Solid State Ionics 16 (1985) 185-194 North-Holland Publishing Company
FORMATION
OF
C.M.P.M. Eindhoven
SODIUM
185
ALUMINATES
SARIS+ University
HIGH
Technology,
of
H. VERWEIJ Philips Research
AT
P.O.
Labs.,
Box
TEMPERATURES
P.O.
Box 513,
80.000,
UNDER
THE
5600 MB Eindhoven,
JA Eindhoven,
5600
INFLUENCE
OF
The
Mg AND
Ca
Netherlands
The Netherlands
The formation of sodium aluminates at high temperatures under the influence of Mg and Ca was studied to obtain insight into lifetime processes that occur in high pressure sodium (HPS) discharge lamps with translucent alumina envelopes. Powders with molar composition Na2C03-5A1203, mixed and fired at Na2CD3-MgO-5A1203 and 2Na2CO3-CaCO3-5A1203 were thoroughly Na2CO3-9A1203, temperatures up to 16OO’C for top-level times up to 100 hrs. Quantitative X-ray diffraction was used to study the composition of the quenched mixtures. In the systems Na2CO3-5A1203 and Na2CO3-9A1203 the compound Na20.Al203 is formed first at low coincident with the decomposition of carbonate. This compound subsequently reacts temperatures, with Al203 to form a mixture of E- and El”- Al203 in a weight ratio of 1:6. At temperatures above 14OO’C 6”-Al203 transforms to El-Al2O3. Remarkably this transformation is most complete in the Na2CO3-5A1203 mixture. In the Na2CO3-MgO-5A1203 mixture the compound Na20.Al203 is also formed ET- and 6”-Al203 are formed subsequently in a weight ratio first, directly followed by MgO.Al203. of about 1:1.6. At temperatures above 14OO’C stabilized 6”-Al203 is then formed almost completely. The reactions in the system 2Na2CO3-CaCO3-5A1203 are vary complex. The compound Na20.Al203 is formed first, directly followed by the ternary compound Na20.CaO.2A1203 which forms solid At about 1OOO’C the compound Na20.3Ca0.8A1203 solutions with Na20.Al203, starting at 115O’C. starts to form with a maximum around 12OO’C. At higher temperatures it is consumed again, resulting in a complete disappearance at 16OO’C. 6/e”-Al203 also starts to form at IOOO’C and is still present at 16OO’C, together with a solid solution of Na20.Ca0.2A1203 and Na20-A1203. Conclusions can be drawn from the present results that are relevant for an understanding of lifetime processes in HP5 lamps.
1.
In recent in
high
with
years
and
5000
inside
the
0.7-l
lamps
discharge
with
envelopes
the
In
wall
at the the
ratures
a very with
must
be
that
ends
but
steady
discharge
: Philips
decreases
degradation
sometimes
HPS
reaction
plasma
Glass
takes
Dev.,
TGA, has
(TGA)
HPS
range
material
in the
highest
There
range
alumina
of
tion
TGA
in
P.O.
BOX 218,
0 167-2738/85/$ 03.30 0 Elsevier Science Publishers B.V. (North-Holland Physics Publishing Division)
are
of
to that
obtain
was
lamp and
translucent
the
that
A1203
almost
The Netherlands
in in
process
to
shown2s3
wall
present
sintering
with
tube
causes
processes a
added
w % MgO to
product
the
leakage.
Mg2+,
to
order
zone
Tube
In
5600 MO Eindhoven,
the
tube
lifetime
0.25
of
efficiency. leads
sodium,
“cold”
sodium
properties
a pressureless
about
sintered
of
on
It
of
the
influence
powder.
of a
colour
indications
an
in
in
and degradation
1BOO’C in H2, MgO is
tempe-
place.
of
lamps.
about
mid
walls
Disappearance
blackening
alumina
the
products
itself.
1.
To
a disappearance
tube
degradation
the
in the
the
excess
white
to 125O’C
with
wall
pressure
in for
are
temperatures
address
ref. sodium
gastight
tube
slow the
the
means
lamp zones
material
* Present
instance
tube
This
translucent
from 85O’C zone.
for
in
causes of
by reaction
lamps
reasonable
preferably
and efficiency
atm.
discharge
reaction
blackening
much interest
performance,
a lifetime see
been
(HPS)
colour
hours;
colour
has
sodium
white
obtain
of
there
pressure
a good
efficiency of
This
INTRODUCTION
at
starting an
addi-
may result theoretical
186
C.M.P.M. Saris, H. Vcrweij / Formation
density
and
ture.
This
subject
a
of
years;
relatively
beneficial many
a review
ring
effect
tions
the
defect
chemistry
grain
boundaries.
1.1.
solubility
1530, 90,
240,
of
solubility
of
MgO at
the
wet
of
refs
5-7
single-crystal
1.2.
pies
of
is
both
ration The also
although
are of
ref.
at
alu-
reported
to of
was reported.
dope
an
that
MgO.Al203
1.3.
