684:
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 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.
132:
1274:
1220:
176:
1298:
1239:
553:–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. The fallout 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
1258:
1316:
745:
distributed evenly through the volume (or with a 10–30% volume of inactive core for larger particles between 0.5–2 mm), and irregular-shaped particles formed at the edges of the fireball by fusion of soil particles, with activity deposited in a thin surface layer. The amount of large irregular particles is insignificant. Particles formed from detonations above, or in, the ocean, will contain short-lived radioactive sodium isotopes, and salts from the
740:
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
312:
723:. Particles larger than 1–2 micrometers are very spherical, corresponding to vaporized material condensing into droplets and then solidifying. The radioactivity is evenly distributed throughout the particle volume, making total activity of the particles linearly dependent on particle volume. About 80% of activity is present in more volatile elements, which condense only after the fireball cools to considerable degree. For example,
282:
20:
36:
534:
1315:
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the altitude they are carried to, determines the length of their stay in the atmosphere, as larger particles are subject to dry precipitation. Smaller particles can be also scavenged by precipitation, either from the moisture condensing in the cloud or from the cloud intersecting with a rain cloud. The fallout carried down by rain is known as
1023:, with the minimal neutron energy needed being about 5.9 MeV. Considerable amounts of neptunium-239 and uranium-237 are indicators of a fission-fusion-fission explosion. Minor amounts of uranium-240 are also formed, and capture of large numbers of neutrons by individual nuclei leads to formation of small but detectable amounts of higher
888:. Too many condensation nuclei actually inhibit condensation, as the particles compete for a relatively insufficient amount of water vapor. 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.
688:
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.
497:. However, if the cloud reaches the tropopause, it may spread against the wind, because its convection speed is higher than the ambient wind speed. At the tropopause, the cloud shape is roughly circular and spread out. The initial color of some radioactive clouds can be colored red or reddish-brown, due to presence of
297:. Without gravity, or without a thick atmosphere, the explosive's by-product gases would remain spherical. Nuclear weapons are usually detonated above the ground (not upon impact, because some of the energy would be dissipated by the ground motions), to maximize the effect of their spherically expanding fireball and
872:). The elements in the fireball are present as oxides, unless the temperature is above the decomposition temperature of a given oxide. Less refractory products condense on surfaces of solidified particles. Isotopes with gaseous precursors solidify on the surface of the particles as they are produced by decay.
633:
687:
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
191:
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
1053:
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
1014:
The most significant radiation sources are the fission products from the primary fission stage, and in the case of fission-fusion-fission weapons, from the fission of the fusion stage uranium tamper. Many more neutrons per unit of energy are released in a thermonuclear explosion in comparison with a
609:
A detonation significantly below ground level or deep below the water (for instance, a nuclear depth charge) does not produce a mushroom cloud, as the explosion causes the vaporization of a huge amount of earth or water, creating a bubble which then collapses in on itself; in the case of a less deep
1193:
around the stem. If the water droplets become sufficiently large, the cloud structure they form may become heavy enough to descend; in this way, a rising stem with a descending bell around it can be produced. Layering of humidity in the atmosphere, responsible for the appearance of the condensation
744:
minerals. The particle sizes do not depend on the yield but instead on the soil character, as they are based on individual grains of the soil or their clusters. Two types of particles are present, spherical, formed by complete vaporization-condensation or at least melting of the soil, with activity
739:
For ground and low-altitude bursts, the cloud contains 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.
598:
meters/kiloton. However, even at these burst altitudes, fallout may be formed by other mechanisms. Airbursts produce white, steamy stems, while surface bursts produce gray to brown stems because large amounts of dust, dirt, soil, and debris are sucked into the mushroom cloud. Surface bursts produce
1176:
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
695:
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
526:. 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
1131:
out to a significant distance from the fireball, surrounding the head of the forming mushroom cloud. This light is most easily visible at night or under conditions of weak daylight. The brightness of the glow decreases rapidly with elapsed time since the detonation, becoming only barely visible
727:
will have less time to condense and coalesce into larger particles, resulting in greater degree of mixing in the volume of air and smaller particles. The particles produced immediately after the burst are small, with 90% of the radioactivity present in particles smaller than 300 nanometers. These
691:
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. The
683:
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
653:
products from the weapon materials, air, and the ground debris form only a minor fraction. Neutron activation starts during the neutron burst at the instant of the blast, and the range of this neutron burst is limited by the absorption of the neutrons as they pass through the Earth's atmosphere.
