- This article is about the radioactive element. For other meanings, see Plutonium (disambiguation).
|
|
| General |
| Name, Symbol,
Number |
plutonium, Pu, 94 |
| Chemical series |
actinides |
| Group, Period,
Block |
n/a, 7,
f |
| Appearance |
silvery white
 |
| Standard atomic weight |
(244) g·mol−1 |
| Electron configuration |
[Rn] 5f6 7s2 |
| Electrons per shell |
2, 8, 18, 32, 24, 8, 2 |
| Physical properties |
| Phase |
solid |
| Density (near r.t.) |
19.816 g·cm−3 |
| Liquid density at m.p. |
16.63 g·cm−3 |
| Melting point |
912.5 K
(639.4 °C, 1182.9 °F) |
| Boiling point |
3505 K
(3228 °C, 5842 °F) |
| Heat of fusion |
2.82 kJ·mol−1 |
| Heat of vaporization |
333.5 kJ·mol−1 |
| Heat capacity |
(25 °C) 35.5 J·mol−1·K−1 |
Vapor pressure
| P(Pa) |
1 |
10 |
100 |
1 k |
10 k |
100 k |
| at T(K) |
1756 |
1953 |
2198 |
2511 |
2926 |
3499 |
|
| Atomic properties |
| Crystal structure |
monoclinic |
| Oxidation states |
6, 5, 4, 3
(amphoteric oxide) |
| Electronegativity |
1.28 (scale Pauling) |
| Ionization energies |
1st: 584.7 kJ/mol |
| Atomic radius |
175 pm |
| Miscellaneous |
| Magnetic ordering |
no data |
| Electrical resistivity |
(0 °C) 1.460 µΩ·m |
| Thermal conductivity |
(300 K) 6.74 W·m−1·K−1 |
| Thermal expansion |
(25 °C) 46.7 µm·m−1·K−1 |
| Speed of sound (thin rod) |
(20 °C) 2260 m/s |
| Young's modulus |
96 GPa |
| Shear modulus |
43 GPa |
| Poisson ratio |
0.21 |
| CAS registry number |
7440-07-5 |
| Selected isotopes |
|
|
| References |
Plutonium (IPA: /ˌpluːˈtəʊniəm/) is a radioactive, metallic
chemical element. It has the symbol Pu and the atomic number 94. It is the element used in most modern nuclear
weapons. The most significant isotope of plutonium is 239Pu, with a
half-life of 24,100 years. It can be made from natural uranium and is fissile. The most stable isotope is 244Pu, with a
half-life of about 80 million years, long enough to be found in extremely small quantities in nature. In fact, 244Pu
is the nucleon-richest atom that naturally occurs in the Earth's crust, albeit in small traces.[1]
Notable characteristics
Plutonium has been called "the most complex metal" and "a physicist's dream but an engineer's nightmare"[2] for its peculiar physical and chemical properties. It has six
allotropes normally and a seventh under pressure, each of which have very similar energy
levels but with significantly varying densities, making it very sensitive to changes in temperature, pressure, or chemistry, and
allowing for dramatic volume changes following phase transitions (in nuclear applications, it is usually alloyed with small amounts of gallium, which stabilizes it in the
delta-phase.)[3] Plutonium is
silvery in pure form, but has a yellow tarnish when oxidized. It is also notable in that it
possesses a low-symmetry structure causing it to become progressively more brittle over time.[4] Because it self-irradiates, it ages both from the outside-in and the
inside-out.[3] However,
self-irradiation can also lead to annealing which counteracts some of the aging
effects. In general, the precise aging properties of plutonium are very complex and poorly understood, greatly complicating
efforts to predict future reliability of weapons components.
The heat given off by alpha particle emission makes plutonium warm to the touch in
reasonable quantities; larger amounts can boil water.[citation needed] It displays five ionic oxidation
states in aqueous solution:
- Pu(III), as Pu3+ (blue lavender)
- Pu(IV), as Pu4+ (yellow brown)
- Pu(V), as PuO2+ (thought to be pink; this ion is unstable in solution and will disproportionate into
Pu4+ and PuO22+; the Pu4+ will then oxidize the remaining PuO2+
to PuO22+, being reduced in turn to Pu3+. Thus, aqueous solutions of plutonium tend over time
towards a mixture of Pu3+ and PuO22+.)[5]
- Pu(VI), as PuO22+ (pink orange)
- Pu(VII), as PuO52- (dark red); the heptavalent ion is rare and prepared only under extreme oxidizing
conditions.