Mg in Al203 7 was to
preci-
concluded lattice;
Mg’Al
by
on the It of
. It
formed
suggestion frequently
encountered
no direct
proof in
forma-
by
plausible
brotin
has
bivalent
in yet
the
H+
literature
been
transition
presence
of
and
similar
to
12.
A rough
Al2O3.
For
1 to
1
to
about
5
of
the
order
of
mag-
MgO solubility
segregation
below
of
Mg
in
of
Mg
the
boundary
reported. metal
the
more
is
was
surfaces.
sensitive
with
depth
of
a
that
these
rent
from
are
rapid
from sec-
normal
after of
Auger refs of
19
XPS in fracture
segregation
factor
Refs
that
18,
show
20-22
that
It
which
on grain is
are
argued diffe-
precipitates,
sintering
no
micropreci-
MgO.Al203 instead.
the
mea-
17,
of
but
MgD.Al203
decrease
in
to
microprecipitates,
upon cooling
on grain
polished
In
at.
occurs
formed
gene-
concluded
used
non-stoichiometric
phases
is
technique
2 and 4 was arrived
pitates
MgO-
as a non-
profiling
and
used
the
it
16 no Mg was found fracture
of the
solubility
phase
on
measurements
on
lot
14 and 15 Mg segrega-
boundaries
Mg segregation
the
second
In refs.
If
the
temperature
on SAM measurements
formed
Al2O3.
exceeds
the
a
regarding
microstructure
grain
combination
of
in
is
in
In ref.
between
literature
lines6.
surfaces
There
sintering
microhardness
and 24
the
MgO.Al203
the
segregation
14-24.
largely
at
at
boundary
Mg segregation
reflected
real
colou-
by
be
H2-sintered
bands
refs
in
limit
boundary
compensation
an MgO also
corresponds
real
grain in
rally
report
crystals.
defect
on
of
surements
(t’lgAl,h’)X
the
of the
10
is
boundary
controversy
suggests
possible very
This
observed
reported
tions.
that
conditions
sapphire
8
concluded7.9 is
are
tion
under
made
cause
the
vacancies
Mg’Al
refs
a
can be expec-
will
studies revealeo
in
of
TGA with
complex
this
Al2O3.
the
Studies
Mg occu-
the
IR
It
2 wppm O-H in
Grain
nature
refs
8
VO and
is
which
of
in
ref.
is
gave
-concentration
Defect
that
oxygen
oxidizing
Mg-doped
reported
0)x
found
-stoichiometric
sapphire.
formation
an O-H . . 0 com-
Al2O3
the
study
that
was argued
..O absorption i3-n'
of
wppm MgO in
Mg-
by a nucleation
of
surrounding. in Hp-sintered
laboratories
of
from
It the
least
compensation
14oo.c.7
was concluded
with
direct
triplets
nitude
particles
ref.
caused
Preliminary
estimate
The
In
H2 gas
(Mg’Al,O-H....
a triplet
be
and can
plot.
sapphire
on an Al site
at
A solubi-
was found’
the
Al;’
compensation
that
defect
6 the
agreement
also
conditions.
under
defects
ti+
are
in of
and
by ion
in the
ted
the
respectively
chemistry
MgO-doped
compensation
that
is
of
of
F-centres
Vi
in
powders found
In
lines
generally
sites
oxidizing defect
Al203
Arrhenius
chemistry
studies It
reduction
TGA at our
translucent
close
it
purpose
compensation tion
in
dislocation
chemistry
Al
Mg at
was studied
was
small
very
Defect
9.
Verneuil-grown
plex
the
at hig/~ tcmpevatures
ERR and IR measurementslo-13.
bivalent
mechanism.
chemistry and
are
in
136O’C
studies
The main defect
of
was studied.
by a single
and growth
Al203,
defect
sapphire
data
along
MgO in
were
H2,
7 the
13 wppm MgO at
occurred
assump-
wppm MgO.
of
of
on
solubilities
183O’C
lity
pitation
depend
segregation
1630-C
in
Verneuil
be described
25
sinte-
MqO-doped
and
250 wppm. In ref. -doped
5
and 1100
sintered
minas,
past
The
MgO in Al203
vacuum;
1730
540
doped
the
MgO in Al203
ref.
in
1630,
4.
aluminates
present.
In
were heated
the
ref.
of
the
of
The solubility 5-7.
in
discussed
and
microstruc-
MgO has been
during
given
Solubility
refs.
of
studies
is
models
about
regular
effect
ofsodium
as
solubility
are a result of
MgO
C.M.P.M. Saris, H.’ Verweij /Formation
with
decreasing
dance
with
the
of
real
absence ded In
in
solubility
clude
with in
that,
large of
boundary
refs
sence
in
are
of
in
the
con-
than
amount
Na
sence between
Cs
is
of
TGA
1.5.
on
The percentage
of
with
the
high
make
it
plausible
offers
-phase
Ns
in
to
with
is
at
pre-
a
boun-
evidence film
for in
grain TGA
such
is
some speculations
enhanced
ionic
diffusion
or
in
a
TGA. attsck
about with
explained
in
stabilizes
thermodynamic
some
terms
in which
phase
which
grain
boundary
tions
in
Na-Cs Ca
causes
terms
aluminate,
forms
a
mechanical
coherence.