1148:
causes a sudden rarefaction of the surrounding medium. This low pressure region causes an adiabatic drop in temperature, causing moisture in the air to condense in an outward moving shell surrounding the explosion. When the pressure and temperature return to normal, the Wilson cloud dissipates.
880:
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
648:
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
371:
gases changes shape due to atmospheric friction, and the surface of the fireball is cooled by energy radiation, turning from a sphere to a violently rotating spheroidal vortex. A Rayleigh–Taylor instability is formed as the cool air underneath initially pushes the bottom fireball gases into an
114:
that draws up a central column, possibly with smoke, debris, condensed water vapor, or a combination of these, to form the "mushroom stem". The mass of gas plus entrained moist air eventually reaches an altitude where it is no longer of lower density than the surrounding air; at this point, it
1198:. The same effect above the top of the cloud, where the expansion of the rising cloud pushes a layer of warm, humid, low-altitude air upwards into cold, high-altitude air, first causes the condensation of water vapour out of the air and then causes the resulting droplets to freeze, forming
372:
inverted cup shape. This causes turbulence and a vortex that sucks more air into the center, creating external afterwinds and further cooling the fireball. The speed of rotation slows as the fireball cools and may stop entirely during later phases. The vaporized parts of the weapon and
473:, 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.
273:" cloud, but a reporter present also spoke of "the mushroom, now the common symbol of the atomic age". Mushrooms have traditionally been associated both with life and death, food and poison, which made them a more powerful symbolic connection than, say, the "cauliflower" cloud.
875:
The largest and therefore 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
1160:
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
975:. The induced isotopes include cobalt-60, 57 and 58, iron-59 and 55, manganese-54, zinc-65, yttrium-88, and possibly nickel-58 and 62, niobium-63, holmium-165, iridium-191, and short-lived manganese-56, sodium-24, silicon-31, and aluminium-28.
577:, 41.4% of the fallout consisted of irregular opaque particles, slightly over 25% of particles with transparent and opaque areas, approximately 20% of microscopic marine organisms, and 2% of microscopic radioactive threads of unknown origin.
463:. 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 invisible cloud continues depositing fallout along its path.
668:, 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
1273:
1602:
593:
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
517:
is also formed. It is estimated that each megaton of yield produces about 5,000 tons of nitrogen oxides. A higher-yield detonation can carry the nitrogen oxides from the burst high enough in atmosphere to cause significant
920:, present a long-term hazard. Intense beta radiation from the fallout particles can cause beta burns to people and animals coming in contact with the fallout shortly after the blast. Ingested or inhaled particles cause an
443:. 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
676:; otherwise, its yield would have been 100 megatons with 51 megatons produced 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
614:. An underwater detonation near the surface may produce a pillar of water which collapses to form a cauliflower-like shape, which is easily mistaken for a mushroom cloud (such as in the well-known pictures of the
599:
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.
1329:
Dog nuclear test. The streamers of smoke seen to the left of the explosion at detonation are vertical smoke flares used to observe the shockwave from the explosion, and are unrelated to the mushroom cloud.
1050:, with half-lives of 33 seconds and 3 minutes. The noble gas nonreactivity and rapid diffusion is responsible for depletion of local fallout in Sr-90, and corresponding Sr-90 enrichment of remote fallout.
1219:
415:
event; this "popcorning effect" results in more soil being lofted into the stem of the mushroom cloud than would otherwise be the case if the device had been placed above a more typical surface or soil.
380:
vortex core becomes yellow, then dark red, then loses visible incandescence. With further cooling, the bulk of the cloud fills in as atmospheric moisture condenses. As the cloud ascends and cools, its
753:
is a very good solvent for metal oxides and scavenges small particles easily; explosions above silica-containing soils will produce particles with isotopes mixed through their volume. In contrast,
439:, virtually identical to those created by intense stratosphere-penetrating thunderstorms. Smaller-scale explosions penetrating the tropopause generate waves of higher frequency, classified as
308:
One way to analyze the motion, once the hot gas has cleared the ground sufficiently, is as a "spherical cap bubble", as this gives agreement between the rate of rise and observed diameter.
924:
of alpha and beta radiation, which may lead to long-term effects, including cancer. The neutron irradiation of the atmosphere produces a small amount of activation, mainly as long-lived
392:, overshooting a large volume of overdense air to greater altitudes than the final stabilization altitude. Significantly smaller fireballs produce clouds with buoyancy-governed ascent.
881:
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.
1599:
1238:
1213:
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.
1257:
123:
following a nuclear blast. The stabilization altitude depends strongly on the profiles of the temperature, dew point, and wind shear in the air at and above the starting altitude.
