home Drugs Testing a hydrogen bomb, aka “Kuzka’s mother”. The most powerful bomb in the world. Which bomb is stronger: vacuum or thermonuclear

Testing a hydrogen bomb, aka “Kuzka’s mother”. The most powerful bomb in the world. Which bomb is stronger: vacuum or thermonuclear

On October 30, 1961, the USSR exploded the most powerful bomb in world history: a 58-megaton hydrogen bomb (“Tsar Bomb”) was detonated at a test site on the island of Novaya Zemlya. Nikita Khrushchev joked that the original plan was to detonate a 100-megaton bomb, but the charge was reduced so as not to break all the glass in Moscow.

The explosion of AN602 was classified as a low air explosion of extremely high power. The results were impressive:

The fireball of the explosion reached a radius of approximately 4.6 kilometers. Theoretically, it could have grown to the surface of the earth, but this was prevented by the reflected shock wave, which crushed and threw the ball off the ground.
The light radiation could potentially cause third-degree burns at a distance of up to 100 kilometers.
Ionization of the atmosphere caused radio interference even hundreds of kilometers from the test site for about 40 minutes
The tangible seismic wave resulting from the explosion circled the globe three times.
Witnesses felt the impact and were able to describe the explosion thousands of kilometers away from its center.
The nuclear mushroom of the explosion rose to a height of 67 kilometers; the diameter of its two-tier “hat” reached (at the top tier) 95 kilometers.
The sound wave generated by the explosion reached Dikson Island at a distance of about 800 kilometers. However, sources do not report any destruction or damage to structures even in the urban-type village of Amderma and the village of Belushya Guba located much closer (280 km) to the test site.
Radioactive contamination of the experimental field with a radius of 2-3 km in the area of the epicenter was no more than 1 mR/hour; the testers appeared at the site of the epicenter 2 hours after the explosion. Radioactive contamination posed virtually no danger to test participants

All nuclear explosions carried out by countries of the world in one video:

The creator of the atomic bomb, Robert Oppenheimer, on the day of the first test of his brainchild said: “If hundreds of thousands of suns rose in the sky at once, their light could be compared with the radiance emanating from the Supreme Lord... I am Death, the great destroyer of the worlds, bringing death to all living things " These words were a quote from the Bhagavad Gita, which the American physicist read in the original.

Photographers from Lookout Mountain stand waist-deep in dust raised by the shock wave after a nuclear explosion (photo from 1953).

Challenge Name: Umbrella
Date: June 8, 1958

Power: 8 kilotons

An underwater nuclear explosion was carried out during Operation Hardtack. Decommissioned ships were used as targets.

Challenge Name: Chama (as part of Project Dominic)
Date: October 18, 1962
Location: Johnston Island
Power: 1.59 megatons

Challenge Name: Oak
Date: June 28, 1958
Location: Enewetak Lagoon in the Pacific Ocean
Yield: 8.9 megatons

Project Upshot Knothole, Annie Test. Date: March 17, 1953; project: Upshot Knothole; challenge: Annie; Location: Knothole, Nevada Test Site, Sector 4; power: 16 kt. (Photo: Wikicommons)

Challenge Name: Castle Bravo
Date: March 1, 1954
Location: Bikini Atoll
Explosion type: surface
Power: 15 megatons

The Castle Bravo hydrogen bomb was the most powerful explosion ever tested by the United States. The power of the explosion turned out to be much greater than the initial forecasts of 4-6 megatons.

Challenge Name: Castle Romeo
Date: March 26, 1954
Location: on a barge in Bravo Crater, Bikini Atoll
Explosion type: surface
Power: 11 megatons

The power of the explosion turned out to be 3 times greater than initial forecasts. Romeo was the first test carried out on a barge.

Project Dominic, Aztec Test

Challenge Name: Priscilla (as part of the "Plumbbob" challenge series)
Date: 1957

Yield: 37 kilotons

This is exactly what the process of releasing huge amounts of radiant and thermal energy looks like during an atomic explosion in the air over the desert. Here you can still see military equipment, which in a moment will be destroyed by the shock wave, captured in the form of a crown surrounding the epicenter of the explosion. You can see how the shock wave was reflected from the earth's surface and is about to merge with the fireball.

Challenge Name: Grable (as part of Operation Upshot Knothole)
Date: May 25, 1953
Location: Nevada Nuclear Test Site
Power: 15 kilotons

At a test site in the Nevada desert, photographers from the Lookout Mountain Center in 1953 took a photograph of an unusual phenomenon (a ring of fire in a nuclear mushroom after the explosion of a shell from a nuclear cannon), the nature of which has long occupied the minds of scientists.

Project Upshot Knothole, Rake test. This test involved an explosion of a 15 kiloton atomic bomb launched by a 280mm atomic cannon. The test took place on May 25, 1953 at the Nevada Test Site. (Photo: National Nuclear Security Administration/Nevada Site Office)

A mushroom cloud formed as a result of the atomic explosion of the Truckee test conducted as part of Project Dominic.

Project Buster, Test Dog.

Project Dominic, Yeso test. Test: Yeso; date: June 10, 1962; project: Dominic; location: 32 km south of Christmas Island; test type: B-52, atmospheric, height – 2.5 m; power: 3.0 mt; charge type: atomic. (Wikicommons)

Challenge Name: YESO
Date: June 10, 1962
Location: Christmas Island
Power: 3 megatons

Testing "Licorn" in French Polynesia. Image #1. (Pierre J./French Army)

Challenge name: “Unicorn” (French: Licorne)
Date: July 3, 1970
Location: Atoll in French Polynesia
Yield: 914 kilotons

Testing "Licorn" in French Polynesia. Image #2. (Photo: Pierre J./French Army)

Testing "Licorn" in French Polynesia. Image #3. (Photo: Pierre J./French Army)

To get good images, test sites often employ entire teams of photographers. Photo: nuclear test explosion in the Nevada desert. On the right are visible rocket plumes, with the help of which scientists determine the characteristics of the shock wave.

Testing "Licorn" in French Polynesia. Image #4. (Photo: Pierre J./French Army)

Project Castle, Romeo Test. (Photo: zvis.com)

Project Hardtack, Umbrella Test. Challenge: Umbrella; date: June 8, 1958; project: Hardtack I; location: Enewetak Atoll lagoon; test type: underwater, depth 45 m; power: 8kt; charge type: atomic.

Project Redwing, Test Seminole. (Photo: Nuclear Weapons Archive)

Riya test. Atmospheric test of an atomic bomb in French Polynesia in August 1971. As part of this test, which took place on August 14, 1971, a thermonuclear warhead codenamed "Riya" with a yield of 1000 kt was detonated. The explosion occurred on the territory of Mururoa Atoll. This photo was taken from a distance of 60 km from the zero mark. Photo: Pierre J.

A mushroom cloud from a nuclear explosion over Hiroshima (left) and Nagasaki (right). During the final stages of World War II, the United States launched two atomic bombs on Hiroshima and Nagasaki. The first explosion occurred on August 6, 1945, and the second on August 9, 1945. This was the only time nuclear weapons were used for military purposes. By order of President Truman, the US Army dropped the Little Boy nuclear bomb on Hiroshima on August 6, 1945, followed by the Fat Man nuclear bomb on Nagasaki on August 9. Within 2-4 months after the nuclear explosions, between 90,000 and 166,000 people died in Hiroshima, and between 60,000 and 80,000 in Nagasaki. (Photo: Wikicommons)

Upshot Knothole Project. Nevada Test Site, March 17, 1953. The blast wave completely destroyed Building No. 1, located at a distance of 1.05 km from the zero mark. The time difference between the first and second shot is 21/3 seconds. The camera was placed in a protective case with a wall thickness of 5 cm. The only light source in this case was a nuclear flash. (Photo: National Nuclear Security Administration/Nevada Site Office)

Project Ranger, 1951. The name of the test is unknown. (Photo: National Nuclear Security Administration/Nevada Site Office)

Trinity Test.

