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Nuclear weapon designs are often divided into two classes, based on the dominant source of the nuclear weapon's energy.

• Fission bombs derive their power from nuclear fission, where heavy nuclei (uranium or plutonium) split into lighter elements when bombarded by neutrons (produce more neutrons which bombard other nuclei, triggering a chain reaction). These are historically called atom bombs or A-bombs, though this name is not precise due to the fact that chemical reactions release energy from atomic bonds and fusion is no less atomic than fission. Despite this possible confusion, the term atom bomb has still been generally accepted to refer specifically to nuclear weapons, and most commonly to pure fission devices.

• Fusion bombs are based on nuclear fusion where light nuclei such as hydrogen and helium combine together into heavier elements and release large amounts of energy. Weapons which have a fusion stage are also referred to as hydrogen bombs or H-bombs because of their primary fuel, or thermonuclear weapons because fusion reactions require extremely high temperatures for a chain reaction to occur.

The distinction between these two types of weapon is blurred by the fact that they are combined in nearly all complex modern weapons: a smaller fission bomb is first used to reach the necessary conditions of high temperature and pressure to allow fusion to occur. On the other hand, a fission device is more efficient when a fusion core first boosts the weapon's energy. Since the distinguishing feature of both fission and fusion weapons is that they release energy from transformations of the atomic nucleus, the best general term for all types of these explosive devices is "nuclear weapon".

Other specific types of nuclear weapon design which are commonly referred to by name include: neutron bomb, cobalt bomb, enhanced radiation weapon, and salted bomb.

The simplest nuclear weapons are pure fission bombs. These were the first types of nuclear weapons built during the Manhattan Project and they are a building block for all advanced nuclear weapons designs.

A mass of fissile material is called critical when it is capable of a sustained chain reaction, which depends upon the size, shape and purity of the material as well as what surrounds the material. A numerical measure of whether a mass is critical or not is available as the neutron multiplication factor, k, where

k = f - l

Where f is the average number of neutrons released per fission event and l is the average number of neutrons lost by either leaving the system or being captured in a non-fission event.When k=1 the mass is critical, k<1 is subcritical and k>1 is supercritical. A fission bomb works by rapidly changing a subcritical mass of fissile material into a supercritical assembly, causing a chain reaction which rapidly releases large amounts of energy. In practice the mass is not made slightly critical, but goes from slightly subcritical (k=.9) to highly supercritical (k= 2 or 3), so that each neutron creates several new neutrons and the chain reaction advances more quickly. The main challenge in producing an efficient explosion using nuclear fission is to keep the bomb together long enough for a substantial fraction of the available nuclear energy to be released.

Until detonation is desired, the weapon must consist of a number of separate pieces each of which is below the critical size either because they are too small or unfavorably shaped. To produce detonation, the fissile material must be brought together rapidly. In the course of this assembly process the chain reaction is likely to start causing the material to heat up and expand, preventing the material from reaching its most compact (and most efficient) form. It may turn out that the explosion is so inefficient as to be practically useless. The majority of the technical difficulties of designing and manufacturing a fission weapon are based on the need to both reduce the time of assembly of a supercritical mass to a minimum and reduce the number of stray (pre-detonation) neutrons to a minimum.

The isotopes desirable for a nuclear weapon are those which have a high probability of fission reaction, yield a high number of excess neutrons, have a low probability of absorbing neutrons without a fission reaction, and do not release a large number of spontaneous neutrons. The primary isotopes which fit these criteria are U-235, Pu-239 and U-233.

Enriched Materials

Naturally occurring uranium consists mostly of U-238, with a small part U-235. The U-238 isotope has a high probability of absorbing a neutron without a fission, and also a higher rate of spontaneous fission. For weapons, uranium is enriched through isotope separation. Uranium which is more than 80% U-235 is called highly enriched uranium (HEU), and weapons grade uranium is at least 93.5% U-235. U-235 has a spontaneous fission rate of 0.16 fissions/s-kg. which is low enough to make super critical assembly relatively easy. The critical mass for an unreflected sphere of U-235 is about 50 kg, which is a sphere with a diameter of 17 cm. This size can be reduced to about 15 kg with the use of a neutron reflector surrounding the sphere.

