slightly different (S&mid and Paterson, 1977) that there is an analogy ... Terent'eva (1958) in bauxite deposits from eastern Saian and south Ural (U.S.S.R.).
365 Elscvier
Scientific
Publishing
EXPERIMENTS REACTIONS GRINDING:
(Received
Company.
Amst~rdai~-Printed
in The Netherlands
ON PHASE TRANSFORMATIONS
OF MECHANICALLY PETROGENETIC
September
ACTIVATED
AND CHEMICAL MINERALS
BY
IMPLICATIONS
17, 1980; revised version
accepted
September
11, 19XI )
ABSTRACT
Dandurand,
J-L.. Gout.
reactions
R. and Schott,
of mechanically
activated
J., 1982. Experiments minerals
by grinding:
on phase
transformations
and chemical
petrogenetic
implications.
Tec~ronc$r~~~/c~.
x3: 365-386 Prolonged
grinding
mu* surfaces can
increases
and internal
result
in polymorphic
solid-state
transformation
transformation dehydration
the energy
defects.
Moreover,
transformations of metastable
of low-pressure
of solids by the production grinding and
mineral
temperatures
phases
of stored Here
(aragonite+
calcite.
(calcite -aragonite);
in the form of pressures
which
we demonstrate anatase-
and
(siderite -magnetite
of minerals
energy
quasi-hydrostatic
decomposition.
to stable polymorphs
to high-pressure
and decarbonation
also generates
the
rutile):
the lowering
or hematite,
the
of the
diaspore-
corundum). In the presence reaction
of a fluid phase. stored energy
rates and, more importantly,
transformations:
ground
calcite-aragonite
(at
dolomite-
aragonite
Assuming consequences
Mg2+
calcite
can be released,
resulting
In this paper we demonstrate
(at low MgZC concentration
concentration),
ground
magnesite-
in accelerated the following
in solution),
hydromagnesite,
and
ground ground
+ Mg*+
an analogy
between
on the release
transformations. aragnnite
calcite -magnesian high
from grinding
phase transformations.
laboratory
of hydrothermal
As examples
and d&spore-bauxites
the possible
and natural fluids, role
grinding,
tectonic
the solubilization
of deformation
on
activity
may have important
of minerals
and on solid-state
the formation
of metamorphic
is discussed.
INTRODUCTION
The experimental study of the mechanical activation of solids by intensive grinding is of great interest in geoscience because minerals are often subjected to naturally occurring mechanical strains. Therefore, knowledge of the effects of mechanical activation should permit a better underst~ding of certain mineral transformations which may occur together with tectonic events. 0040- 195 1/g2/OOOC-C@OO/%O2.75
kp 1982 Elsevier Scientific
publishing
Company
366
During
grinding,
energy
entering
stored.
Storage
boundaries) cracks,
During rapidly
non-hydrostatic
of energy
is linked
and accumulation
twinning
of minerals
essentially
the solid some is rapidly
strains
released
both
of internal
to formation strains
is the sum of these two different
reaches
grinding
a limit.
the increase
Indeed
the rate of agglomeration
of fine
and some is
particles
(grain
in the lattice (dislocations,
processes
increase
micro-
of free energy
of storage.
of free energy due to grain-size
after few hours
and surface
to solids. Of the
phenomena)
etc.. . ). As a result the measured
boundaries
prolonged
are applied
(elastic
the grain-size
area of the powder
reduction remains
reduction rate equals
constant.
Ag-
glomeration produced by cold welding (Bradshaw, 1951; Benjamin, 1976) contributes to the accumulation of defects at the boundaries of grains coalesced by this process. This increase of free energy due to surface energy can be calculated if the particle-size distribution and interfacial free energy of the mineral are known. The relative importance of the two forms of stored energy depends upon the mode of the mechanical actions, their duration and the nature of the material. Thus, it is known (Dandurand about
and Jauberthie,
by grinding
are more important
than with those of prevailing In addition
1976; Dandurand,
to stress
with minerals
ionic-type
effects,
1978) that structural
bonds
grinding
of covalent
to measure
the relative
bonds
can locally
generate
importance
almost
of particle
1957; Perami, 1971; Dandurand et al., 1972). However, as pointed (e.g., Gla’ngeaud, 1947; Termier and Termier, 1956) very little due to stored energy. This investigation
tal results of some types of mechanically which are compared
EXPERIMENTAL
Techniques
induced
physico-chemical
the more
size, stress,
and
from the analysis
Relations between mechanically induced micro-fissures in rocks, liquids, and mineral formation have been studied to a certain extent
transformations
hydrostatic
polymo~hs,
hydrostatic pressure effects which occur during grinding. However, of selected examples their relative consequences may be defined.
natural
(e.g., quartz)
(e.g., calcite).
pressures. This effect favors the formation of high-pressure easily as pressures are applied on strained minerals. It is difficult
changes brought
migration of (e.g., Lafitte,
out occasionally is known about
presents
experimen-
transformations,
to field observations.
TECHNIQUES
of grinding
Mechanical activation has been carried out with a Dangoumau-type percussion grinder (Fig. 1). The grinding vessel is a steel or plastic beaker, which contains a ball, 20 mm in diameter. The beaker is shaken vertically at 730 c/min. The grinding energy can be modified by using balls of different densities. energies, relative to a steel ball, produced by ~uminum and tungsten carbide
Kinetic ball are
367
0.4 and 2.2, respectively.