"Trinity" was the code name for the first nuclear weapons test. This test was conducted by the United States Army on July 16, 1945, at a site located approximately 56 km southeast of Socorro, New Mexico, at the White Sands Missile Range. The test used an implosion-type plutonium bomb, nicknamed “The Thing.” After detonation, an explosion occurred with a power equivalent to 20 kilotons of TNT. The date of this test is considered the beginning of the atomic era. (Photo: Wikicommons)

Challenge Name: Mike
Date: October 31, 1952
Location: Elugelab Island ("Flora"), Enewate Atoll
Power: 10.4 megatons

The device detonated during Mike's test, called the "sausage", was the first true megaton-class "hydrogen" bomb. The mushroom cloud reached a height of 41 km with a diameter of 96 km.

The MET bombing carried out as part of Operation Thipot. It is noteworthy that the MET explosion was comparable in power to the Fat Man plutonium bomb dropped on Nagasaki. April 15, 1955, 22 kt. (Wikimedia)

One of the most powerful explosions of a thermonuclear hydrogen bomb on the US account is Operation Castle Bravo. The charge power was 10 megatons. The explosion took place on March 1, 1954 at Bikini Atoll, Marshall Islands. (Wikimedia)

Operation Castle Romeo was one of the most powerful thermonuclear bomb explosions carried out by the United States. Bikini Atoll, March 27, 1954, 11 megatons. (Wikimedia)

Baker explosion, showing the white surface of the water disturbed by the air shock wave, and the top of the hollow column of spray that formed the hemispherical Wilson cloud. In the background is the shore of Bikini Atoll, July 1946. (Wikimedia)

The explosion of the American thermonuclear (hydrogen) bomb “Mike” with a power of 10.4 megatons. November 1, 1952. (Wikimedia)

Operation Greenhouse was the fifth series of American nuclear tests and the second of them in 1951. The operation tested nuclear warhead designs using nuclear fusion to increase energy output. In addition, the impact of the explosion on structures, including residential buildings, factory buildings and bunkers, was studied. The operation was carried out at the Pacific nuclear test site. All devices were detonated on high metal towers, simulating an air explosion. George explosion, 225 kilotons, May 9, 1951. (Wikimedia)

A mushroom cloud with a column of water instead of a dust stalk. To the right, a hole is visible on the pillar: the battleship Arkansas covered the emission of splashes. Baker test, charge power - 23 kilotons of TNT, July 25, 1946. (Wikimedia)

200 meter cloud over Frenchman Flat after the MET explosion as part of Operation Teapot, April 15, 1955, 22 kt. This projectile had a rare uranium-233 core. (Wikimedia)

The crater was formed when a 100-kiloton blast wave was blasted beneath 635 feet of desert on July 6, 1962, displacing 12 million tons of earth.

Time: 0s. Distance: 0m. Initiation of a nuclear detonator explosion.
Time: 0.0000001s. Distance: 0m Temperature: up to 100 million °C. The beginning and course of nuclear and thermonuclear reactions in a charge. With its explosion, a nuclear detonator creates conditions for the onset of thermonuclear reactions: the thermonuclear combustion zone passes through a shock wave in the charge substance at a speed of the order of 5000 km/s (106 - 107 m/s). About 90% of the neutrons released during the reactions are absorbed by the bomb substance, the remaining 10% are emitted out.

Time: 10−7c. Distance: 0m. Up to 80% or more of the energy of the reacting substance is transformed and released in the form of soft X-ray and hard UV radiation with enormous energy. The X-ray radiation generates a heat wave that heats the bomb, exits and begins to heat the surrounding air.

Time:< 10−7c. Расстояние: 2м Temperature: 30 million°C. The end of the reaction, the beginning of the dispersion of the bomb substance. The bomb immediately disappears from view and in its place a bright luminous sphere (fireball) appears, masking the dispersion of the charge. The growth rate of the sphere in the first meters is close to the speed of light. The density of the substance here drops to 1% of the density of the surrounding air in 0.01 seconds; the temperature drops to 7-8 thousand °C in 2.6 seconds, is held for ~5 seconds and further decreases with the rise of the fiery sphere; After 2-3 seconds the pressure drops to slightly below atmospheric pressure.

Time: 1.1x10−7s. Distance: 10m Temperature: 6 million°C. The expansion of the visible sphere to ~10 m occurs due to the glow of ionized air under X-ray radiation from nuclear reactions, and then through radiative diffusion of the heated air itself. The energy of radiation quanta leaving the thermonuclear charge is such that their free path before being captured by air particles is about 10 m and is initially comparable to the size of a sphere; photons quickly run around the entire sphere, averaging its temperature and fly out of it at the speed of light, ionizing more and more layers of air, hence the same temperature and near-light growth rate. Further, from capture to capture, photons lose energy and their travel distance is reduced, the growth of the sphere slows down.

Time: 1.4x10−7s. Distance: 16m Temperature: 4 million°C. In general, from 10−7 to 0.08 seconds, the 1st phase of the sphere’s glow occurs with a rapid drop in temperature and the release of ~1% of radiation energy, mostly in the form of UV rays and bright light radiation, which can damage the vision of a distant observer without education skin burns. The illumination of the earth's surface at these moments at distances of up to tens of kilometers can be a hundred or more times greater than the sun.

Time: 1.7x10−7s. Distance: 21m Temperature: 3 million°C. Bomb vapors in the form of clubs, dense clots and jets of plasma, like a piston, compress the air in front of them and form a shock wave inside the sphere - an internal shock wave, which differs from an ordinary shock wave in non-adiabatic, almost isothermal properties and at the same pressures several times higher density: shock-compressing the air immediately radiates most of the energy through the ball, which is still transparent to radiation.
In the first tens of meters, the surrounding objects, before the fire sphere hits them, due to its too high speed, do not have time to react in any way - they even practically do not heat up, and once inside the sphere under the flow of radiation they evaporate instantly.

Temperature: 2 million°C. Speed 1000 km/s. As the sphere grows and the temperature drops, the energy and flux density of photons decrease and their range (on the order of a meter) is no longer enough for near-light speeds of expansion of the fire front. The heated volume of air began to expand and a flow of its particles was formed from the center of the explosion. When the air is still at the boundary of the sphere, the heat wave slows down. The expanding heated air inside the sphere collides with the stationary air at its border and somewhere starting from 36-37 m a wave of increasing density appears - the future external air shock wave; Before this, the wave did not have time to appear due to the enormous growth rate of the light sphere.

Time: 0.000001s. Distance: 34m Temperature: 2 million°C. The internal shock and vapors of the bomb are located in a layer 8-12 m from the explosion site, the pressure peak is up to 17,000 MPa at a distance of 10.5 m, the density is ~ 4 times the density of air, the speed is ~ 100 km/s. Hot air region: pressure at the boundary 2,500 MPa, inside the region up to 5000 MPa, particle speed up to 16 km/s. The substance of the bomb vapor begins to lag behind the internals. jump as more and more air in it is drawn into motion. Dense clots and jets maintain speed.

Time: 0.000034s. Distance: 42m Temperature: 1 million°C. Conditions at the epicenter of the explosion of the first Soviet hydrogen bomb (400 kt at a height of 30 m), which created a crater about 50 m in diameter and 8 m deep. 15 m from the epicenter or 5-6 m from the base of the tower with a charge there was a reinforced concrete bunker with walls 2 m thick. For placing scientific equipment on top, covered with a large mound of earth 8 m thick, destroyed.

Temperature: 600 thousand °C. From this moment, the nature of the shock wave ceases to depend on the initial conditions of a nuclear explosion and approaches the typical one for a strong explosion in the air, i.e. Such wave parameters could be observed during the explosion of a large mass of conventional explosives.

Time: 0.0036s. Distance: 60m Temperature: 600 thousand°C. The internal shock, having passed the entire isothermal sphere, catches up and merges with the external one, increasing its density and forming the so-called. a strong shock is a single shock wave front. The density of matter in the sphere drops to 1/3 atmospheric.