971:
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
692:
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.
396:
423:(the bottom of the region of strong static stability) the cloud tends to slow and spread out. If it contains sufficient energy, the central part may continue rising up into the
1169:, water vapour condenses out of the air, producing droplets of water, which become visible as a white cloud. In technical terms, the "Wilson cloud" is also an example of the
1149:
Scientists observing the
Operation Crossroads nuclear tests in 1946 at Bikini Atoll named that transitory cloud a "Wilson cloud" because of its visual similarity to a Wilson
602:
A detonation high above the ground may produce a mushroom cloud without a stem. A double mushroom, with two levels, can be formed under certain conditions. For example, the
1524:
644:
is forming in the middle due to intense updrafts of moist air, and the forming partial stem can be seen below. The cloud exhibits the reddish-brown hue of nitrogen oxides.
1297:
585:
With surface and near-surface air bursts, the amount of debris lofted into the air decreases rapidly with increasing burst altitude. At a burst altitude of approximately 7
728:
coagulate with stratospheric aerosols. Coagulation is more extensive in the troposphere, and, at ground level, most activity is present in particles between 300
840:) are not condensed at that temperature. Intermediate elements have their (or their oxides) boiling points close to the solidification temperature of the particles (
824:; these precipitate the fastest and at the time of particle solidification, at temperature of 1400 °C, are considered to be fully condensed. Volatile elements (
912:, which represent the bulk of activity. Within 24 hours after a burst, the fallout gamma radiation level drops 60 times. Longer-life radioisotopes, typically
1194:
rings as opposed to a spherical cloud, also influences the shape of the condensation artifacts along the stem of the mushroom cloud, as the updraft causes
1360:"MDZ-Reader | Band | Physikalischer Kinderfreund / Vieth, Gerhard Ulrich Anton | Physikalischer Kinderfreund / Vieth, Gerhard Ulrich Anton"
354:, the ascent stops, and the cloud starts flattening to the characteristic mushroom shape, usually aided by surface growth due to the decaying turbulence.
1525:
National
Research Council; Division on Engineering and Physical Sciences; Committee on the Effects of Nuclear Earth-Penetrator and Other Weapons (2005).
1974:
1434:
1097:, a Japanese fishing boat located outside of the predicted danger zone, was also affected. Strontium-90 found in worldwide fallout later led to the
152:
Although the term appears to have been coined in the early 1950s, mushroom clouds generated by explosions were being described centuries before the
493:
The shape of the cloud is influenced by the local atmospheric conditions and wind patterns. The fallout distribution is predominantly a downwind
664:. Fusion products are typically non-radioactive. The degree of radiation fallout production is therefore measured in kilotons of fission. The
1467:
1400:
640:
Charlie, yield 14 kilotons (at 143 m • kt ), during the initial phase of stem formation. The toroidal fireball is visible at the top, a
624:, two different distinct clouds. The amount of radiation vented into the atmosphere decreases rapidly with increasing detonation depth.
336:
1967:
293:
Mushroom clouds are formed by many sorts of large explosions under Earth's gravity, but they are best known for their appearance after
209:
imagines the first demonstration of an atomic weapon "clouds of steam from the boiling sea.. a gigantic mushroom of steam and debris".
40:
2008:
is a set of photographs by Kevin
Tieskoetter, showing fine mushroom cloud structures generated by burning lightbulb filaments in air
1481:
1864:
1794:
110:. The buoyant mass of gas rises rapidly, resulting in turbulent vortices curling downward around its edges, forming a temporary
1966:
3rd edn. Washington, D.C.: United States
Department of Defense and Energy Research and Development Administration, 1977. (esp.
606:
shot formed the first head from the blast, followed by another one generated by the heat from the hot, freshly formed crater.
459:
and other weapon debris aerosols, and are usually dispersed by the wind, though weather patterns (especially rain) can produce
1583:
707:
Particles from air bursts are smaller than 10–25 micrometers, usually in the submicrometer range. They are composed mostly of
1757:
1730:
1698:
1671:
1641:
1536:
1461:
1428:
1385:
1995:
1157:. Analysts of later nuclear bomb tests used the more general term "condensation cloud" in preference to "Wilson cloud".
131:
1900:
1827:
262:" out of the top of which came "a giant mushroom that increased the height of the pillar to a total of 45,000 feet".