When it hits the material
ball is ES = 0.18 J. Assuming obviously
Fig.
that all energy is transferred
inaccurate-one
I. Dangoumau-type
powder-for
to be ground,
can estimate
percussion
that
the energy
the energy of a steel
to the powder-w.hich communicated
is
to 1 g of
grinder.
log of material
in the beaker-after
1 h of grinding
is of the order of
300 J (or 60 J/m2 of powder). These numbers must be considered as limiting values. If not otherwise specified, all data refer to grinding with a steel ball. Grinding at elevated temperatures was realized either by attaching a water jacket to the grinding vessel (T < SO’C) or by using a vertical electrical furnace (T > SO‘%). Ana&ical
techniques
The mechanically (Philips
activated
PW 1010, filtered
material
has been examined
Ka Cu-radiation
or C.G.R.
by X-ray diffractometry
sigma 2070 monochromatic
Kcu, Co-radiation), differential thermal analysis (heating velocity: 700”C/h), and by using a thermo-balance (SETARAM G.70, heating velocity: 500’C/h). The specific area of the grains were measured by B.E.T. analysis (N2 adsorption). tion were obtained by sedimentation (sedigraph 5000 D). RESULTS
AND
Sizes distribu-
DISCUSSION
Experimental results analyzed here deal with the behavior aqueous solutions and with transformations which occur poIymo~~c transformations and mineral decomposition.
of ground minerals in during dry grinding-
36X
Behavior
of ground materials
The behavior increase
in aqueous solution
of minerals
in water
may
be modified
of free energy which makes the material
This may result in an enhancement enrichment
of certain
With carbonates
dissolved
by grinding
due
to an
less stable and thus more reactive.
(either continual
on transitory)
of solubility
and
species.
taken as an example,
the purpose
of this study is to measure
relative importance of the two forms of stored energy of the ground materials in various aqueous solutions.
and to examine
Estimation of surface and strain energies due to grinding Calcite of 2-4 mm grain-size was carefully washed
the
the behavior
in deionized
water.
Its
in pure water was then compared with calcite ground for 24 hrs. The changes caused by grinding of calcite, are illustrated by the X-ray
behavior structural
diagrams of Fig. 2. Previous to dissolution runs, three methods grain size of ground particles: sedimentation,
were used in order to determinate specific surface area and X-ray
the line
broadening. Size distribution deduced from sedimentation of materials of less than 40 pm and of strongly ground materials after energetic disaggregation by soneration are reported ground
and at about Calcite
(calcite
ground
or modal
powdered
for 24 hrs presents
and a density
shape are assumed,
0.4 pm for this ground runs). This is similar
sizes are at about
for 24 hours and dolomite
15 ym for less energetically
ground
measurement) cubic
in Fig. 3. Maximum
materials
a specific
* materials surface
of 2.620. If homogeneous
one can calculate material
9pm
ground
for strongly for 100 hours)
(< 40 pm).
area of 5.6 m2/g grain-size
from surface
and
area a mean grain size of
(see Table I for other materials
to results from X-ray line broadening,
(B.E.T.
distribution
used in dissolution
where a mean dimension
of.0.2 pm for coherent diffraction domains has been calculated for calcite ground for 24 hrs using the method of Stokes and Wilson (1944). These lower values are probably
more reliable
than size distribution
deduced
from sedimentation
because of
agglomeration of grains during grinding. Dissolution experiments on calcite were made at 25°C and a total pressure of I atm in a constant temperature bath as described by Menschel and Usdowski (1975). CO, -gas saturated with water vapor was continuously bubbled through the liquid phase ( Pco, = 0.97 atm.). Figure 4 shows the changes two different
calcite
varieties.
In both
cases pH
tends
of pH obtained towards
a value
with the of 6.03.
However, with ground calcite a maximum at pH = 6.17 is observed at the beginning of dissolution **, and after a period of 6 months this calcite recrystalhzes (Fig. 2).
* In the following
this material
** Note that the attainment placed
in solution
will be referred
of the maximum
be dissolved.
to as gently ground. pH value requires
that at least 25% of the powder
initially
369
1
i-‘
,
I
I
I~.
Fig. 2. X-ray diffraction ground
~
Wrticles
diagrams
for 24 hrs, 3=calcite
Fig. 3. Size distribution Curve
I
15
20
e"25
f =materials
3=dolomite
ground
The degree
of calcite (Co, Ka, ). I =normal
being in water
deduced gently
for 6 months
from sedimentation
reduced
to powder
calcite, 6-10 pm grain size. .?=calcite
after grinding
of some materials of less than
size (micrometers)
for 24 hrs. used in the solubility
40 pm;
I=calcite
ground
experiments. for 24 hrs,
for 100 hrs.
of supersaturation
of the solution
with respect
to normal
calcite
is
given by the maximum pH value. It can be used to calculate the total increase of the free energy of the ground calcite. The calculation yields an order of magnitude of 29X.15 ) =
‘cAG;
TABLE
I
Results
of specific
dissolution
2380 J/mole.
surface
area,
On
the other
density
and
hand,
calculation
it is possible
of mean
grain-size
Surface area