TGA envelopes
in or
precursor
which in
systems
mentioned
transformation
sbout
stabilities
E-Al203
less
reac-
are
studies
ref.
31,
three
high at
cited
in
Na20.5$Mg0.14&
of
stabilized composition
tal
studies
part
It
exist
of
in
refs
Ca
are
was
with
composition with
the and
Single-crystal
coma
new
studies
in the
resulted
system 35 in
complementary;
known
theoreti-
single
crys-
in
theo-
the
Ns20-CaO-A1203 and
ref.
which at
high
36. 36
at
Both the
12OO’C
ternary
was
2Na20.3Ca0.5A1203
Na20.Al203
concluded
:A stsbilized
composition
Na20.A1203-Cs0.A1203-A1203
Na20.Cs0.2A1203,
sys-
reported
Na20.4Mg0.15A120334.
reported
The
the
been
Ns20.MgO.5A1203;
composition
6”-Al203
928 ) ,
have
32.
B “‘-Al203
been
with
compounds
binsry
resulted
be
than
by
uncertainties
Al203
Al2O3.
the
the
hampered
and
6”‘-Al203
with
of
of
are
generally
ref.
6”-Al203
cal
where
in
6”-Al2O3,
6 ““-Al203
l$
died.
Phsse
0.68Ns20.1.88Mg0.7.48A1203,
compound
the
temperatu-
temperatures
17OO’C
1~Ns20.1$MgO.1O&A1203;
retical
in
studies
compounds
of
by
relations
and Ca0.6A120330.
the
ternary
TGA attsck
lOOO-13OO’C
Na20. llA120327
in
the
especially
the
Na20.5$A120329)
into
relevant
of
of
I theor.
(theor.
of phase
kinetics
in
Ca concentra-
generally
kine-
the
insight
higher
studies
aluminate of
TGA in
systems
HP5 lamps.
Phase
kinetic
breakdown
Overall are
could
rates
reaction
the
position
Na+ 25726. of
the
of
range
in
slow
modification
TGA,
exchange
explain
paths
occurs;
applied
of
unclear,
have been
Enhancement
yet
in
litera-
still
there
in
The most
the
attsck
not
that
a second-
although
ionic
in
together
boundary
in
much higher
means that
Na20-MgO/CaO-A1203,
tem Na20-MgO-A1203
and
purity
to
corwppm,
by Ca.
needed
Phase
the
high
sodium
is
by segre-
present
slthough
tubes 1000
be
fundamental
regions.
are
res
surfaces16-19*23.
Ca
will This
diffusion
Auger
temperatures
Ca-containing
systems
A1203-rich
caused
Ca found,
enhanced
the
lamp
reaction
grain
be enhanced
that
of
the
attack
reletions
and
less
TGA,
the
the
about
Na concentration
of
a more
knowledge
and
that
of
observed
segregated
boundary
The mechanism
hours
This
fracture
no real
300
of
must be used
Phase
Na,
immersed
especially
structure,
grain
of
were
rste
sintering
Ca0.6A1203-like
samples Ca,
attack.
is
pre-
on
Na in
Ns20-MgO/CsO-A1203
demonstrsted
was found
and
thought
XPS measurements
for
the
Ca which
also
of
It
boundary
sttack
effect
where
9OO’C
the
concentrations
Cs is
levels
at
and
grain
gation
of
increased
Ns
severe
in
that
the
enhancement
To gain
a detrimental
100 hours.
of
rate
dissolved
grains.
TGA even
that
stages
arguments
tion
on grain
amount of
the Cs concentration.
tic
micropreci-
the
concentrations
means final
187
at high temperatures
to
resctions
various
liquid
responds which
present
MgO.Al203
a minor
experiments26
with
1OOO’C for
by
to
msinly
aluminates
50 wppm while
The
conclu-
we tend
indications
An effect
model
doped
ture
20-23
the
strong
Ca in
lifetime25.
dary
5-7.
TGA samples23.
TGA, Mg is
in
20 wppm, has
in
refs
actor-
was also
non-stoichiometric snd
in
Ca in TGA
There
in
of
precipitates;
and non-segregated
than
18,
normal
planes
1.4.
data
is
on thin-foil
MgO.Al203
pitetes
This
Mg segregation
a STEM study
agreement
in
temperature.
of sodium
have
studies
subsystem
was
stu-
compound as
reformulated forms
solid
temperatures.
solutions In
the
C.M.P.M. Saris, H. Verweij i Formation
188
high-alumina Na20.3Ca0.8A1203 results
a
area
of
was
ref.