Time: 0.014s. Distance: 110m Temperature: 400 thousand°C. A similar shock wave at the epicenter of the explosion of the first Soviet atomic bomb with a power of 22 kt at a height of 30 m generated a seismic shift that destroyed the imitation of metro tunnels with various types of fastening at depths of 10 and 20 m. 30 m, animals in the tunnels at depths of 10, 20 and 30 m died . An inconspicuous saucer-shaped depression with a diameter of about 100 m appeared on the surface. Similar conditions were at the epicenter of the Trinity explosion of 21 kt at an altitude of 30 m; a crater with a diameter of 80 m and a depth of 2 m was formed.

Time: 0.004s. Distance: 135m
Temperature: 300 thousand°C. The maximum height of the air explosion is 1 Mt to form a noticeable crater in the ground. The front of the shock wave is distorted by the impacts of bomb vapor clumps:

Time: 0.007s. Distance: 190m Temperature: 200 thousand°C. On a smooth and seemingly shiny front, the beat. waves form large blisters and bright spots (the sphere seems to be boiling). The density of matter in an isothermal sphere with a diameter of ~150 m drops below 10% of the atmospheric one.
Non-massive objects evaporate a few meters before the arrival of fire. spheres (“Rope tricks”); the human body on the side of the explosion will have time to char, and will completely evaporate with the arrival of the shock wave.

Time: 0.01s. Distance: 214m Temperature: 200 thousand°C. A similar air shock wave of the first Soviet atomic bomb at a distance of 60 m (52 m from the epicenter) destroyed the heads of the shafts leading into imitation subway tunnels under the epicenter (see above). Each head was a powerful reinforced concrete casemate, covered with a small earth embankment. The fragments of the heads fell into the trunks, the latter were then crushed by the seismic wave.

Time: 0.015s. Distance: 250m Temperature: 170 thousand°C. The shock wave greatly destroys rocks. The speed of the shock wave is higher than the speed of sound in metal: the theoretical limit of strength of the entrance door to the shelter; the tank flattens and burns.

Time: 0.028s. Distance: 320m Temperature: 110 thousand°C. The person is dispelled by a stream of plasma (shock wave speed = speed of sound in the bones, the body collapses into dust and immediately burns). Complete destruction of the most durable above-ground structures.

Time: 0.073s. Distance: 400m Temperature: 80 thousand°C. Irregularities on the sphere disappear. The density of the substance drops in the center to almost 1%, and at the edge of the isotherms. spheres with a diameter of ~320 m to 2% atmospheric. At this distance, within 1.5 s, heating to 30,000 °C and dropping to 7000 °C, ~5 s holding at a level of ~6,500 °C and decreasing the temperature in 10-20 s as the fireball moves upward.

Time: 0.079s. Distance: 435m Temperature: 110 thousand°C. Complete destruction of highways with asphalt and concrete surfaces. Temperature minimum of shock wave radiation, end of the 1st phase of glow. A metro-type shelter, lined with cast iron tubes and monolithic reinforced concrete and buried to 18 m, is calculated to be able to withstand an explosion (40 kt) without destruction at a height of 30 m at a minimum distance of 150 m (shock wave pressure of the order of 5 MPa), 38 kt of RDS have been tested. 2 at a distance of 235 m (pressure ~1.5 MPa), received minor deformations and damage. At temperatures in the compression front below 80 thousand °C, new NO2 molecules no longer appear, the layer of nitrogen dioxide gradually disappears and ceases to screen internal radiation. The impact sphere gradually becomes transparent and through it, as through darkened glass, clouds of bomb vapor and the isothermal sphere are visible for some time; In general, the fire sphere is similar to fireworks. Then, as transparency increases, the intensity of the radiation increases and the details of the sphere, as if flaring up again, become invisible. The process is reminiscent of the end of the era of recombination and the birth of light in the Universe several hundred thousand years after the Big Bang.

Time: 0.1s. Distance: 530m Temperature: 70 thousand°C. When the shock wave front separates and moves forward from the boundary of the fire sphere, its growth rate noticeably decreases. The 2nd phase of the glow begins, less intense, but two orders of magnitude longer, with the release of 99% of the explosion radiation energy mainly in the visible and IR spectrum. In the first hundred meters, a person does not have time to see the explosion and dies without suffering (human visual reaction time is 0.1 - 0.3 s, reaction time to a burn is 0.15 - 0.2 s).

Time: 0.15s. Distance: 580m Temperature: 65 thousand°C. Radiation ~100,000 Gy. A person is left with charred bone fragments (the speed of the shock wave is on the order of the speed of sound in soft tissues: a hydrodynamic shock that destroys cells and tissue passes through the body).

Time: 0.25s. Distance: 630m Temperature: 50 thousand°C. Penetrating radiation ~40,000 Gy. A person turns into charred wreckage: the shock wave causes traumatic amputation, which occurs in a fraction of a second. the fiery sphere chars the remains. Complete destruction of the tank. Complete destruction of underground cable lines, water pipelines, gas pipelines, sewers, inspection wells. Destruction of underground reinforced concrete pipes with a diameter of 1.5 m and a wall thickness of 0.2 m. Destruction of the arched concrete dam of a hydroelectric power station. Severe destruction of long-term reinforced concrete fortifications. Minor damage to underground metro structures.

Time: 0.4s. Distance: 800m Temperature: 40 thousand°C. Heating objects up to 3000 °C. Penetrating radiation ~20,000 Gy. Complete destruction of all civil defense protective structures (shelters) and destruction of protective devices at metro entrances. Destruction of the gravity concrete dam of a hydroelectric power station, bunkers become ineffective at a distance of 250 m.

Time: 0.73s. Distance: 1200m Temperature: 17 thousand°C. Radiation ~5000 Gy. With an explosion height of 1200 m, the heating of the ground air at the epicenter before the arrival of the shock. waves up to 900°C. Man - 100% death from the shock wave. Destruction of shelters designed for 200 kPa (type A-III or class 3). Complete destruction of prefabricated reinforced concrete bunkers at a distance of 500 m under the conditions of a ground explosion. Complete destruction of the railway tracks. The maximum brightness of the second phase of the sphere's glow by this time it had released ~20% of light energy

Time: 1.4s. Distance: 1600m Temperature: 12 thousand°C. Heating objects up to 200°C. Radiation 500 Gy. Numerous 3-4 degree burns up to 60-90% of the body surface, severe radiation damage combined with other injuries, mortality immediately or up to 100% in the first day. The tank is thrown back ~10 m and damaged. Complete destruction of metal and reinforced concrete bridges with a span of 30 - 50 m.

Time: 1.6s. Distance: 1750m Temperature: 10 thousand°C. Radiation approx. 70 Gr. The tank crew dies within 2-3 weeks from extremely severe radiation sickness. Complete destruction of concrete, reinforced concrete monolithic (low-rise) and earthquake-resistant buildings of 0.2 MPa, built-in and free-standing shelters designed for 100 kPa (type A-IV or class 4), shelters in the basements of multi-story buildings.

Time: 1.9c. Distance: 1900m Temperature: 9 thousand °C Dangerous damage to a person by the shock wave and throw up to 300 m with an initial speed of up to 400 km/h, of which 100-150 m (0.3-0.5 path) is free flight, and the remaining distance is numerous ricochets about the ground. Radiation of about 50 Gy is a fulminant form of radiation sickness[, 100% mortality within 6-9 days. Destruction of built-in shelters designed for 50 kPa. Severe destruction of earthquake-resistant buildings. Pressure 0.12 MPa and higher - all urban buildings are dense and discharged and turn into solid rubble (individual rubbles merge into one continuous one), the height of the rubble can be 3-4 m. The fire sphere at this time reaches its maximum size (D ~ 2 km), crushed from below by the shock wave reflected from the ground and begins to rise; the isothermal sphere in it collapses, forming a fast upward flow at the epicenter - the future leg of the mushroom.

Time: 2.6s. Distance: 2200m Temperature: 7.5 thousand°C. Severe injuries to a person by a shock wave. Radiation ~10 Gy is an extremely severe acute radiation sickness, with a combination of injuries, 100% mortality within 1-2 weeks. Safe stay in a tank, in a fortified basement with a reinforced reinforced concrete ceiling and in most G.O. shelters. Destruction of trucks. 0.1 MPa - design pressure of a shock wave for the design of structures and protective devices of underground structures of shallow subway lines.

