76-Microsilica-gel Bond Castables for Rapid Heat-up
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Transcript of 76-Microsilica-gel Bond Castables for Rapid Heat-up
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MICROSILICA-GEL BOND
CASTABLES FOR RAPID HEAT-
UP
,
,
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Microsilica-gel bond castables for rapid heat-up.
Bjrn Myhre*, (Elkem Silicon Materials, Norway)Abstract:Microsilica has traditionally been used as a reactive filler in refractory castables. Recent investigations have however
shown that for some of these applications, microsilica also act as binder, giving the desired setting by a coagulationbond (gelling). Normally that coagulation is effected by reaction between calcium ions from cement and microsilica
and the bonding is strong enough to be practically useable. This paper presents this bonding and gives examples of
results obtained under laboratory conditions. Among the very interesting properties of the gel-bond is the absence of
chemically bonded water, which yields castables that can be heated very quickly once they have been dried at low
temperature. Silica sol was also checked as a complimentary binder. The results show a positive effect on the dried
strength.
Introduction and Background
Figure 1: A view of the microsilica process from thestoking deck of a 27MW silicon furnace producing
Elkem Microsilica 971.
Microsilica:
The word microsilica has become generic for
condensed silica fumes produced as by-products of
silicon and ferro-silicon production. Microsilica, also
known as fumed silica, volatilized silica etc. normally
originates from the loss of SiO(g) which is an
intermediate species in the production of silicon or
ferrosilicon. It is difficult to state exactly when the
term microsilica first appeared, but in the early
1980s Elkem registered Elkem Microsilica as a trade
name for their fumed silica. It is probable that this is
the origin of the generic use of microsilica.
Silicon and ferrosilicon is produced in large electrical
smelting furnaces by the reduction of quartz (SiO2)
with carbon. The raw materials are added from the
top of furnace and form a stack. The actual reduction
to metal occurs in the bottom of the stack. Quarts and
the other raw materials are added as fairly large lumps
which heats up on their voyage down the stack. The
carbon may be added as a range of sources like coal,
coke or charcoal; which one that is used is normally
the result of economic and other considerations.Additional to the carbon, normally wood-chips are
added to improve the texture of the stack.
In the bottom of the furnace, where the temperature
exceeds 2000C, the reduction takes place through a
series of intermediate reactions producing carbon
monoxide together with other gaseous species. One of
these reactions produce the volatile species silicon
monoxide (SiO) that at temperatures above
approximately 1800C has a vapour pressure
exceeding 1 atmosphere. This gas which at that time
is under pressure, ejects upwards together with CO,
most of the SiO gets trapped as it condenses, but
some escapes and gets oxidized when it comes in
contact with the air above the stack. This is the origin
of microsilica. Of course, as a lot of energy (some 2/3
of that of Si-production) is used in the partial
reduction of quartz to silicon monoxide, this
represents a loss for the metal producer. Therefore
most metal producers aim for a minimum silica loss.
Nevertheless, some silicon monoxide will always
escape and give microsilica. Typically 10-15% of the
quarts ends up as microsilica under good furnace
operation.
It is not only silicon monoxide that leaves the furnace.
Also a number of impurities are volatilized. The
source of which are the raw materials. Typical volatile
impurities are oxides of alkalis. One of the moresignificant impurities is carbon of various sources.
The carbon of the microsilica is present as several
forms: coke residues, silicon carbide, some tar related
organics and finally as carbon black.
Above the top of the furnace, which essentially is an
open construction, a hood is placed and with the aid
of huge fans, the volatiles are sucked off and forced
through a filter. Because of the suction and because
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the furnace is top-charged, also larger particles like
wood-chips, coke residue and quarts dust are
collected together with the fumes.
Because of the introduction of foreign matter,
microsilica has to be beneficiated to give a high
quality product. In Figure 2, microsilica production is
schematically shown together with a view of the
Fiskaa plant in Norway: The raw materials are fed
into the top of the furnace (A) this is the stoking
deck. The volatiles are sucked off by a fan (D). To get
rid of the coarse particles, the microsilica is treated in
a pre-collector (C). The gas is then blown into a
baghouse filter and collected as raw microsilica.
Further treatment may be given to achieve desired
properties of the product. It should be mentioned that
other filtering equipment than baghouse filters have
been and are being used.