The actual color shown by Pu solutions depends on both the oxidation state and the nature of the acid anion, which influences
the degree of complexing of the Pu species by the acid anion.[6]
Applications
The isotope 239Pu is a key fissile component in nuclear weapons, due to its ease of fissioning and availability. 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. The Manhattan
Project "Fat Man" type plutonium bombs, using explosive compression of Pu to
significantly higher densities than normal, were able to function with plutonium cores of only 6.2 kg.[7] Complete detonation of plutonium will produce an explosion equivalent to the
explosion of 20 kilotons of trinitrotoluene (TNT) per
kilogram.[citation needed] (See also nuclear weapon design.) However, complete detonation requires an additional neutron source (often
from a small amount of fusion fuel), and primitive bombs may be far less efficient. For example, despite the 6.2 kg of plutonium,
the Fat Man yield was only 21 kt.
The isotope plutonium-238 (238Pu) has a half-life of 88 years and emits a
large amount of thermal energy as it decays. Being an alpha emitter it combines high energy radiation with low penetration (thereby requiring minimal
shielding). These characteristics make it well suited for safe electrical power generation for devices which must function
without direct maintenance for timescales approximating a human lifetime. It is therefore used in radioisotope thermoelectric generators such as those powering the Cassini and New Horizons (Pluto) space probes; earlier versions of
the same technology powered the ALSEP and EASEP systems including seismic experiments
on the Apollo Moon missions.
238Pu has been used successfully to power artificial heart pacemakers, to reduce the risk of repeated surgery. It has been largely replaced by
lithium based primary cells, but as of 2003 there were
somewhere between 50 and 100 plutonium-powered pacemakers still implanted and functioning in living patients.
History
The production of plutonium and neptunium by bombarding uranium-238 with neutrons was predicted in 1940 by two teams working independently: Edwin M. McMillan and Philip Abelson at Berkeley Radiation Laboratory at the University of California, Berkeley and by Egon
Bretscher and Norman Feather at the Cavendish Laboratory at University of Cambridge. Coincidentally both teams proposed the same names to follow on from
uranium, like the sequence of the outer planets.
First isolation
Plutonium was first produced and isolated on February 23, 1941 by Dr. Glenn T. Seaborg, Edwin M.
McMillan, J. W. Kennedy, and A. C. Wahl by
deuteron bombardment of uranium in the 60-inch cyclotron at Berkeley. The discovery was kept
secret due to the war. It was named after Pluto, having been
discovered directly after neptunium (which itself was one higher on the periodic table than
uranium), by analogy to solar system planet order as Pluto was considered to be a planet at the
time (though technically it should have been "plutium", Seaborg said that he did not think it sounded as good as "plutonium").
Seaborg chose the letters "Pu" as a joke, which passed without notice into the periodic table.[8] Originally, Seaborg and others thought about naming the element "ultinium" or
"extremium" because they believed at the time that they had found the last possible element on the periodic table.[9]
Chemists at the University of Chicago began to study the newly manufactured
radioactive element. The George Herbert Jones Laboratory at the
university was the site where, on 18 August 1942, a trace quantity of this new element was isolated and measured for the first
time. This procedure enabled chemists to determine the new element's atomic weight. Room 405 of the building was named a
National Historic Landmark in May 1967.[10]
Production
During the Manhattan Project, the first production reactor, the X-10 Graphite Reactor, was built at the Oak Ridge,
Tennessee site that later became Oak Ridge
National Laboratory. Later, large (200MWt) reactors were set up in
Hanford, Washington, for the production of plutonium, which was used in the first atomic
bomb used at the "Trinity" test in July 1945. Plutonium was also used in the
"Fat Man" bomb dropped on Nagasaki, Japan in August 1945. The
"Little Boy" bomb dropped on Hiroshima utilized
uranium-235, not plutonium.