Plutonium (atomic number 94, two more than uranium) does not occur in nature and is manufactured by exposing U-238 to a neutron source (i.e. a nuclear reactor). When U-238 absorbs a neutron the resulting U-239 isotope then beta decays twice into Pu-239. The plutonium can then be chemically separated from the uranium and be isolated for weapons use. Pu-239 has a higher probability for fission than U-235, and a larger number of neutrons produced per fission event, resulting in a smaller critical mass. Pure Pu-239 also has a reasonably low rate of neutron emission due to spontaneous fission (10 fission/s-kg), making it feasible to assemble a super critical mass before predetonation. The Pu-239 will be invariably contaminated by Pu-240, however, due to the fact that the freshly made Pu-239 captures a neutron to make Pu-240. Pu-240 has a high rate of spontaneous fission events (415,000 fission/s-kg), making it extremely difficult to assemble a super critical mass before the neutrons emitted from spontaneous fission start a premature chain reaction and cause the weapon to fizzle. Weapons grade plutonium must contain no more than 7% Pu-240 - and is obtained by only exposing U-238 samples to neutron sources for short periods of time to reduce the amount of Pu-240 made. The critical mass for an unreflected sphere of plutonium is 16 kg, but through the use of a neutron reflecting tamper the pit of plutonium in a fission bomb is reduced to 10 kg, which is a sphere with a diameter of 10 cm.

Combination Methods

The simplest technical mechanism for assembling a supercritical mass is to shoot one piece of fissile material as a projectile against a second part as a target, usually called the gun method. This is how the Little Boy weapon which was detonated over Hiroshima worked. This method of combination can only be used for U-235 because of the relatively long amount of time it takes to combine the materials, making predetonation likely for Pu-239 which has a higher spontaneous neutron release due to Pu-240 contamination.

The more difficult, but superior, method of combination is referred to as the implosion method and uses conventional explosives surrounding the material to rapidly compress the mass to a supercritical state. For Pu-239 assemblies a contamination of only 1% Pu-240 produces so many neutrons that implosion systems are required to produce efficient bombs. This is the reason that the more technically difficult implosion method was used on the plutonium Fat Man weapon which was detonated over Nagasaki.

Weapons assembled with this method also tend to be more efficient than the weapons employing the gun method of combination. The reason that the implosion method is more efficient is because it not only combines the masses, but also increases the density of the mass. The neutron multiplication factor, k, of a fissionable assembly is proportional to the density squared, meaning that k goes up by a factor of four if the density is doubled. Most modern weapons use a hollow plutonium core with an implosion mechanism for detonation.

This precision compression of the pit creates a need for very precise design and machining of the pit and explosive lenses. The milling machines used are so precise that they could cut the polished surfaces of eyeglass lenses. Machining plutonium is difficult not only because of its toxicity but also because plutonium has many different metallic phases and changing phases distorts the metal.

Tamper / Neutron Reflector

In a uranium graphite chain reacting pile the critical size may be considerably reduced by surrounding the pile with a layer of graphite, since such an envelope reflects many neutrons back into the pile. A similar envelope can be used to reduce the critical size of a weapon, but here the envelope has an additional role: its very inertia delays the expansion of the reacting material. For this reason such an envelope is often called a tamper. As has already been remarked, the weapon tends to fly to bits as the reaction proceeds and this tends to stop the reaction, so the use of a tamper makes for a longer lasting, more energetic, and more efficient explosion. The most effective tamper is the one having the highest density; high tensile strength turns out to be unimportant because no material will hold together under the extreme pressures of a nuclear weapon. A coincidence that is fortunate from the point of view of the weapon designer, is that materials of high density are also excellent as reflectors of neutrons.

While the effect of a tamper is to increase the efficiency - both by reflecting neutrons and by delaying the expansion of the bomb, the effect on the efficiency is not as great as on the critical mass. The reason for this is that the process of reflection is relatively time consuming and may not occur extensively before the chain reaction is terminated.

