How a Nuclear Bomb Works

We have seen that these devices have incredible destructive power, but how do they work? In this article, you will learn about the physics that makes a nuclear bomb so powerful, how nuclear bombs are designed and what happens after a nuclear explosion.

Nuclear bombs involve the forces, strong and weak, that hold the nucleus of an atom together, especially atoms with unstable nuclei (see How Nuclear Radiation Works for details). There are two basic ways that nuclear energy can be released from an atom:

• Nuclear fission - You can split the nucleus of an atom into two smaller fragments with a neutron. This method usually involves isotopes of uranium (uranium-235, uranium-233) or plutonium-239.
• Nuclear fusion -You can bring two smaller atoms, usually hydrogen or hydrogen isotopes (deuterium, tritium), together to form a larger one (helium or helium isotopes); this is how the sun produces energy.

In either process, fission or fusion, large amounts of heat energy and radiation are given off.

To build an atomic bomb, you need:

• A source of fissionable or fusionable fuel
• A triggering device
• A way to allow the majority of fuel to fission or fuse before the explosion occurs (otherwise the bomb will fizzle out)

The first nuclear bombs were fission devices, and the later fusion bombs required a fission-bomb trigger. We will discuss the designs of the following devices:

• Fission bombs (in general)
• Gun-triggered fission bomb (Little Boy), which was detonated over Hiroshima, Japan, in 1945
• Implosion-triggered fission bomb (Fat Man), which was detonated over Nagasaki, Japan, in 1945
• Fusion bombs (in general)
• Teller-Ulam design of a hydrogen fusion bomb, which was test-detonated on Elugelap Island in 1952

A fission bomb uses an element like uranium-235 to create a nuclear explosion. If you have read How Nuclear Radiation Works, then you understand the basic process behind radioactive decay and fission. Uranium-235 has an extra property that makes it useful for both nuclear-power production and nuclear-bomb production -- U-235 is one of the few materials that can undergo induced fission. If a free neutron runs into a U-235 nucleus, the nucleus will absorb the neutron without hesitation, become unstable and split immediately.

This figure shows a uranium-235 nucleus with a neutron approaching from the top. As soon as the nucleus captures the neutron, it splits into two lighter atoms and throws off two or three new neutrons (the number of ejected neutrons depends on how the U-235 atom happens to split). The two new atoms then emit gamma radiation as they settle into their new states (see How Nuclear Radiation Works). There are three things about this induced fission process that make it interesting:

• The probability of a U-235 atom capturing a neutron as it passes by is fairly high. In a bomb that is working properly, more than one neutron ejected from each fission causes another fission to occur. This condition is known as supercriticality.
• The process of capturing the neutron and splitting happens very quickly, on the order of picoseconds (1*10E-12 seconds).
• An incredible amount of energy is released, in the form of heat and gamma radiation, when an atom splits. The energy released by a single fission is due to the fact that the fission products and the neutrons, together, weigh less than the original U-235 atom.
• The difference in weight is converted to energy at a rate governed by the equation e = m * c^2. A pound of highly enriched uranium as used in a nuclear bomb is equal to something on the order of a million gallons of gasoline. When you consider that a pound of uranium is smaller than a baseball and a million gallons of gasoline would fill a cube that is 50 feet per side (50 feet is as tall as a five-story building), you can get an idea of the amount of energy available in just a little bit of U-235.

Critical Mass
In a fission bomb, the fuel must be kept in separate subcritical masses, which will not support fission, to prevent premature detonation. Critical mass is the minimum mass of fissionable material required to sustain a nuclear fission reaction. This separation brings about several problems in the design of a fission bomb that must be solved:

• The two or more subcritical masses must be brought together to form a supercritical mass, which will provide more than enough neutrons to sustain a fission reaction, at the time of detonation.
• Free neutrons must be introduced into the supercritical mass to start the fission.
• As much of the material as possible must be fissioned before the bomb explodes to prevent fizzle.

• Gun-triggered
• Implosion

1. The foil is broken when the subcritical masses come together and polonium spontaneously emits alpha particles.
2. These alpha particles then collide with beryllium-9 to produce beryllium-8 and free neutrons.
3. The neutrons then initiate fission.

Types of Bombs
Gun-triggered Fission Bomb
The simplest way to bring the subcritical masses together is to make a gun that fires one mass into the other. A sphere of U-235 is made around the neutron generator and a small bullet of U-235 is removed. The bullet is placed at the one end of a long tube with explosives behind it, while the sphere is placed at the other end. A barometric-pressure sensor determines the appropriate altitude for detonation and triggers the following sequence of events:

1. The explosives fire and propel the bullet down the barrel.
2. The bullet strikes the sphere and generator, initiating the fission reaction.
3. The fission reaction begins.
4. The bomb explodes.

Little Boy was this type of bomb and had a 14.5-kiloton yield (equal to 14,500 tons of TNT) with an efficiency of about 1.5 percent. That is, 1.5 percent of the material was fissioned before the explosion carried the material away.