161:
106:
Mushroom clouds result from the sudden formation of a large volume of lower-density gases at any altitude, causing a
1322:
258:, who accompanied one of the three aircraft that made the bombing run. He wrote of the bomb producing a "pillar of
1185:
of higher-humidity air, combined with the associated drop in pressure and temperature, leads to the formation of
1170:
736:. The coagulation offsets the fractionation processes at particle formation, evening out isotopic distribution.
324:
107:
1140:
Nuclear mushroom clouds are often accompanied by short-lived vapour clouds, known variously as "Wilson clouds",
301:. Immediately after the detonation, the fireball begins to rise into the air, acting on the same principle as a
1569:
1177:
the fireball may become stable, becoming rings around the rising stem. Higher-yield explosions cause intense
1153:; the cloud chamber uses condensation from a rapid pressure drop to mark the tracks of electrically charged
1961:
486:
1600:
Key Issues: Nuclear
Weapons: History: Pre Cold War: Manhattan Project: Trinity: Eyewitness Philip Morrison
367:
At the moment of a nuclear explosion, a fireball is formed. The ascending, roughly spherical mass of hot,
2005:
229:
192:
beneath it. Lichtenberg stated to have later observed somewhat similar clouds, but none as remarkable.
1280:
616:
451:, heating the cloud and driving it to yet higher altitudes. The heads of the clouds consist of highly
187:
In 1798, Gerhard Vieth published a detailed and illustrated account of a cloud in the neighborhood of
1326:
1182:
400:
384:
lessens, and its ascent slows. If the size of the fireball is comparable to the atmospheric density
2021:
1564:
Radioactive fallout after nuclear explosions and accidents, Volume 3, I. A. IzraÄ—l, Elsevier, 2002
319:
explosion at Bikini Atoll, March 1, 1954, showing multiple condensation rings and several ice caps.
139:
1449:
1304:
27:
from an eruption on April 21, 1990. The mushroom-shaped plume rose from avalanches of hot debris (
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677:
669:
637:
603:
456:
769:
285:
Inside a rising mushroom cloud: denser air rapidly forces itself into the bottom center of the
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1397:
513:, and atmospheric moisture. In the high-temperature, high-radiation environment of the blast,
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1720:
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1526:
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494:
479:, 20 seconds to 10 minutes, when the hot gases rise up and early large fallout is deposited.
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1909:
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1115:
The intense radiation in the first seconds after the blast may cause an observable aura of
1024:
988:
657:
546:
538:
377:
266:
175:
80:
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shape. When the detonation altitude is low enough, these afterwinds will draw in dirt and
8:
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1003:
to the bomb casings, to allow identification of fallout produced by specific explosions.
885:
251:
244:
of London of 13 August 1945 as a "huge mushroom of smoke and dust". On 9 September 1945,
88:
60:
1913:
1019:
is a unique thermonuclear explosion marker, as it is produced by a (n,2n) reaction from
1162:
1154:
1141:
1094:
921:
650:
641:
485:, until about 2 days later, when the airborne particles are being distributed by wind,
246:
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84:
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at 300 hours, and after 100–300 days, the significant contributor becomes cobalt-60.
758:
611:
351:
294:
255:
196:
68:
1629:
1144:, or vapor rings. The "negative phase" following the positive overpressure behind a
1057:
Radioactive particles can be carried for considerable distances. Radiation from the
168:
exploding with a mushroom cloud after the
British defenders set it ablaze by firing
1999:
1954:
1921:
1917:
1580:
1120:
1110:
1046:. It diffuses easily in the cloud and undergoes two decays to rubidium-90 and then
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590:
574:
527:
498:
444:
373:
259:
165:
28:
884:
The condensation of water droplets in the mushroom cloud depends on the amount of
1958:
1606:
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1418:
1404:
1165:. This reduction in air pressure causes cooling, and when the air cools past its
1000:
905:
889:
720:
712:
519:
460:
302:
120:
96:
1976:
Mechanisms by Which the
Atmosphere Adjusts to an Extremely Large Explosive Event
1015:
purely fission yield influencing the fission products composition. For example,
67:
resulting from a large explosion. The effect is most commonly associated with a
1090:
980:
661:
554:
550:
328:
200:
116:
1838:
1618:
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test). An underground detonation at low depth produces a mushroom cloud and a
389:
2015:
1929:
1248:
1229:
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932:-41. The elements most important for induced radioactivity for sea water are
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92:
24:
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562:
436:
428:
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385:
316:
224:
100:
76:
64:
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1016:
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1799:
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861:
849:
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773:
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327:
is formed, and air is drawn upwards and into the cloud (similar to the
298:
153:
72:
1181:, where air speeds can reach 300 miles per hour (480 km/h). The
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311:
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fireball, which turbulently mixes into the familiar cloud appearance.