Time: 3.8c. Distance: 2800m Temperature: 7.5 thousand°C. Radiation of 1 Gy - in peaceful conditions and timely treatment, a non-hazardous radiation injury, but with the unsanitary conditions and severe physical and psychological stress accompanying the disaster, lack of medical care, nutrition and normal rest, up to half of the victims die only from radiation and associated diseases, and in terms of the amount of damage ( plus injuries and burns) much more. Pressure less than 0.1 MPa - urban areas with dense buildings turn into solid rubble. Complete destruction of basements without reinforcement of structures 0.075 MPa. The average destruction of earthquake-resistant buildings is 0.08-0.12 MPa. Severe damage to prefabricated reinforced concrete bunkers. Detonation of pyrotechnics.

Time: 6c. Distance: 3600m Temperature: 4.5 thousand°C. Moderate damage to a person by a shock wave. Radiation ~0.05 Gy - the dose is not dangerous. People and objects leave “shadows” on the asphalt. Complete destruction of administrative multi-storey frame (office) buildings (0.05-0.06 MPa), shelters of the simplest type; severe and complete destruction of massive industrial structures. Almost all urban buildings were destroyed with the formation of local rubble (one house - one rubble). Complete destruction of passenger cars, complete destruction of the forest. An electromagnetic pulse of ~3 kV/m affects insensitive electrical appliances. The destruction is similar to an earthquake 10 points. The sphere turned into a fiery dome, like a bubble floating up, carrying with it a column of smoke and dust from the surface of the earth: a characteristic explosive mushroom grows with an initial vertical speed of up to 500 km/h. Wind speed at the surface to the epicenter is ~100 km/h.

Time: 10c. Distance: 6400m Temperature: 2 thousand°C. The end of the effective time of the second glow phase, ~80% of the total energy of light radiation has been released. The remaining 20% light up harmlessly for about a minute with a continuous decrease in intensity, gradually being lost in the clouds. Destruction of the simplest type of shelter (0.035-0.05 MPa). In the first kilometers, a person will not hear the roar of the explosion due to hearing damage from the shock wave. A person is thrown back by a shock wave of ~20 m with an initial speed of ~30 km/h. Complete destruction of multi-storey brick houses, panel houses, severe destruction of warehouses, moderate destruction of frame administrative buildings. The destruction is similar to a magnitude 8 earthquake. Safe in almost any basement.
The glow of the fiery dome ceases to be dangerous, it turns into a fiery cloud, growing in volume as it rises; hot gases in the cloud begin to rotate in a torus-shaped vortex; the hot products of the explosion are localized in the upper part of the cloud. The flow of dusty air in the column moves twice as fast as the rise of the “mushroom”, overtakes the cloud, passes through, diverges and, as it were, is wound around it, as if on a ring-shaped coil.

Time: 15c. Distance: 7500m. Light damage to a person by a shock wave. Third degree burns to exposed parts of the body. Complete destruction of wooden houses, severe destruction of brick multi-storey buildings 0.02-0.03 MPa, average destruction of brick warehouses, multi-storey reinforced concrete, panel houses; weak destruction of administrative buildings 0.02-0.03 MPa, massive industrial structures. Cars catching fire. The destruction is similar to a magnitude 6 earthquake or a magnitude 12 hurricane. up to 39 m/s. The “mushroom” has grown up to 3 km above the center of the explosion (the true height of the mushroom is greater than the height of the warhead explosion, about 1.5 km), it has a “skirt” of condensation of water vapor in a stream of warm air, fanned by the cloud into the cold upper layers atmosphere.

Time: 35c. Distance: 14km. Second degree burns. Paper and dark tarpaulin ignite. A zone of continuous fires; in areas of densely combustible buildings, a fire storm and tornado are possible (Hiroshima, “Operation Gomorrah”). Weak destruction of panel buildings. Disablement of aircraft and missiles. The destruction is similar to an earthquake of 4-5 points, a storm of 9-11 points V = 21 - 28.5 m/s. The “mushroom” has grown to ~5 km; the fiery cloud is shining more and more faintly.

Time: 1 min. Distance: 22km. First degree burns - death is possible in beachwear. Destruction of reinforced glazing. Uprooting large trees. Zone of individual fires. The “mushroom” has risen to 7.5 km, the cloud stops emitting light and now has a reddish tint due to the nitrogen oxides it contains, which will make it stand out sharply among other clouds.

Time: 1.5 min. Distance: 35km. The maximum radius of damage to unprotected sensitive electrical equipment by an electromagnetic pulse. Almost all the ordinary glass and some of the reinforced glass in the windows were broken - especially in the frosty winter, plus the possibility of cuts from flying fragments. The “Mushroom” rose to 10 km, the ascent speed was ~220 km/h. Above the tropopause, the cloud develops predominantly in width.
Time: 4min. Distance: 85km. The flash looks like a large, unnaturally bright Sun on the horizon and can cause a burn to the retina and a rush of heat to the face. The shock wave arriving after 4 minutes can still knock a person off his feet and break individual glass in the windows. “Mushroom” rose over 16 km, ascent speed ~140 km/h

Time: 8 min. Distance: 145km. The flash is not visible beyond the horizon, but a strong glow and a fiery cloud are visible. The total height of the “mushroom” is up to 24 km, the cloud is 9 km in height and 20-30 km in diameter, with its widest part it “rests” on the tropopause. The mushroom cloud has grown to its maximum size and is observed for about an hour or more until it is dissipated by the winds and mixed with normal clouds. Precipitation with relatively large particles falls from the cloud within 10-20 hours, forming a nearby radioactive trace.

Time: 5.5-13 hours Distance: 300-500 km. The far border of the moderately infected zone (zone A). The radiation level at the outer boundary of the zone is 0.08 Gy/h; total radiation dose 0.4-4 Gy.

Time: ~10 months. The effective time of half-deposition of radioactive substances for the lower layers of the tropical stratosphere (up to 21 km); fallout also occurs mainly in the middle latitudes in the same hemisphere where the explosion occurred.

Monument to the first test of the Trinity atomic bomb. This monument was erected at the White Sands test site in 1965, 20 years after the Trinity test. The monument's plaque reads: "The world's first atomic bomb test took place at this site on July 16, 1945." Another plaque below commemorates the site's designation as a National Historic Landmark. (Photo: Wikicommons)

Many of our readers associate the hydrogen bomb with an atomic one, only much more powerful. In fact, this is a fundamentally new weapon, which required disproportionately large intellectual efforts for its creation and works on fundamentally different physical principles.

"Puff"

Modern bomb

The only thing that the atomic and hydrogen bombs have in common is that both release colossal energy hidden in the atomic nucleus. This can be done in two ways: to divide heavy nuclei, for example, uranium or plutonium, into lighter ones (fission reaction) or to force the lightest isotopes of hydrogen to merge (fusion reaction). As a result of both reactions, the mass of the resulting material is always less than the mass of the original atoms. But mass cannot disappear without a trace - it turns into energy according to Einstein’s famous formula E=mc2.

A-bomb

To create an atomic bomb, a necessary and sufficient condition is to obtain fissile material in sufficient quantity. The work is quite labor-intensive, but low-intellectual, lying closer to the mining industry than to high science. The main resources for the creation of such weapons are spent on the construction of giant uranium mines and enrichment plants. Evidence of the simplicity of the device is the fact that less than a month passed between the production of the plutonium needed for the first bomb and the first Soviet nuclear explosion.

Let us briefly recall the operating principle of such a bomb, known from school physics courses. It is based on the property of uranium and some transuranium elements, for example, plutonium, to release more than one neutron during decay. These elements can decay either spontaneously or under the influence of other neutrons.

The released neutron can leave the radioactive material, or it can collide with another atom, causing another fission reaction. When a certain concentration of a substance (critical mass) is exceeded, the number of newborn neutrons, causing further fission of the atomic nucleus, begins to exceed the number of decaying nuclei. The number of decaying atoms begins to grow like an avalanche, giving birth to new neutrons, that is, a chain reaction occurs. For uranium-235, the critical mass is about 50 kg, for plutonium-239 - 5.6 kg. That is, a ball of plutonium weighing slightly less than 5.6 kg is just a warm piece of metal, and a mass of slightly more lasts only a few nanoseconds.