Figure 2: A view of the Fiskaa plant (Norway)together with a simplified flowsheet of the production
of microsilica. (A) Furnace, (B) Chimney, (C) Pre-
collection, (D) Fan, (E) Baghouse filter.
Properties of MicrosilicaIf we grab a handful of microsilica, the appearance is
a fine powder with variable color from almost black
to slightly off-white. There is a strong correlation
between the color and the carbon content. This
correlation is not straight forward though, since the
carbon may be present as coke residue or as silicon
carbide additional to carbon black which is the
impurity influencing color. A closer examination ofthe microsilica by electron microscopy reveals sub-
micron spheres with an average particle size of
approximately 0.15 micron. The surface area, as
determined by nitrogen adsorption (BET), typically
gives values around 20 m2/g which is equivalent to a
spherical diameter of 0.14 micron, i.e. close to the
results obtained by electron microscopy.
Chemically, microsilica consists of amorphous SiO2
with variable purity. Without going into detail, it may
be stated that there is a close relation between the
furnace operation and the quality of the microsilica.
Hence traditionally, the purity of the microsilica tends
to be rather variable, reflecting the furnace operation
at the time it was collected. As the metal normally is
the main product and microsilica the by-product, a
variation in the performance of the microsilica should
thus be expected. Here it should be mentioned that it
is possible to stabilize microsilica quality, but the
procedures required normally adds to cost (like
lowering Si-yield) thus justifying the higher price for
such controlled products (e.g. 971 from Elkem).
Figure 3: Micrograph of a microsilica cluster showing
spherical appearance of the individual particles.
The crystalinity of microsilica is variable according to
source and beneficiation, but values below 0.3 % by
weight 1 have been reported. Unpublished work on
high purity microsilica did however not show any
traces of crystalline silica. When crystallinity is
observed in microsilica, the source is normally quartzcarry-over from the furnace charging. In some special
cases with extended residence time at high
temperatures (> approx 800C for many hours) some
of the microsilica may crystallise as well. The
crystallisation can be accelerated by impurities,
notably alkalies. Such crystallisation should for high
quality microsilica be regarded as negligible though.
Microsilica higher in impurities e.g. alkali levels
above 1% might have more crystalline matter than
purer types.
As shown in Figure 3, microsilica consists of spheres.
These have an average diameter of about 0.15 micron.
The spheres are the building units of agglomeratesthat has been believed to be bonded together by
material bridges2. Improvements in PSD measuring
equipment have however given PSD curves (Figure 4)
that are in good agreement with the results from SEM
and BET surface measurements and the commonness
of those material bridges becomes questionable.
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Figure 4:Typical particle size distribu
dispersed microsilica as measured by la
Although microsilica is dispersed
spheres as seen in Figure 3 & 4, the no
castable is probably as a mixture of dis
and agglomerates. The more dispersed
gets, the better will the resulting flow
is present in sufficient amounts), partic
flowing castables. In free-flowing
increased amount of superfines (e.g. m
acts as flow-enhancers by reducingfriction between the larger aggregates.
The microsilica surfaceEven though the overall composition o
SiO2, the surface of a microsilica parti
siloxane bonds, but is also partially hy
hydrated. Producers of fumed silic
Evonik Degussa) have been very
characterisation and modification of th
in order to tailor specific properties
and fumed silica.
Figure 5: Visualization of the microsili
and with water.
Based on theoretical and experiment
seems that the maximum density of s
groups on the surface of silica is
4.6nm-2.
The surface of microsilica is also co
silanol groups, although the presence
plays some role, measurements have indensities ranging from approximately 2
microsilica from silicon productio
correlation between theoretical valu
found for microsilica may indicate that
of the microsilica are not smothere
surface of the microsilica particles
discrete particles or dissolved in
combination is probable.
tion of a well
ser diffraction.
as individual
rmal state in a
persed spheres
the microsilica
e (provided it
ularly for free-
castables an
icrosilica) also
inter-particle
f microsilica is
le is not plain
droxylated and
(particularly
active in the
silica surface
of precipitated
ca surface, dry
al results 3 , it
lanol (Si-OH)
approximately
ered by such
of impurities
dicated silanolto 4.5nm-2for
. The good
es and those
the impurities
d out on the
but rather as
the silica. A
The presence of the silanol
microsilica easy to disperse i
Depending on the pH, a fraction
dissociate (to H+ and O-) resul
charged surface. The zeta-potent
and values higher than approxim
or negative) are often taken as a
suspensions. Figure 6 shows a m
zeta potential for Elkem Microsi
that the microsilica has a negat
whole range. Due to dissociation
the negative surface charge incr
approximately pH 7. At higher
potential flattens out and at
microsilica starts to dissolve.