211:
1749:
Waging
Nuclear Peace: The Technology and Politics of Nuclear Weapons
545:
The distribution of radiation in the mushroom cloud varies with the
250:
published an eyewitness account of the
Nagasaki bombing, written by
1989:
1128:
1066:
1004:
992:
976:
937:
841:
741:
506:
381:
237:
216:
157:
56:
44:
339:", while, inside the head of the cloud, the hot gases rotate in a
1630:
Thomas Carlyle Jones; Ronald Duncan Hunt; Norval W. King (1997).
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1082:
1032:
1008:
996:
984:
953:
945:
865:
857:
837:
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781:
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contained in the cloud consists of the nuclear fission products;
399:
The evolution of a nuclear mushroom cloud; 19 kt at 120 m • kt .
332:
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19:
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933:
845:
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510:
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136:
Vue du siège de Gibraltar et explosion des batteries flottantes
35:
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from the ground below to form the stem of the mushroom cloud.
79:
will produce a similar effect. They can be caused by powerful
929:
829:
817:
754:
514:
220:
215:
published a report on 1 October 1937 of a Japanese attack on
188:
142:
and the Explosion of the Floating Batteries, artist unknown,
1206:), similar in both appearance and mechanism of formation to
733:
533:
1908:(3). Educational Foundation for Nuclear Science, Inc.: 74.
961:
892:
influences the propagation of fallout radioisotopes in the
1970:
and "Description of Air and Surface Bursts" in Chapter II)
1722:
A Nuclear Winter's Tale: Science and Politics in the 1980s
1609:. Nuclearfiles.org (1945-07-16). Retrieved on 2010-02-08.
1232:
test, showing multiple condensation rings, March 1, 1954.
1267:
hydrogen bomb test, showing multiple condensation rings.
761:, tends to adsorb radioactive particles on its surface.
565:
test had the appearance of white dust and was nicknamed
466:
A mushroom cloud undergoes several phases of formation.
1998:
has many photographs of nuclear tests conducted at the
1828:"The Night the World Changed: The Trinity Nuclear Test"
1686:
435:
to the stratosphere leads to the formation of acoustic
1423:. Cambridge, Massachusetts: Harvard University Press.
1011:-109, and cadmium-113m are also mentioned as tracers.
561:
on the backs of exposed animals. The fallout from the
1528:
Effects of Nuclear Earth-Penetrator and Other Weapons
223:, that generated "a great mushroom of smoke". During
126:
1590:. Nuclearweaponarchive.org. Retrieved on 2010-02-08.
580:
179:
Mushroom cloud in an engraving from Gerhard Vieth's
31:) that cascaded down the north flank of the volcano.
704:if absorbed into already formed falling raindrops.
1659:
1407:hiroshima-remembered.com. Retrieved on 2010-08-09.
768:during particle formation, due to their different
948:. For ground bursts, the elements of concern are
2013:
1447:
1069:. This was deduced, and the origin traced, when
16:Cloud of debris and smoke from a large explosion
1718:
1663:Under the Cloud: The Decades of Nuclear Testing
1398:Eyewitness Account of Atomic Bomb Over Nagasaki
660:produce a significant part of their yield from
573:, stuck to surfaces, and had a salty taste. In
269:nuclear bomb tests were described as having a "
1745:
1416:
1085:. Unanticipated winds carried lethal doses of
376:cool into visible gases, forming a cloud; the
254:, the official newspaper correspondent of the
1655:
1653:
227:, the destruction of the Japanese battleship
1251:test, showing a prominent condensation ring.
979:-152 and 154 can be present, as well as two
1968:"Chronological development of an air-burst"
1456:. Cambridge University Press. p. 470.
1325:The formation of a mushroom cloud from the
557:, often presenting as discolored spots and
335:), producing strong air currents known as "
1714:
1712:
1710:
1650:
999:-188 were produced from elements added as
1619:The Mushroom Cloud, by Virginia L. Snitow
1560:
1558:
1556:
1554:
1552:
1550:
1548:
1038:One of the important fission products is
700:if scavenged during raincloud formation,
1531:. National Academies Press. p. 53.