The actual operation of the bomb is simple: we take two hemispheres of uranium or plutonium, each slightly less than the critical mass, place them at a distance of 45 cm, cover them with explosives and detonate. The uranium or plutonium is sintered into a piece of supercritical mass, and a nuclear reaction begins. All. There is another way to start a nuclear reaction - to compress a piece of plutonium with a powerful explosion: the distance between the atoms will decrease, and the reaction will begin at a lower critical mass. All modern atomic detonators operate on this principle.

The problems with the atomic bomb begin from the moment we want to increase the power of the explosion. Simply increasing the fissile material is not enough - as soon as its mass reaches a critical mass, it detonates. Various ingenious schemes were invented, for example, to make a bomb not from two parts, but from many, which made the bomb begin to resemble a gutted orange, and then assemble it into one piece with one explosion, but still, with a power of over 100 kilotons, the problems became insurmountable.

H-bomb

But fuel for thermonuclear fusion does not have a critical mass. Here the Sun, filled with thermonuclear fuel, hangs overhead, a thermonuclear reaction has been going on inside it for billions of years, and nothing explodes. In addition, during the synthesis reaction of, for example, deuterium and tritium (heavy and superheavy isotope of hydrogen), energy is released 4.2 times more than during the combustion of the same mass of uranium-235.

Making the atomic bomb was an experimental rather than a theoretical process. The creation of a hydrogen bomb required the emergence of completely new physical disciplines: the physics of high-temperature plasma and ultra-high pressures. Before starting to construct a bomb, it was necessary to thoroughly understand the nature of the phenomena that occur only in the core of stars. No experiments could help here - the researchers’ tools were only theoretical physics and higher mathematics. It is no coincidence that a gigantic role in the development of thermonuclear weapons belongs to mathematicians: Ulam, Tikhonov, Samarsky, etc.

Classic super

By the end of 1945, Edward Teller proposed the first hydrogen bomb design, called the "classic super". To create the monstrous pressure and temperature necessary to start the fusion reaction, it was supposed to use a conventional atomic bomb. The “classic super” itself was a long cylinder filled with deuterium. An intermediate “ignition” chamber with a deuterium-tritium mixture was also provided - the synthesis reaction of deuterium and tritium begins at a lower pressure. By analogy with a fire, deuterium was supposed to play the role of firewood, a mixture of deuterium and tritium - a glass of gasoline, and an atomic bomb - a match. This scheme was called a “pipe” - a kind of cigar with an atomic lighter at one end. Soviet physicists began to develop the hydrogen bomb using the same scheme.

However, mathematician Stanislav Ulam, using an ordinary slide rule, proved to Teller that the occurrence of a fusion reaction of pure deuterium in a “super” is hardly possible, and the mixture would require such an amount of tritium that to produce it it would be necessary to practically freeze the production of weapons-grade plutonium in the United States.

Puff with sugar

In mid-1946, Teller proposed another hydrogen bomb design - the “alarm clock”. It consisted of alternating spherical layers of uranium, deuterium and tritium. During the nuclear explosion of the central charge of plutonium, the necessary pressure and temperature were created for the start of a thermonuclear reaction in other layers of the bomb. However, the “alarm clock” required a high-power atomic initiator, and the United States (as well as the USSR) had problems producing weapons-grade uranium and plutonium.

In the fall of 1948, Andrei Sakharov came to a similar scheme. In the Soviet Union, the design was called “sloyka”. For the USSR, which did not have time to produce weapons-grade uranium-235 and plutonium-239 in sufficient quantities, Sakharov’s puff paste was a panacea. And that's why.

In a conventional atomic bomb, natural uranium-238 is not only useless (the neutron energy during decay is not enough to initiate fission), but also harmful because it eagerly absorbs secondary neutrons, slowing down the chain reaction. Therefore, 90% of weapons-grade uranium consists of the isotope uranium-235. However, neutrons resulting from thermonuclear fusion are 10 times more energetic than fission neutrons, and natural uranium-238 irradiated with such neutrons begins to fission excellently. The new bomb made it possible to use uranium-238, which had previously been considered a waste product, as an explosive.

The highlight of Sakharov’s “puff pastry” was also the use of a white light crystalline substance, lithium deuteride 6LiD, instead of acutely deficient tritium.

As mentioned above, a mixture of deuterium and tritium ignites much more easily than pure deuterium. However, this is where the advantages of tritium end, and only disadvantages remain: in its normal state, tritium is a gas, which causes difficulties with storage; tritium is radioactive and decays into stable helium-3, which actively consumes much-needed fast neutrons, limiting the bomb's shelf life to a few months.

Non-radioactive lithium deutride, when irradiated with slow fission neutrons - the consequences of an atomic fuse explosion - turns into tritium. Thus, the radiation from the primary atomic explosion instantly produces a sufficient amount of tritium for a further thermonuclear reaction, and deuterium is initially present in lithium deutride.

It was just such a bomb, RDS-6s, that was successfully tested on August 12, 1953 at the tower of the Semipalatinsk test site. The power of the explosion was 400 kilotons, and there is still debate over whether it was a real thermonuclear explosion or a super-powerful atomic one. After all, the thermonuclear fusion reaction in Sakharov’s puff paste accounted for no more than 20% of the total charge power. The main contribution to the explosion was made by the decay reaction of uranium-238 irradiated with fast neutrons, thanks to which the RDS-6s ushered in the era of the so-called “dirty” bombs.

The fact is that the main radioactive contamination comes from decay products (in particular, strontium-90 and cesium-137). Essentially, Sakharov’s “puff pastry” was a giant atomic bomb, only slightly enhanced by a thermonuclear reaction. It is no coincidence that just one “puff pastry” explosion produced 82% of strontium-90 and 75% of cesium-137, which entered the atmosphere over the entire history of the Semipalatinsk test site.

American bombs

However, it was the Americans who were the first to detonate the hydrogen bomb. On November 1, 1952, the Mike thermonuclear device, with a yield of 10 megatons, was successfully tested at Elugelab Atoll in the Pacific Ocean. It would be hard to call a 74-ton American device a bomb. “Mike” was a bulky device the size of a two-story house, filled with liquid deuterium at a temperature close to absolute zero (Sakharov’s “puff pastry” was a completely transportable product). However, the highlight of “Mike” was not its size, but the ingenious principle of compressing thermonuclear explosives.

Let us recall that the main idea of a hydrogen bomb is to create conditions for fusion (ultra-high pressure and temperature) through a nuclear explosion. In the “puff” scheme, the nuclear charge is located in the center, and therefore it does not so much compress the deuterium as scatter it outwards - increasing the amount of thermonuclear explosive does not lead to an increase in power - it simply does not have time to detonate. This is precisely what limits the maximum power of this scheme - the most powerful “puff” in the world, the Orange Herald, blown up by the British on May 31, 1957, yielded only 720 kilotons.

It would be ideal if we could make the atomic fuse explode inside, compressing the thermonuclear explosive. But how to do that? Edward Teller put forward a brilliant idea: to compress thermonuclear fuel not with mechanical energy and neutron flux, but with the radiation of the primary atomic fuse.

In Teller's new design, the initiating atomic unit was separated from the thermonuclear unit. When the atomic charge was triggered, X-ray radiation preceded the shock wave and spread along the walls of the cylindrical body, evaporating and turning the polyethylene inner lining of the bomb body into plasma. The plasma, in turn, re-emited softer X-rays, which were absorbed by the outer layers of the inner cylinder of uranium-238 - the “pusher”. The layers began to evaporate explosively (this phenomenon is called ablation). Hot uranium plasma can be compared to the jets of a super-powerful rocket engine, the thrust of which is directed into the cylinder with deuterium. The uranium cylinder collapsed, the pressure and temperature of the deuterium reached a critical level. The same pressure compressed the central plutonium tube to a critical mass, and it detonated. The explosion of the plutonium fuse pressed on the deuterium from the inside, further compressing and heating the thermonuclear explosive, which detonated. An intense stream of neutrons splits the uranium-238 nuclei in the “pusher”, causing a secondary decay reaction. All this managed to happen before the moment when the blast wave from the primary nuclear explosion reached the thermonuclear unit. The calculation of all these events, occurring in billionths of a second, required the brainpower of the strongest mathematicians on the planet. The creators of “Mike” experienced not horror from the 10-megaton explosion, but indescribable delight - they managed not only to understand the processes that in the real world occur only in the cores of stars, but also to experimentally test their theories by setting up their own small star on Earth.