Figure 6: Zeta potential of Elkem
function of pH. A 10% microsili
HCl and with zeta potential be
electro-acoustic techniques (Ac
Dynamics)
It is the negative charge on
microsilica that is the property
bonding possible. Such negative
cation and if it is a polyvalent
two adjacent microsilica particle
three dimensions, a gel of
constructed. Figure 7 visualises
dimensions using Ca2+as the brid
Figure 7: Proposed gellin
microsilica-gel bond. Ca2+
microsilica particles.
-35
-30
-25
-20
-15
-10
-5
0
1 2 3 4 5
pH
Zeta-potential(mV)
O-H
O-HH-O
H-O
H-O
O-
O-
O-
O-
OH
O-
+Ca+Microsilica
+C
+Ca+
+Ca+
+Ca+
+Ca+
O-
O-H
H-O+
Microsilica
groups makes the
aqueous systems.
of the silanol groups
ting in a negatively
ial can be measured
tely 25mV (positive
indication of stable
asurement of such a
ica 971, and we see
ive charge over the
of the silanol groups,
ases with pH up to
pH than 7, the zeta
till higher pH the
Microsilica 971 as a
a slurry titrated with
ing measured using
ustosizer, Collodial
the surface of the
that makes the gel-
sites can react with a
ation it may bridge
s. If this happens in
that microsilica is
this process in two
ging cation.
mechanism for
gelling adjacent
6 7 8 9
O-H
O-H
O-H
O-
O-
O-
icrosilica
a+
+Ca+
a+
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Castables based on this bonding concept was
presented as early as at UNITECR 1995 in Kyoto4,5.
At that occasion, also the accelerating effect of
combining small amounts of cement with Alphabond
was demonstrated (Table 1). It was not clear to the
authors what mechanisms was causing the setting, at
that time; it was just assumed that one was talking
about a hydraulic bond of the cement.
Table 1 Fused alumina based castables. Setting time
(days at 20C) for combinations of Alphabond and
cement. Alphabond content (mass%) in left column
and cement content (mass%) in first row.
Alphabond/Cement 0 0.25 0.50 1.00 2.00
0 10 5
0.50 1 1
1.00 18 1
2.00 13 1 1
3.00 4 1
5.00 2
At UNITECR 20116, also this time in Kyoto, a further
study on basically the same system as in 1995 was
presented. At this occasion the setting had been
studied by simultaneous zeta-potential, conductivity
and pH measurements showing that there is a
simultaneous setting combined with a sequestering of
ions in the liquid phase. Figure 8.
Figure 8, Zeta-potential, conductivity and pH of a
slurry mixture of 8parts microsilica, 0.5parts cement,
0.5parts Alphabond, 0.05parts deflocculant
(Castament FS20) and 4.15parts water as a function
of time.
Based on these results, the setting mechanism
proposed in Figure 7 was formulated. The
accelerating effect that had been seen for Alphabond
additions was explained by the Alphabond serving as
nuclei for precipitation of alumina from the liquid;
thus facilitating increased dissolution of Ca2+from the
cement. This in turn reacts with the negatively
charged microsilica surface causing a gel to form.
To test the effect of the setting on real castables,
some compositions based on white fused alumina
with 8wt% microsilcia in combination with different
combinations of cement a Alphabond, were prepared
with 4.1% water. Top size was 5mm and dispersant
was 0.05% Castament FS20. Results from flow decay
measurement s are shown in Figure 9.
Figure 9. Flow decay of combinations of cement and
Alphabond, WFA based castables with 8 wt%
microsilica and 4.1% water.
Clearly, by adding alphabond to the castable together
with 0.5% cement, setting is accelerated. A similar
effect can also be found by using a fixed amount of
Alphabond with the cement as variable. Increased
amounts of Alphabond tend to lower flow though.