36
new
found;
are
compound
the
phase
represented
in
of‘sodium
alumirmtes
2.
EXPERIMENTAL
study
fig.
The
1.
starting
Na2CO3 blic
ques
des
ture
content u,
Ca0.6A1203.
by
ture
range
loss
is
phase
information
quaternary
compounds
-Al203
known
are
1.6. To
Present see
tion
at
a very of
can
in
compounds and
and
ternary
matic
range the
of
is
by
literature.
-filled
followed Two
of
study
of
as
of
compositions were
tl-
chosen
and
B”-Al2O3;
another
Ca-content
studies
on
(1000-13OO’C)
was
stabilized
2Na2C03-Ca0-5A1203 in
the
systems
of
in
TGA.
No syste-
formation
of
the
temperature
are
known
com-
from
6
by
MPa
tempeeaweight
in
in
with
a
measured
lid
of
mocouples
the
The
to
The
level, top
of
levels
and
con-
(Degussa, A123)
Temperatures
and
the
was
200’C/hr
were
furna-
were
S-type
temperature
by
found
temperature
Germany,
material.
sample
followed
was
samples
the
of
heating
configuration.
stabilized
rate
MPa.
chamber
two
sample
heating
top
same
by
100
crucibles
Republic
using
close
the
a
580-925-C.
PID
cascade
alumina
Federal
of
inside
pre-
using
at
on
adaptive
in
half-
followed
bag
range
fired
hours
were
analysis
the
pre-
jars
PMMA die,
treatment
dense
were
a
in
5
Pellets
rubber
standard
heat
Frankfurt,
elements.
a
digital
a
for
carbonates
were
in the
a
in
were
pressing
thermogravimetric
direct
tained
level.
were CaCO3
the
mixing
balls.
of
pellets
During
below
powders
powders
uniaxial
completely
with
the
mixture
polyamide
pressing
The
of
two-sided
occur
with
the
theoretical
polyamide
decomposition
ces
m2/g.
w X in
the
the
using
control in
Na2CO3-MgO-5A1203 range
to
size
analysis.
44.3
mixtures
of
checked
Na2C03,
a function
binary
binary
uses
formation
of
mois-
particle
15.6
CO2 content
vibrating
by
The
area
of
A152,
average
640-81O’C;
with
pared
combina-
the
mixtures
low
interest
which
Na2C03-5A1203
and
related
TGA-Na
present
in
composition
the
in
Na20-CaO-MgO-
moisture
Syntheti-
France),
w X,
loss
g stock
pressure
a
the
time.
B”-Al203
pounds
in
composition
direct
or
literature.
happen
range
the
reflecting
system
powder
and
ternary in
temperatures
130,
Rubis
thermogravimetric
of
London,
44.0%.
isostatic
A1203
composition
chosen
the
approach
Na2CO3-9A1203
one
the
temperatures
temperature
the
from
pragmatic
MgO,CaCO3
in
high
study
whet
high
at
Les
surface
and
Ltd.,
JMC
Jarrie,
specific
isopropanol No
w X.
detectable
wX.
1.12
a weight
pared
0.14
no
Chem.
Kuhlmann,
Alpes,
moisture
75
content
specpure 2.7
(Ugine
checked
and
Matthey
Kingdom),
a-Al203
nas
&
CO2 content
showed
Repu-
content.
United
0.1
Federal
moisture
(Johnson
and
were:
Darmstadt,
suprapure>99.9%,
(idem),
MgO
used
AG,
Germany),
CaC03
FIGURE 1 1200’C in the system relations at Phase Na20.A1203-Ca0.A1203-A1203. The shaded area can be constructed in many ways, depending on the assumption of the relative stability of B-alumi-
Merck
analyse799.5%,
moisture
The
materials
(E.
of
zur
LO
at high temperutures
lOO’C/hr 900,
up
therfurnace
programmed to up
1000,
200-C to
top
1100,
C.M.P.M. Saris, H. Verweij /Formation
1200,
1300,
1400,
times
of
3,
1,
10,
set-point
rStUre
conformity O.l’C
conformity
an
using
(Nederlandse
a type
and CuKa
radiation.
tic
in
peaks
converted
the
into
responding
with
Ca-containing
of
to
-.
cor-
factors,
In the results the
were
the
calibration
owing
powder
spectra
mixtures. the
3 ;
Eindhoven)
quantities
mixture
::
characteris-
diffraction
using
be made quantitative the
of
standard
40
diffractometer
Intensities X-ray
the
samples
X-ray
b.v.,
components
obtained
The
by
PW 1050
2 -ii
was about
0.25%.
Eedrijven
relative
2’C;
case
of
could
not
complexity
of
Mixture
heat
of
the
It
and
of
with
that
its
to
The weight
mixtures
was estimated
results
are
at
top
level
From this has
of time
figure
completely and that
l4OO’C
the
At
centration the which
is
results the
is
also
can be seen
a weight
temperatures of
expense
B”-A1203 of
the are
literature.
the
given
accordance In ref.
