JOTJRNAL
OF KilTCLEAR
5, No. 2 (1962) 262- 263, KORTH-HOLLAND
MATERIALS
PUBLISHING
CO..
AMSTERDAM
THE CRYSTAL HABIT OF URANIUM DIOXIDE R. UKAEA
G. ROBINS
t, R.
S. WILKS
Research Croup, Metallurgy Division, Atomic Energy Research Establishment, Harwell, Didcot, Berka, UK
Received
1.
28 Sept.
Introduction
The close relationship between morphology and the detailed symmetry of atomic arrangement has been demonstrated by observations of the crystal habit of uranium dioxide. Single crystals of the oxide, prepared by several available production routes, were used for these investigations. 2.
and B. T. BRADBURY
1961
(111) (100) (3311, and (111) (100) (113) (See figs. 2 and 3). Electron microscopy of fractured surfaces of polycrystalline uranium oxide, sintered to den-
Experimental Observations
The crystal habit of uranium dioxide single crystals was found to differ slightly, depending upon the method of preparation. Vapour deposited crystals had a (Ill} (100) habit 1) (fig. 1). Electrolytically deposited crystals had a habit which was dependent on the concentration and composition of the electrolyte 23s). The three observed habits were {Ill) {loo},
Fig.
1.
V&pour deposited
the predominant t
{ill}
Present address:
crystals
habit.
of UOa showing
2. (111)
Fig. 3. {ill)
(Crystal size 0.1 mm).
University
Fig.
College, Wollongong, 262
N.S.W.,
Electrodeposited (100)
(331)
habit.
Electrodeposited {IOO) (113) Australia.
habit.
crystal
of
UOa
showing
(Crystal size 3 mm).
crystal
of
UOz
showing
(Crystal size 1 mm).
THE
sities of
94 O/Otheoretical,
CRYSTAL
HABIT
revealed
spherical
pores in grain interiors, some of which exhibited well developed planes on their surface 4+ Some of these grain interior pores or “negative often exhibited very pronounced crystals” growth markings, which were indexed as (111) {loo}
(110)
Fig. 4.
837) (see
“Negative
fig.
crystal”
4).
in sintered UO2 showing
{ 11 l} { 100) { 1 IO} habit of growth markings. Electron micrograph.
OF
of
URANIUM
smallest
3.
Remarks
The Donnay-Harker Principle 9) which is a modification of the Bravais Law, states that the crystal-forms which tend to form most frequently are those with faces parallel to planes
area,
taking
into
con-
planes in the various space groups. Consideration of these two principles results in the same deduction, when those space groups containing no screw axes or glide planes are present, as is the case with uranium dioxide, (space group Fm3m). The forms in order of decreasing importance for space group Fm3m are: (1 ll} (100) (110) (311) (331). Various combinations of all these forms have been observed in uranium oxide (section 2). Thus, the observations reported here for uranium dioxide, provide evidence that the habit of a crystal species is determined by both the particular space group pattern on which the structure is built, and the external environment during crystalhsation.
References 1)
x 30 000.
uranite crystals are or (100) (110) orien-
reticular
sideration the presence of screw axes and glide
J. T. Waber,
J. A.
J. Electrochem. 2) R.
Naturally occurring usually of (110) (111) tation 8).
263
DIOXIDE
a) 4)
G. Robins,
R. 8. Wilks,
UKAEA
(1961)
T.
Padden,
R.
96
3 (1961)
(Harwell)
294
Report,
Westinghouse
A. Portnoff-Porneuf,
6)
B. T. Bradbury,
7)
S. Takahashi,
(USA)
AEREReport,
J. Nut.
Mat.
2 (1960)
181
to be published
et al., J. Atomic.
Energy Sot. Japan
73
*)
C. Frondel,
9)
J. D. H. Donnay 22 (1937)
Mat.
586 (1959)
5)
2 (1960)
and R. Kleinberg,
106 (1959)
J. Nut.
R 3833 WAPD-T
O’Rouke
Sot.
Geological 73
Survey
Bull.
and D. Harker,
1064 (1958)
Amer. Mineral.