1303:The mushroom cloud from the 225-kiloton
1263:The mushroom cloud from the 6.9-megaton
631:
532:
394:
350:After the mass of hot gases reaches its
310:
280:
174:
130:
63:of debris, smoke, and usually condensed
34:
18:
1992:has many photographs of mushroom clouds
1990:Carey Sublette's Nuclear Weapon Archive
1862:
1707:
1244:The mushroom cloud from the 11-megaton
1225:The mushroom cloud from the 15-megaton
1135:
610:underground explosion, this produces a
162:1782 Franco-Spanish attack on Gibraltar
2014:
1825:
1545:
1093:, forcing its evacuation. The crew of
357:
1893:
1279:The water column from the 21-kiloton
537:Mushroom cloud size as a function of
103:can produce natural mushroom clouds.
1511:
1509:
1507:
1307:test, showing a well-developed bell.
627:
1774:"Strontium limits in peace and war"
1450:"6.11, Large Gas Bubbles in Liquid"
1104:
431:. A mass of air ascending from the
407:soil is "popcorned" by the intense
199:produced a mushroom cloud. In 1930
164:shows one of the attacking force's
13:
569:; the tiny white flakes resembled
549:of the explosion, type of weapon,
127:Early accounts and origins of term
14:
2048:
1983:
1901:Bulletin of the Atomic Scientists
1803:. 28 October 1999. Archived from
1778:Bulletin of the Atomic Scientists
1504:
1454:An Introduction to Fluid Dynamics
1420:Nuclear Fear: A History of Images
1287:, showing a prominent, spherical
581:Differences with detonation types
489:, and scavenged by precipitation.
71:, but any sufficiently energetic
1942:Glasstone and Dolan 1977, p. 631
1863:Feynman, Richard (21 May 2005).
1687:Constantin Papastefanou (2008).
1636:. Wiley-Blackwell. p. 690.
1470:from the original on 2016-04-28.
1437:from the original on 2016-06-10.
1314:
1296:
1272:
1256:
1237:
1218:
899:
505:, formed from initially ionized
1948:
1936:
1887:
1865:"'This is how science is done'"
1856:
1826:Nobles, Ralph (December 2008).
1819:
1787:
1766:
1739:
1680:
1666:. Two-Sixty Press. p. 32.
1623:
1612:
1593:
1574:
388:, the whole cloud rise will be
1963:The Effects of Nuclear Weapons
1922:10.1080/00963402.1953.11457386
1518:
1474:
1441:
1410:
1391:
1370:
1352:
904:The primary fallout hazard is
362:
1:
1835:Los Alamos Historical Society
1772:Ralph E. Lapp (October 1956)
1581:Effects of Nuclear Explosions
1364:reader.digitale-sammlungen.de
1346:
1132:after a few tens of seconds.
1073:found x-ray films were being
711:, with smaller proportion of
143:
672:was made of lead instead of
477:Rise and stabilization phase
160:by an unknown artist of the
7:
1894:Borst, Lyle B. (Apr 1953).
1752:. SUNY Press. p. 175.
1660:Richard Lee Miller (1986).
1334:
1171:Prandtl–Glauert singularity
427:as an analog of a standard
325:Rayleigh–Taylor instability
236:The atomic bomb cloud over
233:produced a mushroom cloud.
181:Physikalischer Kinderfreund
108:Rayleigh–Taylor instability
47:, Japan, on August 9, 1945.
10:
2053:
1376:Reynolds, Clark G (1982).
1283:test, involving a nuclear
1108:
1081:packaging produced in the
276:
240:, Japan, was described in
1725:. MIT Press. p. 25.
1448:Batchelor, G. K. (2000).
455:particles, primarily the
1719:Lawrence Badash (2009).
1693:. Elsevier. p. 41.
1515:Glasstone and Dolan 1977
636:The mushroom cloud from
411:of light emitted by the
39:Mushroom cloud from the
1795:"The Legacy of Trinity"
1746:Robert Ehrlich (1985).
1417:Weart, Spencer (1987).
1121:blue-violet-purple glow
1099:Partial Test Ban Treaty
413:prompt supercriticality
1996:DOE Nevada Site Office
995:-185, 181 and 187 and
645:
542:
416:
320:
290:
184:
149:
48:
32:
1896:"Nevada Weapons Test"
1025:transuranium elements
764:The elements undergo
658:Thermonuclear weapons
635:
536:
398:
314:
284:
178:
134:
38:
23:Ascending cloud from
22:
1875:on February 16, 2009
1690:Radioactive Aerosols
1633:Veterinary Pathology
1482:"The Mushroom Cloud"
1285:underwater explosion
1136:Condensation effects
1061:was washed out by a
487:deposited by gravity
267:Operation Crossroads
81:conventional weapons
1914:1953BuAtS...9c..73B
1844:on 28 December 2010
1380:. Time-Life Books.