Neutron trigger / Initiator

One of the key elements in the proper operation of a nuclear weapon is initiation of the fission chain reaction at the proper time. To obtain a significant nuclear yield of the nuclear explosive, sufficient neutrons must be present within the supercritical core at the right time. If the chain reaction starts too soon, the result will be only a 'fizzle yield,' much below the design specification; if it occurs too late, there may be no yield whatever. Several ways to produce neutrons at the appropriate moment have been developed.

Early neutron sources consisted of a highly radioactive isotope of Polonium (Po-210), which is a strong alpha emitter combined with beryllium which will absorb alphas and emit neutrons. This isotope of polonium has a half life of almost 140 days, and a neutron initiator using this material needs to have the polonium, which is generated in a nuclear reactor, to be replaced frequently. To supply the initiation pulse of neutrons at the right time, the polonium and the beryllium need to be kept apart until the appropriate moment and then thoroughly and rapidly mixed by the implosion of the weapon. This method of neutron initiation is sufficient for weapons utilizing the slower gun combination method, but the timing is not precise enough for an implosion weapon design.

Another method of providing source neutrons, is through a pulsed neutron emitter which is a small ion accelerator with a metal hydride target. When the ion source is turned on to create a plasma of deuterium or tritium, a large voltage is applied across the tube which accelerates the ions into tritium rich metal (usually scandium). The ions are accelerated so that there is a high probability of nuclear fusion occurring. The deuterium-tritium fusion reactions emit a short pulse of 14 MeV neutrons which will be sufficient to initiate the fission chain reaction. The timing of the pulse can be precisely controlled making it better suited for an implosion weapon design.

Practical Limitations of the Fission Bomb

A pure fission bomb is practically limited to a yield of a few hundred kilotons by the large amounts of fissile material needed to make a large weapon. It is technically difficult to keep a large amount of fissile material in a subcritical assembly while waiting for detonation, and it is also difficult to physically transform the subcritical assembly into a supercritical one quick enough that the device explodes rather than prematurely detonating such that a majority of the fuel is unused (inefficient predetonation). The most efficient pure fission bomb would still only consume 20% of its fissile material before being blown apart, and can often be much less efficient (Fat Man only had an efficiency of 1.4%). Large yield, pure fission weapons are also unattractive due to the weight, size and cost of using large amounts of highly enriched material.

Thermonuclear weapons (also Hydrogen bomb or Fusion bomb)

The amount of energy released by a weapon can be greatly increased by the addition of nuclear fusion reactions. Fusion releases even more energy per reaction than fission, and can also be used as a source for additional neutrons. The light weight of the elements used as fusion fuel, combined with the larger energy release, means that fusion is a very efficient fuel by weight, making it possible to build extremely high yield weapons which are still portable enough to easily deliver. Fusion is the combination of two light atoms, usually isotopes of hydrogen, to form a more stable heavy atom and release excess energy. The fusion reaction requires the atoms involved to have a high thermal energy, which is why the reaction is called thermonuclear. The extreme temperatures and densities necessary for a fusion reaction are easily generated by a fission explosion.

The simplest way to utilize fusion is to put a mixture of deuterium and tritium inside the hollow core of an implosion style plutonium pit. When the imploding fission chain reaction brings the fusion fuel to a sufficient pressure, the fusion reaction occurs fairly quickly and releases a large number of energetic neutrons into the surrounding fissile material, which allows the fissile material to burn more efficiently. The efficiency (and therefore yield) of a pure fission bomb can be doubled through the use of a fusion boosted core, with very little increase in the size and weight of the device. The amount of energy released through fusion is very small compared to the energy from fission, so the fusion chiefly increases the fission efficiency by providing a burst of additional neutrons. The fusion core of modern fusion weapons is lithium-7 deuteride.

Staged thermonuclear weapons

The basic principles behind modern thermonuclear weapons were discovered independently by scientists in different countries. Edward Teller and Stanislaw Ulam at Los Alamos worked out the idea of staged detonation coupled with radiation implosion in what is known in the United States as the Teller-Ulam design. Soviet physicist Andrei Sakharov independently arrived at the same answer (which he called his Third Idea) a short time later. A single small fission bomb, the trigger, is placed at the point of a cone-shaped arrangement of X-ray mirrors. The mirrors focus the X-rays from the fission explosive on a column of lithium deuteride. The radiation pressure of the X-rays heats and pressurizes the deuterium enough to fuse into helium, and emit copious neutrons. The neutrons transmute the lithium to tritium, which then also fuses and emits large amount of gamma rays. A heavy, U-238 cone between the fission bomb and the column prevented the premature collapse of the column by direct X-ray pressure.