-
x-x
I
\-
and
Na20.Al203 firing
between mixtures of
above
phase
at
the
decreases
is
l59O.C.
found
of con-
These
that
1~00
1500
1600
T(“Cl
FIGURE 2 Calculated compositon of Na2COj-9A120) mixtures after heat treatment with 10 hours top level time as a function of top level temperature.
at
B-Al2039
observations
with
1300
1200
and
ShOSt
B”/B-A1203
of
IWO 1lW
at
1200 is
l4OO’C
gradually
10 hrs
2.
that
ratio
37 it
Al,Oa
-*-8
reacted
for
after
the
B-
1
I
I
-x- +” A1203
patterns;
in fig.
concentration
dominant in
X-ray
at temperatures
with
6.
of the
fired
it
of
rather
Y/
of (NA
I.
mixture,
composition
constant,
the
the
X (WT%I
relatively
of
disappeared
1200’C
about
from
60
the
of
I
-+-=Na20.Al&13
70
at
is
is
a mixture
in Table
the
studied
reacts
80
below
Ne20.Al203
composition
given
The composition
only
formation
form
90
time
decomposition
subsequently
Al203
mixtures
top-level
was
that
after
B”-A1203.
the
of
I
I
ct- .AI,O,
dependence
temperatures
time
first
Na20.Al203
slowly
a strong
at
was found
formed
carbonate fast.
only
effect
llOO-l4OO’C. compound
Na2CO3-9A1203
showed
The influence
remarkable
l2OO’C;
the
treatment
on temperature. was
lOO(
Na2CO3-9A1203
The composition after
h
Table I. X-ray peak heights and calculated composition Na2COy9Al203 mixtures after heat treatment = Na20.Al203).
spectra. 2.1.
189
-
level
The tempe-
level
inspected
Philips
top
hours.
top
of
and
with
was within et
accuracy
air-quenched
diffraction
the
30 and 100
and stability
with
were
and 159O’C
1550
of sodium aluminates at high temperatures
transformation 14OO’C
is
in
not
stable
the
res
that
rate
of
infinitely with are
than
B”-Al203
and
slow
respect
higher
64
to at
that
E-Al203 the
below
B”-Al203 at
is
temperatu-
most 14OO’C.
The
190
C.M.P.M. Saris. H. Verweij / Formation
instability above
of
1550-C
also
found
in
The slight at
binary
in
the the
of
of
is
not
refs
was
38-41.
concentration
14OO’C can
which
at high temperatures
be ascribed
critical
to
for
the
study.
2.2.
Mixture
The
heat
for
the
position
for
the
treatment
are
Na20-VA1203
of
the
from
the
given
in Table
60
Na2C03-5A1203
results
after as
studies
aluminates
temperatures
Na20-A1203
the o-Al203
above
Na20 evaporation present
at
system
phase
increase
temperatures
6”-A1203
binary
of sodium
mixture.
reacted
X-ray
Na2CO3-5A1203 qualitatively
was
and
the
50
same
The weight
mixtures
patterns
mixture the
X[WT%)
com-
estimated
results
are
II. I
lo-
-.
-.
110O 1200
1300
1 hl h:
0
d
900 1000
/ 1500 16CKl
1.400
T(T) FIGURE 3 Calculated composition of Na2CO3-5A1203 mixtures after heat treatment with 10 hours top level time as a function of top level temperature.
O-Al203
at
159O’C
sodium-rich
ascribed of (NA
The
composition
of
the
top-level
time
is
The
composition
constant
in
of the
with
a 8”/8-Al203
sion
to E-Al203 The
below
it
is
atomic and
ratio is
is
overall
scale
is
of
about
6.
complete
that
the
independent
to
2.3.
the
reaction
The observation
The conver-
the
larger
by
ratio
temperature
suggests the
mechanism
between that
that on
Na20.Al203
conversion
to
in
overall
the
most
surprising
used
are
Na2CO3-MgO-5A1203
heat
time
below
but
mobility
if
can
be
in
the
and
tes
and
mation hr
first
at
sent.
the
that
its
not
the
where
were
unreacted
of
at
is
top-level
is
was
at
also
the
compound
the
carbona-
of
fast.
complete
MgO was still
after
top
time
It
rather
yet
of
temperatures
studied.
quantities obtained
mixtures
dependence
influence
only
Na20.Al203
formation
theoretical
and MgO.Al203
a strong
decomposition
MgOaA1203 was not
900’C The
influence was
after
that of
and
remarkable
159O’C again
formed
mixture
Na2CO3-MgO-5A1203 showed
again
was
12OO’C;
1550
of
treatment
temperature
level
observed
at 159O’C.
of
after on
: again
B”/8-Al203
both
10
3.
remarkably
1200-14OO’C
determined
of
with
in fig.
Na20 concentration
completely
a-A1203.
fired
given
mixtures of
almost
observation 14OO’C
and of
the
range
mixtures also
somewhat
mixture.