1155:subatomic particles
1142:condensation clouds
886:condensation nuclei
678:nuclear weapon test
604:Buster-Jangle Sugar
419:After reaching the
401:Tumbler-Snapper Dog
358:Nuclear detonations
295:nuclear detonations
252:William L. Laurence
119:, which results in
85:thermobaric weapons
61:flammagenitus cloud
1784:(8): 287–289, 320.
1605:2014-07-21 at the
1586:2014-04-28 at the
1403:2011-01-06 at the
1095:Daigo Fukuryu Maru
989:Operation Hardtack
651:neutron activation
646:
642:condensation cloud
589:meters/kiloton, a
543:
417:
321:
291:
247:The New York Times
206:Last and First Men
185:
166:floating batteries
150:
140:Siege of Gibraltar
117:drifting back down
97:volcanic eruptions
49:
33:
1955:Glasstone, Samuel
1759:978-0-87395-919-3
1732:978-0-262-25799-2
1700:978-0-08-044075-0
1673:978-0-02-921620-0
1643:978-0-683-04481-2
1538:978-0-309-09673-7
1463:978-0-521-66396-0
1430:978-0-674-62836-6
1386:978-0-8094-3304-9
1341:Rope trick effect
1305:Greenhouse George
1173:in aerodynamics.
1089:fallout over the
987:-102. During the
973:nuclear reactions
908:from short-lived
759:calcium carbonate
757:debris, based on
628:Cloud composition
612:subsidence crater
352:equilibrium level
256:Manhattan Project
197:Halifax Explosion
156:. A contemporary
69:nuclear explosion
55:is a distinctive
29:pyroclastic flows
2044:
2000:Nevada Test Site
1973:Vigh, Jonathan.
1959:Dolan, Philip J.
1943:
1940:
1934:
1933:
1891:
1885:
1884:
1882:
1880:
1871:. Archived from
1860:
1854:
1853:
1851:
1849:
1843:
1837:. Archived from
1832:
1823:
1817:
1816:
1814:
1812:
1791:
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1770:
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1499:
1497:
1488:. Archived from
1478:
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1438:
1414:
1408:
1395:
1389:
1374:
1368:
1367:
1356:
1318:
1300:
1281:Crossroads Baker
1276:
1260:
1241:
1222:
1111:Ionized air glow
1105:Fluorescent glow
1042:, a radioactive
956:-31, sodium-24,
928:and short-lived
721:plutonium oxides
617:Crossroads Baker
597:
588:
575:Operation Wigwam
528:corona discharge
499:nitrogen dioxide
457:fission products
148:
145:
2052:
2051:
2047:
2046:
2045:
2043:
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2022:Nuclear weapons
2012:
2011:
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1607:Wayback Machine
1598:
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1588:Wayback Machine
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1405:Wayback Machine
1396:
1392:
1378:The Carrier War
1375:
1371:
1358:
1357:
1353:
1349:
1337:
1332:
1331:
1330:
1327:Tumbler-Snapper
1324:
1319:
1308:
1301:
1292:
1277:
1268:
1261:
1252:
1242:
1233:
1223:
1163:Bernoulli's Law
1138:
1113:
1107:
981:nuclear isomers
906:gamma radiation
902:
890:Bioaccumulation
713:aluminium oxide
630:
595:
586:
583:
461:nuclear fallout
365:
360:
323:As it rises, a
303:hot-air balloon
279:
146:
129:
25:Redoubt Volcano
17:
12:
11:
5:
2050:
2040:
2039:
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1984:External links
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1944:
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1109:Main article:
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1091:Rongelap Atoll
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822:boiling points
662:nuclear fusion
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626:
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364:
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201:Olaf Stapledon
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53:mushroom cloud
41:atomic bombing
15:
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2035:
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2007:
2006:Burning bulbs
2004:
2002:and elsewhere
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1807:on 9 May 2008
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1492:on 2013-08-30
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1071:Eastman Kodak
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910:radioisotopes
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900:Radioisotopes
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766:fractionation
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638:Buster-Jangle
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437:gravity waves
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405:Nevada desert
402:
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265:In 1946, the
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203:in his novel
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101:impact events
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93:GBU-43/B MOAB
90:
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78:
74:
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66:
62:
58:
54:
46:
42:
37:
30:
26:
21:
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1962:
1949:Bibliography
1938:
1905:
1899:
1889:
1877:. Retrieved
1873:the original
1869:Dimaggio.org
1868:
1858:
1846:. Retrieved
1839:the original
1834:
1821:
1809:. Retrieved
1805:the original
1798:
1789:
1781:
1777:
1768:
1748:
1741:
1721:
1689:
1682:
1662:
1632:
1625:
1614:
1595:
1576:
1527:
1520:
1494:. Retrieved
1490:the original
1485:
1476:
1453:
1443:
1419:
1412:
1393:
1377:
1372:
1363:
1354:
1289:Wilson cloud
1265:Castle Union
1246:Castle Romeo
1227:Castle Bravo
1212:
1208:scarf clouds
1203:
1199:
1196:laminar flow
1190:
1186:
1175:
1159:
1139:
1117:fluorescence
1114:
1087:Castle Bravo
1059:Trinity test
1056:
1052:
1048:strontium-90
1037:
1013:
970:
918:strontium-90
903:
883:
874:
763:
738:
725:strontium-90
706:
701:
697:
694:
690:
686:
682:
680:, combined.