Flow and Strength.It should not be surprising to expect that the result of
a bond consisting of a gelled microsilica should be
fairly low. But just what levels are sufficient for
demoulding and handling?
Braulio et al7indicates that an initial splitting tensile
strength higher than 1 MPa would be enough to avoid
crack generation during demoulding. 1MPa splitting
tensile strength is, depending on citation, equivalent
to between 1.3 to 1.4MPa M.O.R. In other words, any
M.O.R value above 1.5MPa should be sufficiently
strong.
Even though a lot of information (e.g.8and9) was
available on the hot-strength of castables based on themicrosilica-gel bond, we had surprisingly few results
from low temperatures. Therefore it was decided as
part of another investigation to measure flow and
green-strength of a chosen castable, the recipe is
given in Table 2.
As good results also were obtained with lower water
additions10such as 3.5% water, it was chosen to make
the mixes with both the custom 4.1, and with 3.5%
-60
-50
-40
-30
-20
-10
0
10
20
30
0.00 2.00 4.00 6.00 25.00 29.00
time[h]
[mS/cm]/[mV]
0.00
1.00
2.00
3.00
4.00
5.00
6.00
7.00
8.00
9.00
10.00
pH
conductivity [mS/cm]
Zeta-potential [mV]
pH value
0
40
80
120
160
200
0 2 4 6 8 10 12
Time [h]
Flow
-value
%
0.5%Cement + 0.0%Alphabond Free-flow 0.5%Cement + 0.0%Alphabond Vibra-flow
0.5%Cement + 0.5%Alphabond Free-flow 0.5%Cement + 0.5%Alphabond Vibra-flow
0.5%Cement + 1.0%Alphabond Free-flow 0.5%Cement + 1.0%Alphabond Vibra-flow
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water. For the flow measurements, the flow cone
(height 50mm) as described in ASTM C 230 was used,
but since the European standard EN 1402-4 prescribes
the use of a taller cone (height 80mm) for self-flow
measurements, both self-flow using the ASTM cone
and the EN-cone was measured.
Table 2: White fused alumina castables withmicrosilica gel bond.
NCC microsilica-gel bond [weight %]Elkem Microsilica 971U : 8CAC cement, Secar 71 : 0,5Alphabond 300 : 0,5White Fused Alumina 3-5mm : 10White Fused Alumina 0,5-3 mm : 32White Fused Alumina 0-0,5mm : 16White Fused Alumina -74 mic : 20Calcined alumina,CT 9FG : 13Dispersant, Castament FS20 : 0.05
Figure 10 shows the flow values of the castable of
Table 2 with 3.5% and 4.1% water. It is remarkable
how high the self flow is even at 3.5% water, yielding
values that normally are found for significantly higher
water additions. Here it should be mentioned that to
obtain such high flow values, the microsilica quality
plays a decisive role. It is of uttermost importance
that the microsilica is easy to disperse and that the
mixture does not contain flocculating contaminants
like easily dissolvable salts, notably polyvalent.
Lowering the water addition creates one problem
connected to extended wet-out time. At very low
water additions the wet-out becomes difficult, if theresults of Fig. 10 are taken as an example, the wetout-
time increased from 20 to 45 seconds when water was
reduced from 4.1 to 3.5%. Even lower water additions
can be used, but then wetout-time becomes a
problematic issue. In such cases different strategies
can be sought like mixing parts of the mix with the
water and afterwards adding the rest of the dry mix
etc.
Some hours after the mixing, the castable sets but will
it be possible to demould the piece? Figure 11 and 12
shows the strength green after 24 hours and after
subsequent drying at 110C.
Figure 10: Flow of the white fused alumina based
NCC base on the microsilica-gel bond. Flow values
measured with 3.5 and 4.1% water.
Figure 11: WFA based microsilica-gel bonded
castables cast with 3.5 and 4.1% water. Strength
measured green (undried) after 24hours and after
subsequent drying at 110C/24h.
The green C-M.O.R. was found to be around 2MPa
for both water additions. Although low, it should
according to Braulio et al. be possible to demould.
Drying increases the strength significantly and herethe lower water pays off yielding significantly higher
strength.