Large stockpiles of "weapons-grade" plutonium were built up by both the Soviet Union and
the United States during the Cold War. The U.S. reactors
at Hanford and the Savannah River Site in
South Carolina produced 103,000 kg;[11] It was estimated
there are another 170,000 kg of military plutonium in Russia, with 300,000 kg accumulated worldwide. [12] Since the end of the Cold War, these stockpiles have become a focus of
nuclear proliferation concerns. In 2002, the United States Department of Energy took possession of 34 metric tons of excess
weapons-grade plutonium stockpiles from the United States Department of
Defense, and as of early 2003 was considering converting several nuclear power plants in the US from enriched uranium fuel to MOX fuel as a means of disposing of
plutonium stocks.
Medical experimentation
During the initial years after the discovery of plutonium, when its biological and physical properties were very poorly
understood, a series of human radiation experiments were performed by the
U.S. government and by private organizations acting on its behalf. During and after the end of World War II, scientists working
on the Manhattan Project and other nuclear weapons research projects conducted studies
of the effects of plutonium on laboratory animals and human subjects. In the case of human subjects, this involved injecting
solutions containing (typically) five micrograms of plutonium into hospital patients thought to be either terminally ill, or to
have a life expectancy of less than ten years either due to age or chronic disease condition. These eighteen injections were made
without the informed consent of those patients and were not done with the belief that
the injections would heal their conditions; rather, they were used to develop diagnostic tools for determining the uptake of
plutonium in the body for use in developing safety standards for people working with plutonium during the course of developing
nuclear weapons.[13]
The episode is now considered to be a serious breach of medical ethics and of the Hippocratic Oath, and has been sharply criticised as failing "both the test of our national values and
the test of humanity."[14] More sympathetic commentators
have noted that while it was definitely a breach in trust and ethics, "the effects of the plutonium injections were not as
damaging to the subjects as the early news stories painted, nor were they so inconsequential as many scientists, then and now,
believe."[15]
Occurrence
While almost all plutonium is manufactured synthetically, extremely tiny trace amounts are found naturally in uranium ores. These come about by a process of neutron capture by
238U nuclei, initially forming 239U; two subsequent beta decays then
form 239Pu (with a 239Np intermediary), which has a half-life of 24,110
years. This is also the process used to manufacture 239Pu in nuclear
reactors. Some traces of 244Pu remain from the birth of the solar system from the waste of supernovae, because
its half-life of 80 million years is fairly long.
A relatively high concentration of plutonium was discovered at the natural
nuclear fission reactor in Oklo, Gabon in 1972. Since 1945,
approximately 7700 kg has been released onto Earth through nuclear explosions.
Manufacture
Pu-240, Pu-241 and Pu-242
The activation cross section for 239Pu is 270 barns while the fission cross section is 747 barns for thermal neutrons. The higher plutonium isotopes are
created when the uranium fuel is used for a long time. It is the case that for high burnup used fuel that the concentrations of
the higher plutonium isotopes will be higher than the low burnup fuel which is reprocessed to obtain bomb grade plutonium.
The formation of 240Pu, 241Pu and 242Pu from 238U
| Element |
Isotope |
Thermal neutron
cross section |
decay mode |
halflife |
| U |
238 |
2.7 |
α |
4.47 x 109 years |
| U |
239 |
- |
β |
23 minutes |
| Np |
239 |
- |
β |
2.36 days |
| Pu |
239 |
270 (capture) |
α |
24110 years |
| Pu |
240 |
289 (capture) |
α |
6564 years |
| Pu |
241 |
362 (capture) |
β |
14.35 years |
| Pu |
242 |
18.8 |
α |
373300 years |
Pu-239
-
Plutonium-239 is one of the three fissile materials used for the production of
nuclear weapons and in some nuclear
reactors as a source of energy. The other fissile materials are uranium-235 and
uranium-233. Plutonium-239 is virtually nonexistent in nature. It is made by bombarding
uranium-238 with neutrons in a nuclear reactor. Uranium-238 is present in quantity in most
reactor fuel; hence plutonium-239 is continuously made in these reactors. Since plutonium-239 can itself be split by
neutrons to release energy, plutonium-239 provides a portion of the energy
generation in a nuclear reactor.