Bravo

Having surpassed the Russians in the beauty of the design, the Americans were unable to make their device compact: they used liquid supercooled deuterium instead of Sakharov’s powdered lithium deuteride. In Los Alamos they reacted to Sakharov’s “puff pastry” with a bit of envy: “instead of a huge cow with a bucket of raw milk, the Russians use a bag of powdered milk.” However, both sides failed to hide secrets from each other. On March 1, 1954, near the Bikini Atoll, the Americans tested a 15-megaton bomb “Bravo” using lithium deuteride, and on November 22, 1955, the first Soviet two-stage thermonuclear bomb RDS-37 with a power of 1.7 megatons exploded over the Semipalatinsk test site, demolishing almost half of the test site. Since then, the design of the thermonuclear bomb has undergone minor changes (for example, a uranium shield appeared between the initiating bomb and the main charge) and has become canonical. And there are no more large-scale mysteries of nature left in the world that could be solved with such a spectacular experiment. Perhaps the birth of a supernova.

The content of the article

H-BOMB, a weapon of great destructive power (on the order of megatons in TNT equivalent), the operating principle of which is based on the reaction of thermonuclear fusion of light nuclei. The source of explosion energy is processes similar to those occurring on the Sun and other stars.

Thermonuclear reactions.

The interior of the Sun contains a gigantic amount of hydrogen, which is in a state of ultra-high compression at a temperature of approx. 15,000,000 K. At such high temperatures and plasma densities, hydrogen nuclei experience constant collisions with each other, some of which result in their fusion and ultimately the formation of heavier helium nuclei. Such reactions, called thermonuclear fusion, are accompanied by the release of enormous amounts of energy. According to the laws of physics, the energy release during thermonuclear fusion is due to the fact that during the formation of a heavier nucleus, part of the mass of the light nuclei included in its composition is converted into a colossal amount of energy. That is why the Sun, having a gigantic mass, loses approx. every day in the process of thermonuclear fusion. 100 billion tons of matter and releases energy, thanks to which life on Earth became possible.

Isotopes of hydrogen.

The hydrogen atom is the simplest of all existing atoms. It consists of one proton, which is its nucleus, around which a single electron rotates. Careful studies of water (H 2 O) have shown that it contains negligible amounts of “heavy” water containing the “heavy isotope” of hydrogen - deuterium (2 H). The deuterium nucleus consists of a proton and a neutron - a neutral particle with a mass close to a proton.

There is a third isotope of hydrogen, tritium, whose nucleus contains one proton and two neutrons. Tritium is unstable and undergoes spontaneous radioactive decay, turning into an isotope of helium. Traces of tritium have been found in the Earth's atmosphere, where it is formed as a result of the interaction of cosmic rays with gas molecules that make up the air. Tritium is produced artificially in a nuclear reactor by irradiating the lithium-6 isotope with a stream of neutrons.

Development of the hydrogen bomb.

Preliminary theoretical analysis has shown that thermonuclear fusion is most easily accomplished in a mixture of deuterium and tritium. Taking this as a basis, US scientists at the beginning of 1950 began implementing a project to create a hydrogen bomb (HB). The first tests of a model nuclear device were carried out at the Enewetak test site in the spring of 1951; thermonuclear fusion was only partial. Significant success was achieved on November 1, 1951 during the testing of a massive nuclear device, the explosion power of which was 4 × 8 Mt in TNT equivalent.

The first hydrogen aerial bomb was detonated in the USSR on August 12, 1953, and on March 1, 1954, the Americans detonated a more powerful (approximately 15 Mt) aerial bomb on Bikini Atoll. Since then, both powers have carried out explosions of advanced megaton weapons.

The explosion at Bikini Atoll was accompanied by the release of large amounts of radioactive substances. Some of them fell hundreds of kilometers from the explosion site on the Japanese fishing vessel "Lucky Dragon", while others covered the island of Rongelap. Since thermonuclear fusion produces stable helium, the radioactivity from the explosion of a pure hydrogen bomb should be no more than that of an atomic detonator of a thermonuclear reaction. However, in the case under consideration, the predicted and actual radioactive fallout differed significantly in quantity and composition.

The mechanism of action of the hydrogen bomb.

The sequence of processes occurring during the explosion of a hydrogen bomb can be represented as follows. First, the thermonuclear reaction initiator charge (a small atomic bomb) located inside the HB shell explodes, resulting in a neutron flash and creating the high temperature necessary to initiate thermonuclear fusion. Neutrons bombard an insert made of lithium deuteride, a compound of deuterium and lithium (a lithium isotope with mass number 6 is used). Lithium-6 is split into helium and tritium under the influence of neutrons. Thus, the atomic fuse creates the materials necessary for synthesis directly in the actual bomb itself.

Then a thermonuclear reaction begins in a mixture of deuterium and tritium, the temperature inside the bomb rapidly increases, involving more and more hydrogen in the synthesis. With a further increase in temperature, a reaction between deuterium nuclei, characteristic of a pure hydrogen bomb, could begin. All reactions, of course, occur so quickly that they are perceived as instantaneous.

Fission, fusion, fission (superbomb).

In fact, in a bomb, the sequence of processes described above ends at the stage of the reaction of deuterium with tritium. Further, the bomb designers chose not to use nuclear fusion, but nuclear fission. The fusion of deuterium and tritium nuclei produces helium and fast neutrons, the energy of which is high enough to cause nuclear fission of uranium-238 (the main isotope of uranium, much cheaper than the uranium-235 used in conventional atomic bombs). Fast neutrons split the atoms of the uranium shell of the superbomb. The fission of one ton of uranium creates energy equivalent to 18 Mt. Energy goes not only to explosion and heat generation. Each uranium nucleus splits into two highly radioactive “fragments.” Fission products include 36 different chemical elements and nearly 200 radioactive isotopes. All this constitutes the radioactive fallout that accompanies superbomb explosions.

Thanks to the unique design and the described mechanism of action, weapons of this type can be made as powerful as desired. It is much cheaper than atomic bombs of the same power.

Consequences of the explosion.

Shock wave and thermal effect.

The direct (primary) impact of a superbomb explosion is threefold. The most obvious direct impact is a shock wave of enormous intensity. The strength of its impact, depending on the power of the bomb, the height of the explosion above the surface of the earth and the nature of the terrain, decreases with distance from the epicenter of the explosion. The thermal impact of an explosion is determined by the same factors, but also depends on the transparency of the air - fog sharply reduces the distance at which a thermal flash can cause serious burns.

According to calculations, during an explosion in the atmosphere of a 20-megaton bomb, people will remain alive in 50% of cases if they 1) take refuge in an underground reinforced concrete shelter at a distance of approximately 8 km from the epicenter of the explosion (E), 2) are in ordinary urban buildings at a distance of approx. . 15 km from EV, 3) found themselves in an open place at a distance of approx. 20 km from EV. In conditions of poor visibility and at a distance of at least 25 km, if the atmosphere is clear, for people in open areas, the likelihood of survival increases rapidly with distance from the epicenter; at a distance of 32 km its calculated value is more than 90%. The area over which the penetrating radiation generated during an explosion causes death is relatively small, even in the case of a high-power superbomb.

Fire ball.

Depending on the composition and mass of flammable material involved in the fireball, giant self-sustaining firestorms can form and rage for many hours. However, the most dangerous (albeit secondary) consequence of the explosion is radioactive contamination of the environment.

Fallout.

How they are formed.