87
128 124124
152
180
0
20
40
60
80
100
120
140
160
180
200
self-flow vibra-flow self-flow
ASTM cone ASTM cone EN cone
Flowvalue[%]
3.5% water
4.1% water
2.0
2.3
7.9
0
1
2
3
4
5
6
7
8
9
Green 20C Dried at 110C
Cold-M.O.R.[MPa]
4.15% water
3.5% water
5.3
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Figure 12: WFA based microsilica-gel bonded
castables cast with 3.5 and 4.1% water. Strength
measured green (undried) after 24hours and after
subsequent drying at 110C/24h.
Figure 12 shows the CCS of the samples again
demonstrating the good effect of drying.
Explosion resistanceAt IREFCON 20128Myhre and Fan presented results
on explosion resistance using the castable
composition of Table 2. They compared the results of
the microsilica-gel bond with results using a similar
LCC composition using 6% CA-cement. The
composition is given in Table 3.
Table 3 Low-cement castable based on white fused
alumina. 4.15% water for casting.
LCC CA-cement bond [weight %]Elkem Microsilica 971U : 8CAC cement, Secar 71 : 6White Fused Alumina 3-5mm : 10White Fused Alumina 0,5-3 mm : 32White Fused Alumina 0-0,5mm : 16White Fused Alumina -74 mic : 16Calcined alumina,CT 9FG : 12Dispersant, Castament FS20 : 0.05
Based on the recipes given in Table 2 and 3, a set of
NCC (microsilica-gel bond) and LCC castables were
cast with 4.15% water. Samples were cast into 50mm
cubes as described in the Chinese standard
YB/T4117-2003.
The standard describes placing green (not dried)
samples (cubes of 50mm) into a furnace heated to a
preset temperature and inspecting the sample after 30
minutes. The temperature at which cracks forms or
explosion occurs is then reported as explosion
resistance.
After 24 hours curing at 100% relative humidity and
20C, the demoulded samples were protected from
drying before being placed into the furnace for 30
minutes. After inspecting the samples for cracks etc.,
the temperature of the furnace was increased and a
new sample inserted into the hot furnace. This was
repeated until cracks or explosions were detected.
In Table 4, the results are shown. It became quickly
clear that the undried NCC exploded into tiny
fragments already at 350C, whilst the LCC was able
to take 600C before it split in two pieces. The low
explosion resistance of the NCC surprised us since we
were convinced that the NCC should take heat-up
very well due to the lack of bonded water. Could it be
that our assumptions of only minute amounts of
bonded water were incorrect? It was quickly
suggested that low strength also could be a reason for
the steam explosion of the NCC when tested
green/undried. To check, samples were dried at 110Cbefore testing. Testing of the dried samples gave a
very different result. The LCC split in two pieces at
600C as it did for the undried sample, but the NCC
was virtually indestructable even at temperatures as
high as 1200C!
Table 4: Results from explosion testing of the
castables shown in Table 2 and 3.
Temp.[C]Before drying
After drying at110C
LCC NCC LCC NCC
200
250
300
350
400
500
550
600
800
1000
1200
:sample passed the test, :sample did not pass.Reducing the casting water from 4.15 to 3.5% gives
benefits beyond those related to strength. It does
increase the explosion temperature. In our testing an
increase from 350 to 500C was experienced. Table
5 shows a comparison between the two.
12.4
39.4
16.8
62.2
0
10
20
30
40
50
60
70
Green 20C Dried at 110C
CCS[MP
a]
4.15% water
3.5% water
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Table 5: Explosion resistance for NCC samples tested
green i.e. directly from the mould. Samples with
4.15 mass% and 3.5 mass% water for casting.
Temp. [C] NCC (microsilica-gel bond)4.15 mass%water
3.50 mass%water
300 350
400
500 :sample passed the test, :sample did not pass.
It is seen that drying at 110C does not affect the
explosion resistance of the LCC indicating that the
bond is not considerably changed during the drying.
The fact that it tolerates temperatures up to 600C
before failing the test is probably an effect of the
good strength of the castable. The improvement of the
NCC by lowering the water may also be similar, not
only is the amount of water less, but the strength is
improved as well.
The excellent results of the dried NCC was attributed
to the low amount of residual water in the bond after
drying. To substantiate this hypothesis, a series of
gravimetric experiments were undertaken and the
following figure, Figure 13, was presented at
IREFCON 20128
Figure 13: Weight loss of microsilica-gel bonded
NCC as a function of thermal treatment. Castable of
Table 2 cast with 4.15% water.