Advanced Thermonuclear Weapons Designs

The largest modern fission-fusion-fission weapons include a fissionable outer shell of U-238, the more inert waste isotope of uranium, or constructed the X-ray mirrors of polished U-238. This otherwise inert U-238 would be detonated by the intense fast neutrons from the fusion stage, increasing the yield of the bomb many times. For maximum yield, however, moderately enriched uranium is preferable as a jacket material. The largest bomb ever exploded was of this type, a 50 megaton bomb named Tsar Bomba that was exploded by the Soviet Union in Novaya Zemlya.

The cobalt bomb uses cobalt in the shell, and the fusion neutrons convert the cobalt into cobalt-60, a powerful long-term (5 years) emitter of gamma rays, which produces major radioactive contamination. In general this type of weapon is a salted bomb and variable fallout effects can be obtained by using different salting isotopes. Gold has been proposed for short-term fallout (days), tantalum and zinc for fallout of intermediate duration (months), and cobalt for long term contamination (years). To be useful for salting, the parent isotopes must be abundant in the natural element, and the neutron-bred radioactive product must be a strong emitter of penetrating gamma rays.

The primary purpose of this weapon is to create extremely radioactive fallout to deny a region to an advancing army, a sort of wind-deployed mine-field. No cobalt or other salted bomb has ever been atmospherically tested, and as far as is publicly known none have ever been built. In light of the ready availability of fission-fusion-fission bombs, it is unlikely any special-purpose fallout contamination weapon will ever be developed. The British did test a bomb that incorporated cobalt as an experimental radiochemical tracer (Antler/Round 1, 14 September 1957). This 1 kt device was exploded at the Tadje site, Maralinga range, Australia. The experiment was regarded as a failure and not repeated.

The thought of using cobalt, which has the longest half-life of the feasible salting materials, caused Leó Szilárd to refer to the weapon as a potential doomsday device. With a 5yr half-life people would have to remain shielded underground for many years, effectively wiping out humanity. However this would require a massive (unrealistic) amount of such bombs, yet the public heard of it and there were numerous stories involving a single bomb wiping out the planet.

A final variant of the thermonuclear weapons is the enhanced radiation weapon, or neutron bomb which are small thermonuclear weapons in which the burst of neutrons generated by the fusion reaction is intentionally not absorbed inside the weapon, but allowed to escape. The X-ray mirrors and shell of the weapon are made of chromium or nickel so that the neutrons are permitted to escape. This intense burst of high-energy neutrons is the principle destructive mechanism. Neutrons are more penetrating than other types of radiation so many shielding materials that work well against gamma rays do not work nearly as well. The term "enhanced radiation" refers only to the burst of ionizing radiation released at the moment of detonation, not to any enhancement of residual radiation in fallout (as in the salted bombs discussed above).

Neutron bombs could be used as strategic anti-missile weapons, and as tactical weapons intended for use against armored forces. As an anti-missile weapon ER weapons were developed to protect U.S. ICBM silos from incoming Soviet warheads by damaging the nuclear components of the incoming warhead with the intense neutron flux. Tactical neutron bombs are primarily intended to kill soldiers who are protected by armor. Armored vehicles are extremely resistant to blast and heat produced by nuclear weapons, so the effective range of a nuclear weapon against tanks is determined by the lethal range of the radiation, although this is also reduced by the armor. By emitting large amounts of lethal radiation of the most penetrating kind, ER warheads maximize the lethal range of a given yield of nuclear warhead against armored targets.