A ring of weapons-grade electrorefined plutonium, with 99.96% purity. This 5.3 kg ring is enough plutonium for use in a modern
nuclear weapon.
It is clear to see that with a low flux of neutrons that 238U will be converted into 239Pu
Pu-238
-
There are small amounts of Pu-238 in the plutonium of usual plutonium-producing reactors. However, isotopic separation would
be quite expensive compared to another method: when a U-235 atom captures a neutron, it is converted to an excited state of
U-236. Some of the excited U-236 nuclei undergo fission, but some decay to the ground state of U-236 by emitting gamma radiation.
Further neutron capture creates U-237 which has a half-life of 7 days and thus quickly decays to Np-237. Since nearly all neptunium is produced in this way or consists of isotopes which decay quickly, one
gets nearly pure Np-237 by chemical separation of neptunium. After this chemical separation, Np-237 is again irradiated by
reactor neutrons to be converted to Np-238 which decays to Pu-238 with a half-life of 2 days.
Compounds
Plutonium reacts readily with oxygen, forming PuO and PuO2, as well as intermediate oxides. It reacts with the halogens, giving rise to compounds such as PuX3 where X can be F, Cl, Br or I; PuF4 and PuF6 are also seen. The following oxyhalides are observed: PuOCl,
PuOBr and PuOI. It will react with carbon to form PuC, nitrogen
to form PuN and silicon to form PuSi2.
Plutonium like other actinides readily forms a dioxide plutonyl core (PuO2). In the environment, this plutonyl core
readily complexes with carbonate as well as other oxygen moieties (OH-, NO2-,
NO3-, and SO4-2) to form charged complexes which can be readily mobile with low
affinities to soil.
- PuO2(CO3)1-2
- PuO2(CO3)2-4
- PuO2(CO3)3-6
PuO2 formed from neutralizing highly acidic nitric acid solutions tends to form polymeric PuO2 which is
resistant to complexation. Plutonium also readily shifts valences between the +3, +4, +5 and +6 states. It is common for some
fraction of plutonium in solution to exist in all of these states in equilibrium.
Image showing colors of various oxidation states of Pu in solution on the left and colors of only one Pu oxidation state (IV) on
the right in solutions containing different anions.
Allotropes
A diagram of the allotropes of plutonium at ambient pressure
Even at ambient pressure, plutonium occurs in a variety of allotropes. These allotropes
differ widely in crystal structure and density; the α and δ allotropes differ in density by more than 25% at constant
pressure.
The presence of these many allotropes makes machining plutonium very difficult, as it changes state very readily. The reasons
for the complicated phase diagram are not entirely understood; recent research has focused on constructing accurate computer
models of the phase transitions.
In weapons applications, plutonium is often alloyed with another metal (e.g., delta phase with
a small percentage of gallium) to increase phase stability and thereby enhance workability and
ease of handling. Interestingly, in fission weapons, the explosive shock waves used to
compress a plutonium core will also cause a transition from the usual delta phase plutonium to the denser alpha phase,
significantly helping to achieve supercriticality.
Isotopes
-
Twenty-one plutonium radioisotopes have been characterized. The most stable are Pu-244,
with a half-life of 80.8 million years, Pu-242, with a half-life of 373,300 years, and Pu-239,
with a half-life of 24,110 years. All of the remaining radioactive isotopes have half-lives
that are less than 7,000 years. This element also has eight meta states, though none are
very stable (all have half-lives less than one second).
The isotopes of plutonium range in atomic weight from 228.0387 u (Pu-228) to 247.074 u (Pu-247). The primary decay modes
before the most stable isotope, Pu-244, are spontaneous fission and alpha emission; the primary mode after is beta emission. The primary
decay products before Pu-244 are uranium and neptunium isotopes (neglecting the wide range
of daughter nuclei created by fission processes), and the primary products after are americium
isotopes.
A pellet of plutonium-238, glowing under its own light, used for
radioisotope thermoelectric generators.