According to these results, some 89% of the water
disappears at 110C, leaving only 10.84% of theoriginal 4.15wt% water (0.45wt%). Somewhat
surprising, it was found that as much as 19% (0.78
out of 4.15%) had disappeared before drying at 110C.
It is assumed that most of this loss came during the
handling and weighing of the samples after
demoulding.
We felt that we should have a correlation with the
LCC in order to explain and verify our hypothesis.
Therefore some additional gravimetric investigations
were performed on the LCC composition using 4.15%
water. Instead of 800C a temperature of 600C was
chosen as firing temperature since firing at 1000C
did not give any further weight loss. Figure 14 shows
the results obtained on the LCC sample.
Figure 14 shows that the residual water was as high as
27% after drying at 110C. If this difference is tied up
in hydrates that both clog the pore structure and
liberates over a narrow temperature range, it may well
result in bursting of the sample at 600C.
Figure 14: Weight loss of LCC as a function of
thermal treatment. Castable of Table 3 cast with 4.15%
water.
Silica sol
After the patents (e.g. 11 ) of Magneco Metrel
concerning use of silica sol as binder in refractorycastables recently started to expire we have seen an
incrteased interest in using silica sol as binder. This
has to some extent puzzled us since basically we are
dealing with a variation of the bond system treated in
this paper, i. e. the microsilica-gel bond. The
difference is that a liquid silica sol (sometimes termed
colloidal silica) is made to gel by some gelling agent.
If used together with microsilica, it becomes very
difficult to distinguish between the effects of the
gelling of the sol or the microsilica. To check for
beneficial effects of silica sol additions, we set up a
program where parts of the microsilica was replaced
by silica sol. The silca sol was a silica of 130m2/g
dissolved in an aqueous liquid at 40weight%, while
compensating for the added liquid, so that silica
sol+microsilica and total water was kept constant at 8
and 4.1% respectively. It was expected that the
addition of the silica sol that was much finer than
microsilica, could complement on particle packing
and thus enhance flow. Alternatively a chance existed
that the IPS (interparticle separation), would become
too small so that the particles started to interact and
18.80%
70.36%
10.84%
Curing 20C Drying 110C Firing 800C
10 %
63 %
27 %
Curing 20C Drying 110C Firing 600C
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thus influence flow negatively.
In Table 6, the experimental set up, the recipes, are
given, the compositions were made so that amount of
liquid and amount of superfine silica should be
constant at 4.1 and 8% respectively.
Table 6: Castables with silica sol. The compositions were made so that amount of liquid and amount of silica should
be constant at 4.1 and 8% respectively.
[weight %]Elkem Microsilica 971U 8 7.8 7.2 6.4 5.6CAC cement, Secar 71 0,5 0,5 0,5 0,5 0,5Alphabond 300 0,5 0,5 0,5 0,5 0,5White Fused Alumina 3-5mm 10 10 10 10 10White Fused Alumina 0,5-3 mm 32 32 32 32 32White Fused Alumina 0-0,5mm 16 16 16 16 16White Fused Alumina -74 micron 20 20 20 20 20Calcined alumina,CT 9FG 13 13 13 13 13Dispersant, Castament FS20 0.05 0.05 0.05 0.05 0.05
Silica sol: BindZil 40/130 % 0 0,5 2 4 6Water 4.1 3.8 2.9 1.7 0.5
Figure 15: Flow (ASTM cone) as a function of silica
sol addition. Castables with a total of 4.1% water and
8% silica according to recipes given in Table 6.
Figure 15 shows the flow values of the castables in
Table 6 as measured with the 50mm tall ASTM cone.
Up to 4% silica sol addition, the flow is unaffected,
from 4% on a decrease becomes obvious. The reason
for this is not obvious, but may be connected to the
high surface of the colloidal silica. At 4% silica sol
the colloidal silica has a surface area similar to 8-10%
microsilica. As a consequence, the IPS decreases,
possibly to a level where interactions start to become
noticeable. At what distance particle-particle
interaction starts to become problematic is difficult to
predict, but distances of 50-70nm has been suggested
in literature12..