Implosion-Triggered Fission Bomb
Early in the Manhattan Project, the secret U.S. program to develop the atomic bomb, scientists working on the project recognized that compressing the subcritical masses together into a sphere by implosion might be a good way to make a supercritical mass. There were several problems with this idea, particularly how to control and direct the shock wave uniformly across the sphere. But the Manhattan Project team solved the problems. The implosion device consisted of a sphere of uranium-235 (tamper) and a plutonium-239 core surrounded by high explosives. When the bomb was detonated, this is what happened:

• The explosives fired, creating a shock wave.
• The shock wave compressed the core.
• The fission reaction began.
• The bomb exploded.

Fat Man was this type of bomb and had a 23-kiloton yield with an efficiency of 17 percent. These bombs exploded in fractions of a second. The fission usually occurred in 560 billionths of a second.

Modern Implosion-Triggered Design
In a later modification of the implosion-triggered design, here is what happens:

• The explosives fire, creating a shock wave.
• The shock wave propels the plutonium pieces together into a sphere.
• The plutonium pieces strike a pellet of beryllium/polonium at the center.
• The fission reaction begins.
• The bomb explodes.

Fusion Bombs
Fission bombs worked, but they weren't very efficient. Fusion bombs, also called thermonuclear bombs, have higher kiloton yields and greater efficiencies than fission bombs. To design a fusion bomb, some problems have to be solved:

• Deuterium and tritium, the fuel for fusion, are both gases, which are hard to store.
• Tritium is in short supply and has a short half-life, so the fuel in the bomb would have to be continuously replenished.
• Deuterium or tritium has to be highly compressed at high temperature to initiate the fusion reaction.

Teller-Ulam Design of a Fusion Bomb
To understand this bomb design, imagine that within a bomb casing you have an implosion fission bomb and a cylinder casing of uranium-238 (tamper). Within the tamper is the lithium deuteride (fuel) and a hollow rod of plutonium-239 in the center of the cylinder. Separating the cylinder from the implosion bomb is a shield of uranium-238 and plastic foam that fills the remaining spaces in the bomb casing. Detonation of the bomb caused the following sequence of events:

1. The fission bomb imploded, giving off X-rays.
2. These X-rays heated the interior of the bomb and the tamper; the shield prevented premature detonation of the fuel.
3. The heat caused the tamper to expand and burn away, exerting pressure inward against the lithium deuterate.
4. The lithium deuterate was squeezed by about 30-fold.
5. The compression shock waves initiated fission in the plutonium rod.
6. The fissioning rod gave off radiation, heat and neutrons.
7. The neutrons went into the lithium deuterate, combined with the lithium and made tritium.
8. The combination of high temperature and pressure were sufficient for tritium-deuterium and deuterium-deuterium fusion reactions to occur, producing more heat, radiation and neutrons.
9. The neutrons from the fusion reactions induced fission in the uranium-238 pieces from the tamper and shield.
10. Fission of the tamper and shield pieces produced even more radiation and heat.
11. The bomb exploded.

All of these events happened in about 600 billionths of a second (550 billionths of a second for the fission bomb implosion, 50 billionths of a second for the fusion events). The result was an immense explosion that was more than 700 times greater than the Little Boy explosion: It had a 10,000-kiloton yield.

Consequences and Health Risks
The detonation of a nuclear bomb over a target such as a populated city causes immense damage. The degree of damage depends upon the distance from the center of the bomb blast, which is called the hypocenter or ground zero. The closer one is to the hypocenter, the more severe the damage. The damage is caused by several things:

• A wave of intense heat from the explosion
• Pressure from the shock wave created by the blast
• Radiation
• Radioactive fallout (clouds of fine radioactive particles of dust and bomb debris that fall back to the ground)

Scientists have studied survivors of the Hiroshima and Nagasaki bombings to understand the short-term and long-term effects of nuclear explosions on human health. Radiation and radioactive fallout affect those cells in the body that actively divide (hair, intestine, bone marrow, reproductive organs). Some of the resulting health conditions include:

• Nausea, vomiting and diarrhea
• Cataracts
• Hair loss
• Loss of blood cells

• Leukemia
• Cancer
• Infertility
• Birth defects

Scientists and physicians are still studying the survivors of the bombs dropped on Japan and expect more results to appear over time.

In the 1980s, scientists assessed the possible effects of nuclear warfare (many nuclear bombs exploding in different parts of the world) and proposed the theory that a nuclear winter could occur. In the nuclear-winter scenario, the explosion of many bombs would raise great clouds of dust and radioactive material that would travel high into Earth's atmosphere. These clouds would block out sunlight. The reduced level of sunlight would lower the surface temperature of the planet and reduce photosynthesis by plants and bacteria. The reduction in photosynthesis would disrupt the food chain, causing mass extinction of life (including humans). This scenario is similar to the asteroid hypothesis that has been proposed to explain the extinction of the dinosaurs. Proponents of the nuclear-winter scenario pointed to the clouds of dust and debris that traveled far across the planet after the volcanic eruptions of Mount St. Helens in the United States and Mount Pinatubo in the Philippines.

Nuclear weapons have incredible, long-term destructive power that travels far beyond the original target. This is why the world's governments are trying to control the spread of nuclear-bomb-making technology and materials and reduce the arsenal of nuclear weapons deployed during the Cold War.