium-24, manganese-56, iron-59, and cobalt-60.
The bomb casing can be a significant sources of neutron-activated radioisotopes. The neutron flux in the bombs, especially thermonuclear devices, is sufficient for high-threshold
The most significant radiation sources are the
One of the important fission products is
The radioactivity of the particles decreases with time, with different isotopes being significant at different timespans. For soil activation products, aluminium-28 is the most important contributor during the first 15 minutes. Manganese-56 and sodium-24 follow until about 200 hours. Iron-59 follows at 300 hours, and after 100–300 days, the significant contributor becomes cobalt-60.
Radioactive particles can be carried for considerable distances. Radiation from the
Fluorescent glow
The intense radiation in the first seconds after the blast may cause an observable aura of
Condensation effects
Nuclear mushroom clouds are often accompanied by short-lived vapour clouds, known variously as "
The same kind of condensation is sometimes seen above the wings of jet aircraft at low altitude in high-humidity conditions. The top of a wing is a curved surface. The curvature (and increased air velocity) causes a reduction in air pressure, as given by
The shape of the shock wave is influenced by variation of the speed of sound with altitude, and the temperature and humidity of different atmospheric layers determines the appearance of the Wilson clouds. Condensation rings around or above the fireball are a commonly observed feature. Rings around the fireball may become stable, becoming rings around the rising stem. Higher-yield explosions cause intense
The resulting composite structures can become very complex. The Castle Bravo cloud had, at various phases of its development, 4 condensation rings, 3 ice caps, 2 skirts, and 3 bells.
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The mushroom cloud from the 15-megatonhydrogen bombtest, showing multiple condensation rings, March 1, 1954.
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The mushroom cloud from the 11-megatonhydrogen bombtest, showing a prominent condensation ring.
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The mushroom cloud from the 6.9-megaton Castle Union hydrogen bomb test, showing multiple condensation rings.
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The water column from the 21-kilotonWilson cloud.
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The mushroom cloud from the 225-kiloton Greenhouse George test, showing a well-developed bell.
See also
References
- ^ "MDZ-Reader | Band | Physikalischer Kinderfreund / Vieth, Gerhard Ulrich Anton | Physikalischer Kinderfreund / Vieth, Gerhard Ulrich Anton". reader.digitale-sammlungen.de.
- ISBN 978-0-8094-3304-9. p. 169.
- ^ Eyewitness Account of Atomic Bomb Over Nagasaki Archived 2011-01-06 at the Wayback Machine hiroshima-remembered.com. Retrieved on 2010-08-09.
- ISBN 978-0-674-62836-6. Archivedfrom the original on 2016-06-10.
- ISBN 978-0-521-66396-0. Archivedfrom the original on 2016-04-28.
- ^ a b c Glasstone and Dolan 1977
- ^ The Mushroom Cloud, by Virginia L. Snitow
- ^ Full text of "Nuclear survival manual : BOSDEC-the concrete curtain". Archive.org. Retrieved on 2010-02-08.
- ^ "The Mushroom Cloud". Atomic Archive. Archived from the original on 2013-08-30. Retrieved January 14, 2018.
- ISBN 978-0-309-09673-7.
- ^ ISBN 0080438555
- ^ Effects of Nuclear Explosions Archived 2014-04-28 at the Wayback Machine. Nuclearweaponarchive.org. Retrieved on 2010-02-08.
- ^ Key Issues: Nuclear Weapons: History: Pre Cold War: Manhattan Project: Trinity: Eyewitness Philip Morrison Archived 2014-07-21 at the Wayback Machine. Nuclearfiles.org (1945-07-16). Retrieved on 2010-02-08.
- ^ ISBN 978-0-02-921620-0.
- ISBN 978-0-683-04481-2.
- ISBN 978-0-08-044075-0.
- ^ ISBN 978-0-262-25799-2.
- ISBN 978-0-87395-919-3.
- ^ Ralph E. Lapp (October 1956) "Strontium limits in peace and war", Bulletin of the Atomic Scientists, 12 (8): 287–289, 320.
- ABQjournal. 28 October 1999. Archived from the originalon 9 May 2008. Retrieved 8 February 2010.
- ^ Nobles, Ralph (December 2008). "The Night the World Changed: The Trinity Nuclear Test" (PDF). Los Alamos Historical Society. Archived from the original (PDF) on 28 December 2010. Retrieved 15 February 2019.
- ^ Feynman, Richard (21 May 2005). "'This is how science is done'". Dimaggio.org. Archived from the original on February 16, 2009. Retrieved 8 February 2010.
- ISSN 0096-3402.
- ^ Glasstone and Dolan 1977, p. 631
Bibliography
- Glasstone, Samuel, and Dolan, Philip J. The Effects of Nuclear Weapons[permanent dead link] 3rd edn. Washington, D.C.: United States Department of Defense and Energy Research and Development Administration, 1977. (esp. "Chronological development of an air-burst" and "Description of Air and Surface Bursts" in Chapter II)
- Vigh, Jonathan. Mechanisms by Which the Atmosphere Adjusts to an Extremely Large Explosive Event, 2001.
External links
- Carey Sublette's Nuclear Weapon Archive has many photographs of mushroom clouds
- DOE Nevada Site Office has many photographs of nuclear tests conducted at the Nevada Test Site and elsewhere
- Burning bulbs is a set of photographs by Kevin Tieskoetter, showing fine mushroom cloud structures generated by burning lightbulb filaments in air