If the water in our mix (i.e. that with 4% silica sol)
is evenly distributed on the silica surface, then rough
calculations without taking interparticle porosity into
consideration, yields a layer of approximate 11nm
thickness, - or an average particle-particle distance of
22nm. This is well below the 50-70nm suggested in10.
With addition of more silica surface, it was
considered probable that this could result in better
strength values due to lower IPS and more silanol
groups. Figure 16 shows the cold modulus of ruptureand the cold crushing strength as measured
immediately after demoulding. The samples had been
cured for 24 hours at close to 100% relative humidity
prior to the testing.
Opposite to the expectations, no positive effect of the
silica sol additions were seen in the green state. A
possible explanation could be that the Bindzil is
stabilised in such a way that it does not react with
Ca2+under alkaline conditions. The rather high pH of
9.2 13 of the Bindzil indicate that some sort of pH
adjustment has been performed on it. Such adjustment
could possibly render the silica surface unreactive
under the present coagulation conditions.
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Figure 16:Green strength as a function
addition. Castables with a total of 4.1%
silica according to recipes given in Tab
After drying however, the picture iFigure 17, it is seen that both M
increases with the addition of silica
during the drying at 110C, the silica
bonding. The mechanism behind is diff
but it has been put forward14
that the
on the silica surfaces may condens
siloxane and water. This condensation i
Figure 17.
Figure 17:Dried strength as a function o
addition. Castables with a total of 4.1%
silica according to recipes given in Tab
f silica sol
water and 8%
e 6.
s changed. InR and CCS
ol. Somehow,
sol improves
cult to explain,
silanol groups
e to bonding
s illustrated in
f silica sol
water and 8%
e 6.
Figure18: Suggested12silanol co
drying of microsilica containing
Although probable, we do not h
this mechanism. Nevertheless
strengthening following th
strengthening seems to be depe
of silica sol so even if the sili
green-bodies, it contributes to hig
The overall conclusion may the
in the following way: If it is pos
silica sol additional to the dry-m
in green-strength is not a problegood idea to make castables
microsilica is supplemented with
resistance has not been tested, bu
similar results as the non-silica so
Hot strength
This paper is not intended to pre
hot-properties of this type of
figures taken from another sou
bond systems.
It is an old experience that iftogether with cement, often
refractoriness may suffer severel
comparison between the refrac
(R.U.L.) of three castables based
given in Table 2 and 3 with 8 ma
two LCC differ in the type of c
common 70% CAC the other
clearly seen that the reduction in
leads to improved refract
improvement comes for our
NCC with properties that can
temperatures up to 1800C. All
formation, a topic that has been tearlier 15 publications. Brief
microsilica, in absence of cement
and forms mullite. The situation
cement is present. A liquid is
composition close to 50 mass%
combination with 50 mass% mi
castable with 5 mass% micros
cement is tested, then 10 mas
1500C. The result is a catastr
densation during
LCC and NCC.
ve firm evidence of
we do observe
e drying. This
dent on the amount
a sol gives weaker
her dried strength.
efore be formulated
ible to have a liquid
ix, and the lowering
m, then it may be ahere some of the
silica sol. Explosion
t is expected to yield
l compositions.
sent much about the
astable, just a few
ce10 with the same
microsilica is usedmass% of each,
. Figure 19 shows a
toriness under load
on the compositons
ss% microsilica. The
ment used, one is a
an 84% CAC. It is
CaO (84% cement)
riness. The big
icrosilica-gel bond
ake it applicable at
his is due to mullite
reated extensively iny described, the
, reacts with alumina
is quite different if
formed that has a
70% CA-cement in
rosilica. So if e.g. a
ilica and 5 mass%
s% liquid forms at
ophic failure of the
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castable when temperature reaches 1500C This may
be seen in Figure 9 as the almost vertical drop at
1500C.
Fig. 19: Effect of cement on RUL for WFA based
castables with 8 mass% microsilica. LCC has6 mass% cement.
Compared to microsilica free castables, the
microsilica-gel bond shows similar refractoriness,
Figure 20. When using the microsilica-gel bond it is
possible to obtain a refractoriness equal to or even
above the microsilica-free LCC alternative.