When a bomb explodes, the resulting fireball is filled with a huge amount of radioactive particles. Typically, these particles are so small that once they reach the upper atmosphere, they can remain there for a long time. But if a fireball comes into contact with the surface of the Earth, it turns everything on it into hot dust and ash and draws them into a fiery tornado. In a whirlwind of flame, they mix and bind with radioactive particles. Radioactive dust, except the largest, does not settle immediately. Finer dust is carried away by the resulting cloud and gradually falls out as it moves with the wind. Directly at the site of the explosion, radioactive fallout can be extremely intense - mainly large dust settling on the ground. Hundreds of kilometers from the explosion site and at greater distances, small but still visible particles of ash fall to the ground. They often form a cover similar to fallen snow, deadly to anyone who happens to be nearby. Even smaller and invisible particles, before they settle on the ground, can wander in the atmosphere for months and even years, circling the globe many times. By the time they fall out, their radioactivity is significantly weakened. The most dangerous radiation remains strontium-90 with a half-life of 28 years. Its loss is clearly observed throughout the world. When it settles on leaves and grass, it enters food chains that include humans. As a consequence of this, noticeable, although not yet dangerous, amounts of strontium-90 have been found in the bones of residents of most countries. The accumulation of strontium-90 in human bones is very dangerous in the long term, as it leads to the formation of malignant bone tumors.

Long-term contamination of the area with radioactive fallout.

In the event of hostilities, the use of a hydrogen bomb will lead to immediate radioactive contamination of an area within a radius of approx. 100 km from the epicenter of the explosion. If a superbomb explodes, an area of tens of thousands of square kilometers will be contaminated. Such a huge area of destruction with a single bomb makes it a completely new type of weapon. Even if the superbomb does not hit the target, i.e. will not hit the object with shock-thermal effects, the penetrating radiation and radioactive fallout accompanying the explosion will make the surrounding space uninhabitable. Such precipitation can continue for many days, weeks and even months. Depending on their quantity, the intensity of radiation can reach deadly levels. A relatively small number of superbombs is enough to completely cover a large country with a layer of radioactive dust that is deadly to all living things. Thus, the creation of the superbomb marked the beginning of an era when it became possible to make entire continents uninhabitable. Even long after the cessation of direct exposure to radioactive fallout, the danger due to the high radiotoxicity of isotopes such as strontium-90 will remain. With food grown on soils contaminated with this isotope, radioactivity will enter the human body.

On October 30, 1961, the most powerful explosion in human history occurred at the Soviet nuclear test site on Novaya Zemlya. The nuclear mushroom rose to a height of 67 kilometers, and the diameter of the “cap” of this mushroom was 95 kilometers. The shock wave circled the globe three times (and the blast wave demolished wooden buildings at a distance of several hundred kilometers from the test site). The flash of the explosion was visible from a distance of a thousand kilometers, despite the fact that thick clouds hung over Novaya Zemlya. For almost an hour there was no radio communication throughout the entire Arctic. The power of the explosion, according to various sources, ranged from 50 to 57 megatons (million tons of TNT).

However, as Nikita Sergeevich Khrushchev joked, they did not increase the power of the bomb to 100 megatons, only because in this case all the windows in Moscow would have been broken. But every joke has its share of a joke - it was originally planned to detonate a 100 megaton bomb. And the explosion on Novaya Zemlya convincingly proved that creating a bomb with a capacity of at least 100 megatons, at least 200, is a completely feasible task. But 50 megatons is almost ten times the power of all the ammunition expended during the entire Second World War by all participating countries. Moreover, in the event of testing a product with a capacity of 100 megatons, only a melted crater would remain from the test site on Novaya Zemlya (and most of this island). In Moscow, the glass most likely would have survived, but in Murmansk they could have been blown out.

Model of a hydrogen bomb. Historical and Memorial Museum of Nuclear Weapons in Sarov

The device, detonated at an altitude of 4200 meters above sea level on October 30, 1961, went down in history under the name “Tsar Bomba”. Another unofficial name is “Kuzkina Mother”. But the official name of this hydrogen bomb was not so loud - the modest product AN602. This miracle weapon had no military significance - not in tons of TNT equivalent, but in ordinary metric tons, the “product” weighed 26 tons and it would have been problematic to deliver it to the “addressee”. It was a show of force - clear proof that the Soviet Union was capable of creating weapons of mass destruction of any power. What made the leadership of our country take such an unprecedented step? Of course, nothing more than a worsening of relations with the United States. More recently, it seemed that the United States and the Soviet Union had reached mutual understanding on all issues - in September 1959, Khrushchev visited the United States on an official visit, and a return visit to Moscow by President Dwight Eisenhower was also planned. But on May 1, 1960, an American U-2 reconnaissance aircraft was shot down over Soviet territory. In April 1961, American intelligence agencies organized the landing of well-trained Cuban emigrants in the Bay of Playa Giron (this adventure ended in a convincing victory for Fidel Castro). In Europe, the great powers could not decide on the status of West Berlin. As a result, on August 13, 1961, the capital of Germany was blocked by the famous Berlin Wall. Finally, in 1961, the United States deployed PGM-19 Jupiter missiles in Turkey - European Russia (including Moscow) was within range of these missiles (a year later, the Soviet Union would deploy missiles in Cuba and the famous Cuban Missile Crisis would begin). This is not to mention the fact that there was no parity in the number of nuclear charges and their carriers between the Soviet Union and America at that time - we could counter 6 thousand American warheads with only three hundred. So, the demonstration of thermonuclear power was not at all superfluous in the current situation.

Soviet short film about the testing of the Tsar Bomba

There is a popular myth that the superbomb was developed on Khrushchev’s orders in the same 1961 in record time - in just 112 days. In fact, the development of the bomb began in 1954. And in 1961, the developers simply brought the existing “product” to the required power. At the same time, the Tupolev Design Bureau was modernizing Tu-16 and Tu-95 aircraft for new weapons. According to initial calculations, the weight of the bomb should have been at least 40 tons, but aircraft designers explained to nuclear scientists that at the moment there are no carriers for a product with such a weight and there cannot be. Nuclear scientists promised to reduce the weight of the bomb to a quite acceptable 20 tons. True, such weight and such dimensions required a complete rework of the bomb compartments, fastenings, and bomb bays.

Hydrogen bomb explosion

Work on the bomb was carried out by a group of young nuclear physicists under the leadership of I.V. Kurchatova. This group also included Andrei Sakharov, who at that time had not yet thought about dissent. Moreover, he was one of the leading developers of the product.

Such power was achieved through the use of a multi-stage design - a uranium charge with a power of “only” one and a half megatons launched a nuclear reaction in a second-stage charge with a power of 50 megatons. Without changing the dimensions of the bomb, it was possible to make it three-stage (this is already 100 megatons). Theoretically, the number of stage charges could be unlimited. The design of the bomb was unique for its time.

Khrushchev hurried the developers - in October, the 22nd Congress of the CPSU was taking place in the newly built Kremlin Palace of Congresses, and the news about the most powerful explosion in the history of mankind should have been announced from the rostrum of the congress. And on October 30, 1961, Khrushchev received a long-awaited telegram signed by the Minister of Medium Engineering E.P. Slavsky and Marshal of the Soviet Union K.S. Moskalenko (test leaders):

"Moscow. The Kremlin. N.S. Khrushchev.
The test on Novaya Zemlya was successful. The safety of testers and the surrounding population is ensured. The training ground and all participants completed the task of the Motherland. We're going back to the convention."

The explosion of the Tsar Bomba almost immediately served as fertile ground for all sorts of myths. Some of them were distributed ... by the official press. For example, Pravda called the Tsar Bomba nothing less than the yesterday of atomic weapons and argued that more powerful charges had already been created. There were also rumors about a self-sustaining thermonuclear reaction in the atmosphere. The reduction in the power of the explosion, according to some, was caused by the fear of splitting the earth's crust or...causing a thermonuclear reaction in the oceans.

But be that as it may, a year later, during the Cuban Missile Crisis, the United States still had an overwhelming superiority in the number of nuclear warheads. But they never decided to use them.