One problem with using radiation as a tactical anti-personnel weapon is that to bring about rapid incapacitation of the target, a radiation dose that is many times the lethal level must be administered. A radiation dose of 600 rads is normally considered lethal (it will kill at least half of those who are exposed to it), but no effect is noticeable for several hours. Neutron bombs were intended to deliver a dose of 8000 rads to produce immediate and permanent incapacitation. A 1 kt ER warhead can do this to a T-72 tank crew at a range of 690 m, compared to 360 m for a pure fission bomb. For a "mere" 600 rad dose the distances are 1100 m and 700 m respectively, and for unprotected soldiers 600 rad exposures occur at 1350 m and 900 m. The lethal range for tactical neutron bombs exceeds the lethal range for blast and heat even for unprotected troops.

The neutron flux can induce significant amounts of short lived secondary radioactivity in the environment in the high flux region near the burst point. The alloy steels used in armor can develop radioactivity that is dangerous for 24-48 hours. If a tank exposed to a 1 kt neutron bomb at 690 m (the effective range for immediate crew incapacitation) is immediately occupied by a new crew, they will receive a lethal dose of radiation within 24 hours.

Some authorities say that due to the rapid attenuation of neutron energy by the atmosphere (it drops by a factor of 10 every 500 m in addition to the effects of spreading) ER weapons are only effective at short ranges, and thus are practical only in relatively low yields. These ER warheads are said to be designed to minimize the amount of fission energy and blast effect produced relative to the neutron yield. The principal reason is said to be to allow their use close to friendly forces.

These same authorities say that the common perception of the neutron bomb as a "landlord bomb" that would kill people but leave buildings undamaged is greatly overstated. At the conventional effective combat range (690 m) the blast from a 1 kt neutron bomb will destroy or damage to the point of inutility almost any civilian building. Thus the use of neutron bombs to stop an enemy attack, which requires exploding large numbers of them to blanket the enemy forces, would also destroy all buildings in the area.

Another view of the neutron bomb and its tactics exists. The inventor of the neutron bomb, Samuel Cohen, wrote a book in which he stated that the effective range of a pure neutron bomb exceeded 10 Km of altitude. Samuel Cohen stated explicitly that "enhanced radiation" weapons deployed in Germany during the cold war were political compromises designed to have substantial blast, with radiation effects deliberately reduced to eliminate any possibility of surviving structures. He also quoted radiation releases of 100KRads at the ground from pure neutron weapons exploded at 10Km.

The neutron absorption spectra of air is disputed by some authorities, and may depend in part on absorption by hydrogen from water vapor. It therefore might vary exponentially with humidity, making high-altitude neutron bombs immensely more deadly in desert climates than in humid ones. This effect also varies with altitude.

According to Samuel Cohen, one possible tactic of using such "true" neutron bombs is therefore to launch them as defensive weapons against armored attacks. Civilians enter radiation shelters, and the bomb is exploded 10Km over the armored attack. Portable armor is said to be unable to shield tank and aircraft crews. In such an event, a city's trees and grass would have been killed by radiation, but buildings would remain undamaged for the emerging civilians.

Such neutron bombs would be very potent anti-ship weapons. A major support of Cohen's research was the U.S. Navy.

References

• Glasstone, Samuel and Dolan, Philip J., The Effects of Nuclear Weapons (third edition), U.S. Government Printing Office, 1977. PDF Version
• Nuclear Weapon Archive from Carey Sublette is a reliable source of information and has links to other sources.
• The Federation of American Scientists provide solid information on weapons of mass destruction, including nuclear weapons and their effects
• Cohen, Sam, The Truth About the Neutron Bomb: The Inventor of the Bomb Speaks Out, William Morrow & Co., 1983
• Militarily Critical Technologies List (MCTL) from the US Government's Defense Technical Information Center
• Grace, S. Charles, Nuclear Weapons: Principles, Effects and Survivability (Land Warfare: Brassey's New Battlefield Weapons Systems and Technology, vol 10)
• Smyth, H. DeW., Atomic Energy for Military Purposes, Princeton University Press, 1945.
• The Effects of Nuclear War, Office of Technology Assessment (May 1979).
• Rhodes, Richard. Dark Sun: The Making of the Hydrogen Bomb. Simon and Schuster, New York, (1995 ISBN 0684824140)
• Rhodes, Richard. The Making of the Atomic Bomb. Simon and Schuster, New York, (1986 ISBN 0684813785)

• Nuclear weapons