Key isotopes for applications are Pu-239, which is suitable for use in nuclear weapons and nuclear reactors, and Pu-238, which
is suitable for use in radioisotope thermoelectric generators; see
above for more details. The isotope Pu-240 undergoes spontaneous fission very readily, and is produced when Pu-239 is exposed to
neutrons. The presence of Pu-240 in a material limits its nuclear bomb potential since it emits neutrons randomly, increasing the
difficulty of initiating accurately the chain reaction at the desired instant and thus
reducing the bomb's reliability and power. Plutonium consisting of more than about 90% Pu-239 is called weapon-grade
plutonium; plutonium obtained from commercial reactors generally contains at least 20% Pu-240 and is called reactor-grade
plutonium.
Pu-240, while of little importance by itself, plays a crucial role as a contaminant in plutonium used in nuclear weapons. It
spontaneously fissions at a high rate, and as a 1% impurity in Pu-239 will lead to unacceptably early initiation of a fission
chain reaction in gun-type atomic weapons, blowing the weapon apart before much of its material can fission. Pu-240 contamination
is the reason plutonium weapons must use an implosion design. A theoretical 100% pure Pu-239 weapon could be constructed as a gun
type device, but achieving this level of purity is prohibitively difficult. Pu-240 contamination has proven a mixed blessing to
weapons designers. While it created delays and headaches during the Manhattan Project because of the need to develop implosion
technology, those very same difficulties are currently a barrier to nuclear proliferation. Implosion devices are also inherently
more efficient and less prone toward accidental detonation than are gun-type weapons.
Precautions
Toxicity
All isotopes and compounds of plutonium are toxic and radioactive. While plutonium is sometimes described in media reports as
"the most toxic substance known to man", from the standpoint of actual chemical or radiological
toxicity this is incorrect. When taken in by mouth, plutonium is less poisonous than if
inhaled, since it is not absorbed into the body efficiently when ingested. The U.S. Department of energy estimates the increase
in lifetime cancer risk for inhaled plutonium as 3 10-8 pCi-1.[16] (This means that inhaling 1μCi is estimated to increase one's lifetime risk of
developing cancer as a result of the exposure to 3%.) When plutonium is absorbed into the body, it is excreted very slowly, with
a biological half-life of 200 years.[17]
From a purely chemical standpoint, it is about as poisonous as lead and other heavy metals. [citation needed] Not surprisingly, it has a metallic taste.[18]
Glowing hot bits of plutonium in a box, which have been set alight due to plutonium's
pyrophoric nature.
Plutonium may be extremely dangerous when handled incorrectly. The alpha radiation it
emits does not penetrate the skin, but can irradiate internal organs when plutonium is inhaled or ingested. Particularly at risk
are the skeleton, where it is likely to be absorbed by the bone surface, and the
liver, where it will likely collect and become concentrated. Approximately 0.008 microcuries
absorbed in bone marrow is the maximum withstandable dose. Anything more is considered toxic. Extremely fine particles of
plutonium (on the order of micrograms) can cause lung cancer if inhaled.[citation needed]
Other substances including ricin, tetrodotoxin,
botulinum toxin, and tetanus toxin are fatal in doses
of (sometimes far) under one milligram, and others (the nerve agents, the amanita toxin) are in the range of a few milligrams. As such, plutonium is not unusual in terms of toxicity,
even by inhalation. In addition, those substances are fatal in hours to days, whereas plutonium (and other cancer-causing
radioactives) give an increased chance of illness decades in the future. Considerably larger amounts may cause acute
radiation poisoning and death if ingested or inhaled; however, so far, no human is
known to have immediately died because of inhaling or ingesting plutonium and many people have measurable amounts of plutonium in
their bodies.[citation needed]
Disposal difficulties
In contrast to naturally occurring radioisotopes such as radium or C-14, plutonium was manufactured, concentrated, and isolated in large amounts (hundreds of metric tons) during
the Cold War for weapons production. These stockpiles, whether or not in weapons form, pose a
significant problem because, unlike chemical or biological agents, no chemical process can destroy them. One proposal to dispose
of surplus weapons-grade plutonium is to mix it with highly radioactive isotopes (e.g., spent reactor fuel) to deter handling by
potential thieves or terrorists. Another is to mix it with uranium and use it to fuel nuclear power reactors (the mixed
oxide or MOX approach). This would not only fission (and thereby destroy) much of the
Pu-239, but also transmute a significant fraction of the remainder into Pu-240 and heavier isotopes that would make the resulting
mixture useless for nuclear weapons.[19]
Criticality potential
Toxicity issues aside, care must be taken to avoid the accumulation of amounts of plutonium which approach critical mass, particularly because plutonium's critical mass is only a third of that of uranium-235's.