In addition, the mega-explosion is believed to have helped move forward the three-medium nuclear test ban negotiations that had been going on in Geneva since the late fifties. In 1959-60, all nuclear powers, with the exception of France, accepted a unilateral refusal to test while these negotiations were ongoing. But we talked below about the reasons that forced the Soviet Union not to comply with its obligations. After the explosion on Novaya Zemlya, negotiations resumed. And on October 10, 1963, the “Treaty Banning Nuclear Weapons Tests in the Atmosphere, Outer Space and Under Water” was signed in Moscow. As long as this Treaty is respected, the Soviet Tsar Bomba will remain the most powerful explosive device in human history.

Modern computer reconstruction

There are a considerable number of different political clubs in the world. The G7, now the G20, BRICS, SCO, NATO, the European Union, to some extent. However, none of these clubs can boast of a unique function - the ability to destroy the world as we know it. The “nuclear club” has similar capabilities.

Today there are 9 countries that have nuclear weapons:

Countries are ranked as they acquire nuclear weapons in their arsenal. If the list were arranged by the number of warheads, then Russia would be in first place with its 8,000 units, 1,600 of which can be launched even now. The states are only 700 units behind, but they have 320 more charges at hand. “Nuclear club” is a purely relative concept; in fact, there is no club. There are a number of agreements between countries on non-proliferation and reduction of nuclear weapons stockpiles.

The first tests of the atomic bomb, as we know, were carried out by the United States back in 1945. This weapon was tested in the “field” conditions of World War II on residents of the Japanese cities of Hiroshima and Nagasaki. They operate on the principle of division. During the explosion, a chain reaction is triggered, which provokes the fission of nuclei into two, with the accompanying release of energy. Uranium and plutonium are mainly used for this reaction. Our ideas about what nuclear bombs are made of are connected with these elements. Since uranium occurs in nature only as a mixture of three isotopes, of which only one is capable of supporting such a reaction, it is necessary to enrich uranium. The alternative is plutonium-239, which does not occur naturally and must be produced from uranium.

If a fission reaction occurs in a uranium bomb, then a fusion reaction occurs in a hydrogen bomb - this is the essence of how a hydrogen bomb differs from an atomic one. We all know that the sun gives us light, warmth, and one might say life. The same processes that occur in the sun can easily destroy cities and countries. The explosion of a hydrogen bomb is generated by the synthesis of light nuclei, the so-called thermonuclear fusion. This “miracle” is possible thanks to hydrogen isotopes - deuterium and tritium. This is actually why the bomb is called a hydrogen bomb. You can also see the name “thermonuclear bomb”, from the reaction that underlies this weapon.

After the world saw the destructive power of nuclear weapons, in August 1945, the USSR began a race that lasted until its collapse. The United States was the first to create, test and use nuclear weapons, the first to detonate a hydrogen bomb, but the USSR can be credited with the first production of a compact hydrogen bomb, which can be delivered to the enemy on a regular Tu-16. The first US bomb was the size of a three-story house; a hydrogen bomb of that size would be of little use. The Soviets received such weapons already in 1952, while the United States' first "adequate" bomb was adopted only in 1954. If you look back and analyze the explosions in Nagasaki and Hiroshima, you can come to the conclusion that they were not so powerful . Two bombs in total destroyed both cities and killed, according to various sources, up to 220,000 people. Carpet bombing of Tokyo could kill 150-200,000 people a day even without any nuclear weapons. This is due to the low power of the first bombs - only a few tens of kilotons of TNT. Hydrogen bombs were tested with an aim to overcome 1 megaton or more.

The first Soviet bomb was tested with a claim of 3 Mt, but in the end they tested 1.6 Mt.

The most powerful hydrogen bomb was tested by the Soviets in 1961. Its capacity reached 58-75 Mt, with the declared 51 Mt. “Tsar” plunged the world into a slight shock, in the literal sense. The shock wave circled the planet three times. There was not a single hill left at the test site (Novaya Zemlya), the explosion was heard at a distance of 800 km. The fireball reached a diameter of almost 5 km, the “mushroom” grew by 67 km, and the diameter of its cap was almost 100 km. The consequences of such an explosion in a large city are hard to imagine. According to many experts, it was the test of a hydrogen bomb of such power (the States at that time had bombs four times less powerful) that became the first step towards signing various treaties banning nuclear weapons, their testing and reducing production. For the first time, the world began to think about its own security, which was truly at risk.

As mentioned earlier, the principle of operation of a hydrogen bomb is based on a fusion reaction. Thermonuclear fusion is the process of fusion of two nuclei into one, with the formation of a third element, the release of a fourth and energy. The forces that repel nuclei are enormous, so in order for the atoms to come close enough to merge, the temperature must be simply enormous. Scientists have been puzzling over cold thermonuclear fusion for centuries, trying, so to speak, to reset the fusion temperature to room temperature, ideally. In this case, humanity will have access to the energy of the future. As for the current thermonuclear reaction, to start it you still need to light a miniature sun here on Earth - bombs usually use a uranium or plutonium charge to start the fusion.

In addition to the consequences described above from the use of a bomb of tens of megatons, a hydrogen bomb, like any nuclear weapon, has a number of consequences from its use. Some people tend to believe that the hydrogen bomb is a “cleaner weapon” than a conventional bomb. Perhaps this has something to do with the name. People hear the word “water” and think that it has something to do with water and hydrogen, and therefore the consequences are not so dire. In fact, this is certainly not the case, because the action of a hydrogen bomb is based on extremely radioactive substances. It is theoretically possible to make a bomb without a uranium charge, but this is impractical due to the complexity of the process, so the pure fusion reaction is “diluted” with uranium to increase power. At the same time, the amount of radioactive fallout increases to 1000%. Everything that falls into the fireball will be destroyed, the area within the affected radius will become uninhabitable for people for decades. Radioactive fallout can harm the health of people hundreds and thousands of kilometers away. Specific numbers and the area of infection can be calculated by knowing the strength of the charge.

However, the destruction of cities is not the worst thing that can happen “thanks” to weapons of mass destruction. After a nuclear war, the world will not be completely destroyed. Thousands of large cities, billions of people will remain on the planet, and only a small percentage of territories will lose their “livable” status. In the long term, the entire world will be at risk due to the so-called “nuclear winter.” Detonation of the “club’s” nuclear arsenal could trigger the release of enough substance (dust, soot, smoke) into the atmosphere to “reduce” the brightness of the sun. The shroud, which could spread across the entire planet, would destroy crops for several years to come, causing famine and inevitable population decline. There has already been a “year without summer” in history, after a major volcanic eruption in 1816, so nuclear winter looks more than possible. Again, depending on how the war proceeds, we may end up with the following types of global climate change:

a cooling of 1 degree will pass unnoticed;
nuclear autumn - cooling by 2-4 degrees, crop failures and increased formation of hurricanes are possible;
an analogue of the “year without summer” - when the temperature dropped significantly, by several degrees for a year;
Little Ice Age – temperatures may drop by 30–40 degrees for a significant period of time and will be accompanied by depopulation of a number of northern zones and crop failures;
ice age - the development of the Little Ice Age, when the reflection of sunlight from the surface can reach a certain critical level and the temperature will continue to fall, the only difference is the temperature;
irreversible cooling is a very sad version of the Ice Age, which, under the influence of many factors, will turn the Earth into a new planet.

The nuclear winter theory has been constantly criticized, and its implications seem a bit overblown. However, there is no need to doubt its inevitable offensive in any global conflict involving the use of hydrogen bombs.

The Cold War is long behind us, and therefore nuclear hysteria can only be seen in old Hollywood films and on the covers of rare magazines and comics. Despite this, we may be on the verge of a, albeit small, but serious nuclear conflict. All this thanks to the rocket lover and hero of the fight against US imperialist ambitions - Kim Jong-un. The DPRK hydrogen bomb is still a hypothetical object; only indirect evidence speaks of its existence. Of course, the North Korean government constantly reports that they have managed to make new bombs, but no one has seen them live yet. Naturally, the States and their allies - Japan and South Korea - are a little more concerned about the presence, even hypothetical, of such weapons in the DPRK. The reality is that at the moment the DPRK does not have enough technology to successfully attack the United States, which they announce to the whole world every year. Even an attack on neighboring Japan or the South may not be very successful, if at all, but every year the danger of a new conflict on the Korean Peninsula is growing.