Fig. 20: Comparison of RUL for WFA based
microsilica-gel bond NCC (0.5 mass% cement) with 8
mass% microsilica, LCC (6 mass% cement) with 8mass% microsilica and LCC (6 mass% cement)
without microsilica
Conclusion:
For castables are based on gelation of microsilica as
bond system, several attractive properties have been
identified. These are; very good placing properties
combined with high refractoriness and hot strength.
The green strength is low but sufficient, and the dried
strength is good. Further, the bond contains only
small amounts of bonded water, so once the free
water is removed, the castable tolerates very high
heating rates. If silica sol is used complementary to
the microsilica, improved strength was seen for the
dried samples. The green strength did not benefit
however.
In general, the gel-bond offer attractive possibilities
for advanced refractories, opportunities that may be
difficult to match with alternative bond-systems.
References:
1K. Heggestad, J.L. Holm, K. Lnvik and B.
Sandberg, "Investigations of Elkem Microsilica by
Thermosonimetry", Thermochimica Acta, 72 (1984),
205-2122E.Dingsyr, M. Dstl and C. Wedberg, in "Preprint
of the Fifth European Symposium Particle
Characterization, 24-26 March 1992, Nrnberg,
Germany. publ. by Nrnberg Messe GMBH3 R.K. Iler, The chemistry of silica, John Wiley &
Sons, New York 1979.4B. Myhre and K. Sunde, "Alumina based castables
with very low contents of hydraulic compound. Part I:
The effect of binder and particle-size distribution on
flow and set.", Proc. UNITECR95, Kyoto, Japan,
Nov. 19-22 1995, p. II/309-165B. Myhre and K. Sunde, "Alumina based castables
with very low contents of hydraulic compound. PartII." Strength and High-Temperature Reactions of No-
cement Castables with Hydraulic Alumina and
Microsilica, Proc. UNITECR95, Kyoto, Japan,
Nov. 19-22 1995, p. II/317-246B. Myhre and H. Fan, Gel Bonded CastablesBased on Microsilica as Binder, proc.
UNITECR20117 M. A. L. Braulio*, V. C. Pandolfelli and C. Tontrup,
Colloidal Alumina as a Novel Refractory Castable
Binder proc. 53rd Int. Coll. on Ref. Aachen 2010 p.
111-1148B. Myhre and Aase M. Hundere: Substitution of
Reactive Alumina with Microsilica in Low Cement
and Ultra Low Cement Castables. Part I: Properties
Related to Installation and Demoulding Proc.
UNITECR97, New Orleans, USA, Nov. 4-7 1997, p.
43-529Aase M. Hundere and B. Myhre: Substitution of
Reactive Alumina with Microsilica in Low Cement
and Ultra Low Cement Castables. Part II: The Effect
of Temperature on Hot Properties Proc.
-2
-1
0
1
2
0 500 1000 1500 2000
Temperature [C]
Expansion[%]
LCC (70% CAC)
LCC (84% CAC)
0.5% (70%CAC)
-2
-1
0
1
2
0 500 1000 1500 2000
Temperature [C]
Expansion[%]
0.5% cement 8% MS6% cement 8% MS6% cement , 0% MS
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UNITECR97, New Orleans, USA, Nov. 4-7 1997, p.
91-10010Bjrn Myhre and Haibing Fan, Microsilica-gel
bond for explosion proof castables proc. IREFCON
2012, Kolkata 2012 p 71-7611US pat. 5147830 Composition and method for
manufacturing steel-containment equipment
Subrata Banerjee et al12J.E. Funk and D. R. Dinger:"Particle Size Control
for High-Solids Castable Refractories", Am. Ceram.
Soc. Bull.73[10],66-69, (1994)13ALBIN KLINT, Amphiphilic surface modification
of colloidal silica sols, Master of Science Thesis in
the Master Degree Programme Chemistry and
Bioscience, Department of Chemical and Biological
Engineering, Division of Applied Surface Chemistry
CHALMERS UNIVERSITY OF TECHNOLOGY,
SWEDEN14Li Zaigeng et al., Phase Compositions and Setting
Mechanisms of Low Cement, Ultra-low Cement andCement-free Castables in Proc. 2nd Int. Symp on
Refr. Beijing China, Oct. 30 - Nov. 2 1992, p.
540-54715B. Myhre: Lets Make a Mullite Matrix! Ref.
Appl. and News, vol 13, No 6, 2008