The composition
hours
more complete is
arguments
stoichiometry Table I X-ray peak heights and calculated composition Na2CO3-5A1203 mixtures after heat treatment = Na20.Al203).
is
mixture
of
For-
after
1
pra-
Na20.A1203
firing
for
10
C.M.P.M. Saris, H. Verweij /Formation
hours
at
react
compounds B/Ef11-A1203 the
At
1OOO’C.
mixtures.
incorporation
not
be
to
drawn
from
in
the
X-ray
position
of
the
reacted
diffractograma,
of
the
IY-Al203
to
due MgO is form
a
6”-Al203
phase.
No
aluminates
could
be
The weight
com-
estimated
from
mixtures,
are
could
diffractograma
diagrams.
given
in
at high temperatures
about
compounds
Moat
sodium
detected
the
X-ray
ternary
Mg-containing
form
to
conclusions
into
stabilized
both
Al203
these
limitations.
incorporated
partially other
Mg in
the
temperatures
with
Direct
of
resolution
probably
higher
further
of sodium aluminates
Table
III.
n
Kl
FIGURE 4 Calculated composition of Na20-MgO-5A1203 mixtures after heat treatment with 10 hours. top level times as a function of top level temperature.
found
in
the
binary
difference
Table III X-ray peak heights and calculated compositions of Na2CO3-MgO-5A1203 mixtures after heat treatment (NA = Na20.Al203 and MA = MgO.Al203).
strong at
with
increase
can be seen
appeared is
after
the
the
system
binary
is
Na20.Al203
at
a
The
after
present
10 hours
at
top
and
part
of
of
present,
of
level
top
quantity
the
time
is
temperature
position
of
stant
but
ratio
of
in 1.6
the this
range mixture, case
instead
of
of
llOO-14OO’C
again, with the
is
value
of
10 hra.
of
Mg. At a
catalyst
2.4.
has
The
Mixture
dependence
con-
weight
6 that
was
after
top
level
to
1400’C.
tion
position
effect
a top
of
of
level of
the
B”-A1203
by
Mg apparently
formation
of
heat on time
acts
B”-A1203
to
form of
2Na2CO3.CaCO3.5A1203
treatment
also
temperature
and
was remarkable
From high
experiments
starts
Mg-stabilized with
as and
2Na2CO3-CaCO3-5A1203
composition
given
the corn--
the
almost
a demonstration
temperatures
the
6”-Al203
B-A1203.
tures
in
partially
is
is
of
The mixture
at 159O.C
This
for
especially
mixtures
14OO’C. of
firing
noticeable
concentration
stabilization
lower
mixtures
almoat
a B”/B-Al203
time
the
4.
In the
consists after
Another
binary
the
above
B”-Al203
well-known
At 11OO’C 10 hours
initially
composition
which
temperature
mixtures.
considerable
already
dia-
llOO’C,
corresponding
and MgO.Al203,
disappeared. for
firing
stationary
when
B/B”-Al203
fig.
the
has completely
Na2CO3-A1203
becomes
time
fired
a-Al203
10 hours
below
lOO’C,
for
level
that
the of
temperatures
completely It
mixtures.
it at
the
was observed 700’C
Na2CO3, followed
mix-
a marked
influence
at temperatures
temperature
about
showed
X-ray that with
of up
diffracNa20.A.1203
the
decom-
by decomposition
of
C.M.P.M. Suris, H. Verweij / Formation
192
CaCO3
up
to
8OO'C.
Na20.3CaO.RA1203 starts
to
The form
component at
1OOO'C
of sodium aluminates
at high temperatures
study of ref. 36 if it is assumed that the limit of solubility of Na20.Al203 in Na20.Ca0.2A1203
together with the formation of B/B"-Al203; the
at 11OO'C is such that the overall composition
concentration of this component goes through a
of the mixture is within the phase triangle
maximum at firing temperatures of 12OO'C and is
Na20.Ca0.2A1203/Na20.A1203S.S. -
almost zero after firing at 16OO'C. Due to the
l3"-A1203-Na20.3CaO.I3Al203. This assumption can
complexity of
be made plausible from the observation that at
the
spectra
the
distinction
between E- and 6"-Al203 could not be made with
11OO'C and top level times less than 10 hrs a
lany accuracy. If b/D"-Al203 is counted as one
mixture of only s-s. and Al203 is formed. If it
phase, the number of phases found in the mix-
is assumed that the S.S. already has reached
tures fired at temperatures above 1OOO'C was
equilibrium the composition of the S.S. limit at
always 4, which conflicts with the phase rule.
11OO'C can be estimated to 32% Na20. Wualitati-
This discrepancy can be ascribed to the fact
vely the reaction rate of the components is
that Na20.Al203 and Na20.Ca0.2A1203 form com-
about the same as for the binary Na2CO3-A1203
plete solid solutions (s.s.1 at high temperatu-
mixtures. This gives an
res that decompose on cooling36. No attempt was
sluggish formation of B/B"-Al203 at this tempe-
indication that the
made to estimate the weight composition of the
rature is rate determining :
mixtures because of the complexity of the X-ray
cannot be formed directly from the solid solu-
patterns. The
relative peak
heights of
the
components found are given in Table IV.