656:
647:
615:
608:
601:
584:
566:
563:Castle Bravo
544:
492:
482:
476:
470:
465:
445:phase change
429:thunderstorm
425:stratosphere
418:
408:
403:. The sandy
386:scale height
369:incandescent
366:
349:
322:
317:Castle Bravo
307:
292:
264:
245:
241:
235:
228:
225:World War II
210:
204:
194:
186:
180:
151:
138:View of the
135:
105:
87:such as the
83:, including
77:deflagration
65:water vapour
52:
50:
2037:Cloud types
1848:15 February
1496:January 14,
1183:entrainment
1146:shock front
1123:of ionized
1029:einsteinium
1021:uranium-238
1017:uranium-237
914:caesium-137
732:and 1
709:iron oxides
674:uranium-238
567:Bikini snow
524:ozone layer
503:nitric acid
453:radioactive
449:latent heat
433:troposphere
374:ionized air
363:Description
315:15-megaton
271:cauliflower
260:purple fire
170:heated shot
147: 1782
115:disperses,
112:vortex ring
2032:Explosions
2016:Categories
1879:8 February
1811:8 February
1800:ABQjournal
1570:0080438555
1347:References
1040:krypton-90
878:half-lives
820:with high
776:elements (
774:Refractory
770:volatility
666:Tsar Bomba
622:base surge
571:snowflakes
555:beta burns
471:Early time
441:infrasound
421:tropopause
337:afterwinds
299:blast wave
154:Atomic Age
73:detonation
1930:0096-3402
1388:. p. 169.
1167:dew point
1079:cardboard
1063:rainstorm
1044:noble gas
1031:-255 and
966:cobalt-60
964:-59, and
958:manganese
950:aluminium
942:magnesium
926:carbon-14
894:biosphere
749:. Molten
747:sea water
520:depletion
483:Late time
447:releases
390:ballistic
378:white-hot
242:The Times
212:The Times
195:The 1917
2027:Vortices
1603:Archived
1584:Archived
1468:Archived
1435:Archived
1401:Archived
1335:See also
1200:ice caps
1179:updrafts
1129:nitrogen
1067:Illinois
1005:Antimony
993:tungsten
977:Europium
938:chlorine
742:silicate
698:rain-out
507:nitrogen
382:buoyancy
341:toroidal
287:toroidal
238:Nagasaki
217:Shanghai
158:aquatint
59:-shaped
57:mushroom
45:Nagasaki
1979:, 2001.
1910:Bibcode
1204:icecaps
1083:Midwest
1033:fermium
1027:, e.g.
1009:cadmium
1001:tracers
997:rhenium
985:rhodium
954:silicon
946:bromine
816:) form
717:uranium
702:washout
559:lesions
522:of the
333:chimney
329:updraft
277:Physics
121:fallout
95:. Some
1957:, and
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1125:oxygen
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1075:fogged
1035:-255.
1007:-124,
944:, and
934:sodium
818:oxides
751:silica
715:, and
670:tamper
596:
591:crater
587:
551:fusion
511:oxygen
345:debris
230:Yamato
183:(1798)
1842:(PDF)
1831:(PDF)
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960:-56,
952:-28,
936:-24,
930:argon
755:coral
547:yield
539:yield
515:ozone
495:plume
409:flash
331:of a
221:China
189:Gotha
89:ATBIP
1926:ISSN
1881:2010
1850:2019
1813:2010
1754:ISBN
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1498:2018
1458:ISBN
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1127:and
962:iron
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850:Mo
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846:Cs
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842:Rb
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830:Xe
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826:Kr
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