Despite not being confined by external pressure as is required for a nuclear weapon, it will nevertheless heat itself and break
whatever confining environment it is in. Shape is relevant; compact shapes such as spheres are to be avoided. Plutonium in
solution is more likely to form a critical mass than the solid form (due to moderation by the hydrogen in water). A weapon-scale
nuclear explosion cannot occur accidentally, since it requires a greatly supercritical mass in order to explode rather than
simply melt or fragment. However, a marginally critical mass will cause a lethal dose of radiation and has in fact done so in the
past on several occasions.
Criticality accidents have occurred in the past, some of them with lethal
consequences. Careless handling of tungsten carbide bricks around a 6.2 kg plutonium sphere resulted in a lethal dose of
radiation at Los Alamos on August 21,
1945, when scientist Harry K. Daghlian, Jr.
received a dose estimated to be 510 rems (5.1 Sv) and died four weeks later. Nine months later, another Los Alamos scientist, Louis Slotin, died from a similar accident involving a beryllium reflector and the same plutonium core (the
so-called "demon core") that had previously claimed the life of Daghlian. These incidents were fictionalized in the 1989 film
Fat Man and Little Boy. In 1958, during a process of purifying plutonium
at Los Alamos, a critical mass was formed in a mixing vessel, which resulted in the death of a crane operator. Other accidents of
this sort have occurred in the Soviet Union, Japan, and many
other countries. (See List of nuclear accidents.) The 1986
Chernobyl accident caused a minor
release of plutonium.[citation needed]
Flammability
Metallic plutonium is also a fire hazard, especially if the material is finely divided. It reacts chemically with oxygen and
water which may result in an accumulation of plutonium hydride, a pyrophoric substance; that is, a material that will ignite in air at room temperature. Plutonium expands
considerably in size as it oxidizes and thus may break its container. The radioactivity of the burning material is an additional
hazard. Magnesium oxide sand is the most effective material for extinguishing a plutonium fire. It cools the burning material,
acting as a heat sink, and also blocks off oxygen. There was a major plutonium-initiated fire
at the Rocky Flats Plant near Boulder,
Colorado in 1969.[20]
To avoid these problems, special precautions are necessary to store or handle plutonium in any form; generally a dry
inert atmosphere is required.[21]
See also
References
- ^
Levine, Charles A. & Glenn T., Seaborg,
(1950), The Occurrence of Plutonium in Nature, Radiation Laboratory, University of California,
<http://www.osti.gov/energycitations/product.biblio.jsp?osti_id=4429051>
- ^ Siegfried S. Hecker (2000). "Plutonium: An element at odds with itself" (PDF). Los Alamos Science 26:
16–23, on 16.
- ^ a b Siegfried S. Hecker (2000). "Plutonium and its alloys: from
atoms to microstructure" (PDF). Los Alamos Science 26: 290–335.
- ^ Lawrence Livermore National Laboratory (2006). Scientists resolve
60-year-old plutonium questions. Retrieved on 2006-06-06.
- ^ Crooks, William J. (2002). Nuclear Criticality Safety Engineering Training
Module 10 - Criticality Safety in Material Processing Operations, Part 1 (PDF). Retrieved on 2006-02-15.
- ^ Matlack, George: A Plutonium Primer: An Introduction to Plutonium Chemistry
and its Radioactivity (LA-UR-02-6594)
- ^ Much of the information about the plutonium in the Fat Man bomb comes from reports of the criticality accidents of Harry
K. Daghlian, Jr. and Louis Slotin, both of whom died after conducting experiments
with plutonium bomb cores. See,i.e., http://members.tripod.com/~Arnold_Dion/Daghlian/accident.html.