Na20.3CaO.RA1203
tion and Al203 without the formation of another Na20-containing compound, which in this case is 6/6'l-Al203.
The course of the reactions at 1200, 1300 and 14OO'C as a function of top level time is qualitatively the same as for the reactions at 11OO'C except that the reaction rates are increasingly higher while the ratio (Na20.3CaO.l3A1203)/(R/B"-Al2O3) steadily decreases. This can be ascribed to a gradual expansion of the two-phase area s.s.-E"-Al2O3, at the expense of the two-phase area
s.s.-Na20.3CaO.BA1203,
towards
the
Na20.Ca0.2A1203 composition with increasing temperature. With this expansion the composition of Table IV Relative peak heights for 2 Na2CO3-CaO-5A1203 mixtures after heat treatment (N q Na20, C = CaO, A = Al2O3).
-6"-Al203 boundary, which means that at some
The reactions at 11OO'C were not yet stabilized
longer present. This phenomenon is indeed obser-
after 100 hours firing. At this temperature the
ved for mixtures, fired at 1600'C. The qualita-
the mixture gradually approaches the low s.s.-
temperature above 14OO'C these two phases will be in equilibrium and Na20.3CaO.RA1203 is no
combination Na20.Ca0.2A1203/Na20.A1203apparent-
tive course of the reactions after 10 hours at
ly reacts very slowly with A1203 to form the
top level as a function of temperature is given
high
alumina
compounds Na20.3CaO.RA1203 and
r'3/B81-A1203. This is in agreement with the phase
in figure 5.
193
C.M.P.M. Saris, H. Verweij / Formation of sodium aluminates at high temperatures probably
a concurrent
E/W’-Al203
the surface
at
reaction
grain
of
boundary
reaction
of
Al203
(3b);
6”-Al203
(and &A1203?)
is not certain
investigation.
uD0
1500
ml0
FIGURE
of
of
the maximum in concentration
the component Na203.CaO.RA1203 is
with
the
slow
but
kinetics
at low temperatures
sing
the
of
of reactions processes
relevant effect
of
for lifetime of reaction
dary coherence tion
1.
and with the cros-
planes. -
for
precursor
phase.
3.
REMARKS AND CONCLUSIONS
micro-precipitates
clusions
results
about
magnesium-
the
and
can be used to draw con-
mechanism of
calcium-containing
sodium vapour in the temperature -13OO’C.
These reactions
into three steps: tion
Reaction
Na20.Al203;
TGA
of with
range of lOOO-
can roughly be divided step 1 must be oxida-
of Na to Na20 by reduction
is s reaction
reactions
of TGA. Step 2
of Na20 and Al203 to the compound fast
formation
of this
compound from
Al203 and Na2C03 was always found in our experiments. Step 3, the actual
corrosion
process,
is
of
be most
The
as it
grain
is
boundary
grain boundary phase network for
instance,
the
Na20.3CaO.RA1203
presence
of
MgO.Al203
or normal second phase seems importance
as it
is
present
along the grain boundaries. of reactions
have to be the subject in which the present useful.
the
connected
only discontinuously Further details
for reac-
Ca seems to
along
for
to be of secondary
is destroyed
boundary corrosion
a perfectly of,
This step,
1. A secondary
becomes available
The Ca0.6A1203-like
formation
The present
rate-determining
is reaction
grain
binary at higher temperatures.
of lamp
lamps.
HP5
an
3 may be that the grain boun-
continuously
provides
be
that the reac-
of the TGA material
6”-Al203 FINAL
to
than the rates
current
The presence
important
S.S.
of further
conclusion
study is
present
Na20.Ca0.2A1203/Na20.A1203
Mg2+ or H+ or
2 and 3 are generally
rates
formation
fast
of reac-
tion
connected
increasingly
boundary lines.
is the subject
One general
so that more surface The occurrence
and a normal
by dissolved
this
means that the primarily
5
on the
drawn from the present
lifetime Relative peak heights of characteristic X-ray 2Na2CO3-CaCO3-5A1203 mixtures reflections of after heat treatment with 10 hours top level time as a function of top level temperature.
(3~)
on grain
order of magnitude larger
T(‘C)
and
grain-boundary
whether the kinetics
tion 1 are influenced
1300
6/B”-Al203
about the same as 3c with normal
other impurities;
1000 1100 1200
Ca0.6A1203-like
to
with B/B”-Al2O3 to stabi-
MgO.Al203 precipitates
900
boun-
MgO.Al203 microprecipitates
bulk reaction, It
a grain
a pseudo
grain boundary planes lized
a number of
(3a);
Na20.Al203,
and
Na20.3Ca0.8A1203
REL. PEAK HT(%l
of
: Reaction of Na20.Al203 with Al203 to
reactions dary
process
1, 2 and 3 will
of more detailed results
may appear
studies to be
C.M.P.M. Saris, H. Verweij 1 Formation
194
of sodium
alumirlates
at high temperatures
REFERENCES 1.
