allotropes of plutonium
{{Short description|Six or seven different forms that pure plutonium metal can take}}
{{Use dmy dates|date=April 2022}}
File:Pu-phases.png of plutonium at ambient pressure. Atomic volumes in cubic angstroms.
class="wikitable" | ||
Phase | Crystal structure | Density (g/cm3) |
---|---|---|
alpha (α)
| simple monoclinic || 19.86 | ||
beta (β)
| body-centered monoclinic | 17.70 | ||
gamma (γ)
| face-centered orthorhombic | 17.14 | ||
delta (δ)
| face-centered cubic | 15.92 | ||
delta prime ({{prime|δ}}) | body-centered tetragonal | 16.00 | ||
epsilon (ε)
| body-centered cubic | 16.51 |
|editor-last=Wick
|editor-first=O.J.
|date=1967
|title=Plutonium handbook
|volume=I
|url=https://archive.org/details/plutoniumhandboo0001unse
|location=New York
|publisher=Gordon and Breach
|page=34
|access-date=2025-01-24
}}
]]Plutonium occurs in a variety of allotropes, even at ambient pressure. These allotropes differ widely in crystal structure and density; the α and δ allotropes differ in density by more than 25% at constant pressure.
Overview
Plutonium normally has six allotropes and forms a seventh (zeta, ζ) under high temperature and a limited pressure range.
{{cite journal
|url=https://permalink.lanl.gov/object/tr?what=info:lanl-repo/lareport/LA-UR-83-5074
|title=Plutonium: A Wartime Nightmare but a Metallurgist's Dream
|last1=Baker
|first1=Richard D.
|last2=Hecker
|first2=Siegfried S.
|last3=Harbur
|first3=Delbert R.
|journal=Los Alamos Science
|date=Winter–Spring 1983
|publisher=Los Alamos National Laboratory
|pages=142–151
|access-date=2025-01-23
}}S. Dabos-Seignon, J. P. Dancausse, R. Gering, S. Heathman, U. Benedict: Pressure induced phase transition in α-Pu. In: Journal of Alloys and Compounds. 190, 1993, S. 237–242 (doi:10.1016/0925-8388(93)90404-B).visualisation of the crystal structure at [https://log-web.de/chemie/Start.htm?name=Pu_HP&lang=en log-web.de]. These allotropes have very similar energy levels but significantly varying densities and crystal structures. This makes plutonium very sensitive to changes in temperature, pressure, or chemistry, and allows for dramatic volume changes following phase transitions.
{{cite journal
| first = Siegfried S.
| last = Hecker
| title = Plutonium and its alloys: from atoms to microstructure
| journal = Los Alamos Science
| volume = 26
| year = 2000
| pages = 290–335
| url = https://fas.org/sgp/othergov/doe/lanl/pubs/00818035.pdf
}} Unlike most materials, plutonium increases in density when it melts, by 2.5%, but the liquid metal exhibits a linear decrease in density with temperature.{{cite book
|title = The Encyclopedia of the Chemical Elements
|url = https://archive.org/details/encyclopediaofch00hamp
|url-access = registration
|publisher = Reinhold Book Corporation
|location = New York
|year = 1968
|editor = Clifford A. Hampel
|last = Miner
|first = William N.
|author2=Schonfeld, Fred W.
|chapter = Plutonium
|page = [https://archive.org/details/encyclopediaofch00hamp/page/544 544]
}} Densities of the different allotropes vary from 16.00 g/cm3 to 19.86 g/cm3.
Machining plutonium
The presence of these many allotropes makes machining plutonium very difficult, as it changes state very readily. For example, the alpha (α) phase exists at room temperature in unalloyed plutonium. It has machining characteristics similar to cast iron but changes to the beta (β) phase at slightly higher temperatures.
The reasons for the complicated phase diagram are not entirely understood; recent research has focused on constructing accurate computer models of the phase transitions. The α phase has a low-symmetry monoclinic structure,{{cite web| url = https://log-web.de/chemie/Start.htm?name=Pu_alpha&lang=en| title = geometry of crystalline alpha plutonium}} hence its poor conductivity, brittleness, strength and compressibility.
Stabilization
Plutonium in the delta (δ) phase{{cite web| url = https://log-web.de/chemie/Start.htm?name=Pu_delta&lang=en| title = geometry of crystalline delta plutonium}} normally exists in the 310 °C to 452 °C range but is stable at room temperature when alloyed with a small percentage of gallium, aluminium, or cerium, enhancing workability and allowing it to be welded in weapons applications. The δ phase has more typical metallic character and is roughly as strong and malleable as aluminium. In fission weapons, the explosive shock waves used to compress a plutonium core will also cause a transition from the usual δ phase plutonium to the denser α phase, significantly helping to achieve supercriticality.[http://www.globalsecurity.org/wmd/intro/pu-phase.htm Plutonium Crystal Phase Transitions]. Globalsecurity.org (27 April 2005). Retrieved 2010-02-08. The plutonium–gallium alloy is the most common δ-stabilized alloy.
Gallium, aluminium, americium, scandium and cerium can stabilize the δ phase of plutonium for room temperature. Silicon, indium, zinc and zirconium allow formation of a metastable δ state when rapidly cooled. High amounts of hafnium, holmium and thallium also allows retaining some of the δ phase at room temperature. Neptunium is the only element that can stabilize the α phase at higher temperatures. Titanium, hafnium and zirconium stabilize the β phase at room temperature when rapidly cooled.
File:Phase diagram of plutonium (1975) 150 kbar region.png File:Phase diagram of plutonium (1975).png