- ^ As one article puts it, referring to information Seaborg gave in a talk:
"The obvious choice for the symbol would have been Pl, but facetiously, Seaborg suggested Pu, like the words a child would
exclaim, 'Pee-yoo!' when smelling something bad. Seaborg thought that he would receive a great deal of flak over that suggestion,
but the naming committee accepted the symbol without a word." David L. Clark and David E. Hobart
(2000). "Reflections on
the Legacy of a Legend: Glenn T. Seaborg, 1912–1999" (PDF). Los Alamos Science 26: 56–61, on
57.
- ^ Frontline
interview with Seaborg
- ^ Room 405,
George Herbert Jones Laboratory. National Park Service.
- ^ Plutonium: The first 50 years: United States plutonium production, acquisition, and utilization
from 1944 to 1994. U.S. Department of Energy (September 1994).
- ^ Thomas B. Cochran (Natural Resources Defense Council) (1997-06-12).
Safeguarding nuclear
weapons-usable materials in Russia. Proceedings of the international forum on illegal nuclear traffic. Retrieved on
2007-06-16.
- ^ William Moss and Roger Eckhardt (1995).
"The Human Plutonium
Injection Experiments" (PDF). Los Alamos Science 23: 177–233. Retrieved on 2006-06-06.
- ^ R.C. Longworth (1999). Injected! (Review of Eileen
Welsome's The Plutonium Files). Bulletin of the Atomic Scientists. Retrieved on 2006-06-06.
- ^ Michael S. Yesley (1995). "'Ethical Harm' and the
Plutonium Injection Experiments" (PDF). Los Alamos Science 23: 280–283, on 283.
- ^ ANL human health
fact sheet--plutonium. Argonne National Laboratory (October 2001). Retrieved on 2007-06-16.
- ^ Radiological control technical training DOE-HDBK-1122-99. U.S. Department of Energy.
- ^ Welsome, Eileen (2000).
The Plutonium Files: America's Secret Medical Experiments in the Cold War. New York: Random House, p17. ISBN
0-385-31954-1.
- ^ National Academy of Sciences, Committee on International Security and
Arms Control (1994). Management and Disposition of Excess Weapons Plutonium.
- ^ David Albright and Kevin O'Neill (1999). The Lessons of Nuclear
Secrecy at Rocky Flats. ISIS Issue Brief.
- ^ Primer on Spontaneous Heating and Pyrophoricity - Pyrophoric Metals - Plutonium, Department of Energy Handbook
DOE-HDBK-1081-94, December 1994. U.S. Department of Energy, Washington, D.C.
External links
Wikimedia Commons has media related to:
- "A Perspective on the Dangers
of Plutonium" by Lawrence Livermore National Laboratory
- Collection of articles on plutonium at
the Canadian Coalition for Nuclear Responsibility
- The Myth of Plutonium Toxicity
- Criticality
Accidents Report Issued
- Nuclear
Weapons: Disposal Options for Surplus Weapons-Usable Plutonium
- Unraveling the Phase Diagram
of Plutonium
- Physical, Nuclear, and Chemical,
Properties of Plutonium from IEER
- Los Alamos National Laboratory —
Plutonium
- It's Elemental —
Plutonium
- DOE
Plutonium fact sheet (PDF)
- End of the
Plutonium Age, D. Samuels, Discover Magazine, vol. 26, no. 11 (November, 2005).
- WebElements.com — Plutonium
- EnvironmentalChemistry.com — Plutonium (JavaScript required)
- Federation of American
Scientists — Plutonium production
- nuclearweaponarchive.org —
Plutonium Manufacture and Fabrication
- Ambient pressure phase diagram of plutonium — A unified theory for α-Pu and δ-Pu, P. Söderlind, Europhys. Lett.,
55 (4), p. 525 (2001).
- Nuclear Files.org Information regarding world plutonium inventories
- "Challenges in
Plutonium Science" — Special issue of Los Alamos Science from 2000 dedicated to scientific work on plutonium.
- NLM Hazardous Substances Databank – Plutonium, Radioactive
- Plutonium: A History of the World's Most Dangerous Element