H. Akutsu, Y. Wetarai, N. Saito and H. Mizuno, J. Ill. Eng. Sot. 13 (1984) 341.
21. W.C. Johnson, J. Am. Ceram. Sot. 61 (1978) 234.
2.
H.P. Cahoon and C.J. Christensen, J. Am. Ceram. Sot. 39 (1956) 337.
22. W.C. Johnson and R.L. Coble, J. Am. Ceram. Sot. 61 (1978) 110.
3.
R.L. Coble, J. Appl. Phys. 32 (1961) 793.
4.
E. Dijrreand H. HGbner, Alumina-Processing, Properties and Applications, Materials Research and Engineering Series, Eds. B. Ilschner and N.J. Grant (Springer-Verlag, Berlin, Heidelberg, New York, Tokyo, 1984).
23. D.R. Clarke, J. Am. Ceram. Sot. 63 (1980) 339. 24. P.E.C. Franken and A.P. Gehring, J. ,Mater. Sci. 16 (1981) 384. 25. P. Hing, J. Ill. Eng. Sot. 10 (1981) 194.
5.
S.K. Roy and R.L. Coble, J. Am. Cersm. Sot. 51 (1968) 1.
26. G. de With, P.J. Vrugt and A.J.C. van de Ven, J. Mater. Sci. in press.
6.
J.G.J. Peelen, Ph. D. thesis, Eindhoven University of Technology, 1977.
27. C.A. Beevers and M.A.S. Ross, 2. Kryst. 97 (1937) 59.
7.
H.A. Wang, C.H. Lee, F.A. KrBger and R,T. Cox, Phys. Rev. 827 (1983) 3821.
28. C.R. Peeters, M. Bettman, J.W. Moore and M.D. Glick, Acta Cryst. 827 (1976) 1826.
8.
J.J. Rasmussen and W.D. Kingery, J. Am. Ceram. Sot. 53 (1970) 436.
29. G. Yamaguchi and K. Suzuki, Bull. Chem. Sot. Japan 41 (1968) 93.
9.
S.K. Mohapatra and F.A. Krijger, J. Ceram. Sot. 60 (1977) 141.
30. K. Kato and H. Saalfeld, Minerall. 109 (1968) 192:
10.
R. Mijllerand H.H. Gijnthard,J. Chem. Phys. 44 (1966) 365.
Am.
Neues
Jb.
31. N. Weber and A.F. Venero, Ceram. Bull. 49 (1970) 498.
11. K. Hauffe and D. Hoeffgen, Ber. Bunsen Ges. 74 (1970) 537.
32. J.T. Kummer, Prog. Sol. State Chem. 7 (1972) 141.
12. K. Eigenmsnn and H.H. Gijnthard,Chem.
33. M. Bettman and C.R. Peters, J. Phys.
13.
Lett.
12
(1971)
B.F.
Giichter,
Phys.
73
12. H.
Blum
and
H.H.
Gijnthard,
Chem. Phys. Lett. 17 (1972) 217.
34.
(1969)
Chem.
1774.
M. Bettman and (1971) 1442.
L.L.
Terner,
Inorg.
Chem.
10
14. P.J. Jorgensen and J.H. Westbrook, J. Am. Ceram. Sot. 47 (1964) 332.
35. L.T. Brownmiller and R.H. Bogue, 3. Res. Nat. Bur. Stand. 8 (1932) 289.
15. P.J. Jorgensen, J. (1965) 207.
36. H. Verweij published.
Am.
Ceram. Sot., 48
and
C.M.P.M.
Saris,
to
be
16. H.L. Marcus and M.E. Fine, J. Am. Cersm. Sot. 55 (1972) 568.
37. J.D. 168.
17. R.I. Taylor, J.P. Coad and R.J. Brook, J. Am. Ceram. Sot. 57 (1974) 539.
38. R.C. de Vries and W.L. Sot. 52 (1969) 364.
18. W.C. Johnson and D.F. Stein, J. Am. Ceram. sot. 58 (1975) 485.
39. J.T. Kummer, Prog. Solid State Chem. 7 (1972) 141.
19. R.I. Taylor, J.P. Coed and A.E. Hughes, J. Am. Ceram. Sot. 59 (1976) 374.
40. Y. le Cars, J. Th&y and R. Collongues, C.R. Acad. SC. Paris 274C (1972) 4.
20. W.C. Johnson, Met. Trans. 8A (1977) 1413.
41. J. Liebertz, Ber. Dt. Keram. Ges. 49 (1972) 288.
Hodge,
J. Am. Ceram. Sot. 66 (1983) Roth,
J.
Am. Ceram.