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Lecture #8 - Alfred's Clay Store

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Firing<br />

<strong>Lecture</strong> <strong>#8</strong>


Firing<br />

• The final frontier<br />

– Work either makes it or breaks it<br />

• Even when forming and drying conditions<br />

are ideal, we can still loose work at this<br />

stage<br />

• Understanding the firing process can help<br />

us avoid costly mistakes<br />

• Before looking at firing, we will look at<br />

silica, as it is integral to the firing process


(alpha)<br />

(beta)<br />

(alpha)<br />

(beta)<br />

(no inversion)<br />

• A changes from one<br />

phase to another is<br />

called a silica<br />

conversion<br />

• Conversions are not<br />

reversible - they are<br />

one way streets<br />

• Within the same<br />

phase, a change from<br />

one form to another is<br />

called a silica<br />

inversion<br />

• Inversions are<br />

temperature dependent<br />

and are reversible


Quartz<br />

• Also known as free silica<br />

– “free” distinguishes this silica as not being chemically<br />

bound to other molecules (i.e. the silica in our Kaolinite<br />

crystal is not “free”; it’s bound with alumina)<br />

– If you had very small tweezers and steady hands, you<br />

could remove free silica from the clay<br />

• The major impurity found in clay<br />

– Up to 85% of a naturally occurring clay can be quartz<br />

• Quartz is also added to a body through flint or<br />

sand


Determining free silica in clays<br />

• Pure kaolin contains<br />

46% SiO 2 ; 39%<br />

Al 2 O 3<br />

– Silica above 46% is<br />

free silica<br />

• Secondary clays<br />

contain more free<br />

silica than primary<br />

clays<br />

– They have picked up<br />

silica in their travels<br />

% SiO 2 Al 2 O 3<br />

Grolleg 47.7 37.7<br />

OM4 53 30.8<br />

Red Art 54.3 16.4<br />

Hawthorn 55.1 39.11<br />

KT Stone 67.1 20.7


Alpha to Beta Quartz<br />

1064°F<br />

<br />

• 573 °C (1063 °F ) is known as the quartz inversion point<br />

• Quartz below 573 °C is always alpha quartz<br />

• Quartz above 573 °C is always beta quartz<br />

• Every time we pass the quartz inversion point, quartz<br />

inversion takes place


Effect of quartz inversion<br />

Alpha<br />

• As we approach the<br />

inversion temperature,<br />

the angle of bonding<br />

between silica<br />

tetrahedra changes<br />

– There is a straightening<br />

the the silica molecules<br />

Beta


Effect of quartz inversion<br />

573°C<br />

<br />

1%<br />

volume<br />

change<br />

• The straightening of the silica molecules<br />

accounts for approximately 1% volume<br />

expansion from alpha to beta quartz<br />

• This affects all quartz in the body


Alpha/Beta quartz expansion<br />

Inversion Point<br />

• Volume expands progressively quicker with<br />

temperature until it reaches the inversion point


Cristobalite inversion<br />

• Like quartz, cristobalite has two forms<br />

– Alpha and Beta<br />

• Inversion from Alpha to Beta occurs at 226 °C (439 °F)<br />

– Occurs more rapidly than quartz inversion<br />

– Like all inversions, this is reversible<br />

• Up to 3% volume change!<br />

• Happens at lower temps. when the body is rigid<br />

• Porous bodies handle cristobalite inversion better than<br />

dense bodies<br />

– Porous bodies can absorb shock better than tighter bodies


Alpha/Beta cristobalite expansion<br />

• Volume expansion increases suddenly at the<br />

inversion point


Poorly mixed<br />

Well mixed<br />

Silica<br />

<strong>Clay</strong><br />

Glass<br />

Cristobalite<br />

Cristobalite can form<br />

Cristobalite won’t form<br />

• Cristobalite formation is promoted by poor mixing<br />

– Clumps of silica in poorly mixed bodies can form cristobalite<br />

(because silica inside the pocket is isolated)<br />

– Isolated silica grains in a well mixed body form glass (each silica<br />

particle is surrounded/coated by clay)<br />

• We can avoid cristobalite by ensuring no two quartz<br />

particles touch<br />

– there is enough clay in any recipe to do this (assuming proper<br />

mixing takes place, i.e. Shar it!)


Cristobalite<br />

• Forms at higher temperatures<br />

– Free Quartz can convert to cristobalite above 1100<br />

°C (2012 °F ) cone 02<br />

• Temperature varies based on fluxes and time<br />

• Soaking above 1100 °C increases cristobalite formation<br />

• Conversion to cristobalite is irreversible as<br />

silica bonds of quartz are destroyed and<br />

reformed as cristobalite<br />

– Once cristobalite forms, it won’t go back to quartz


Glass<br />

• Glass forms when silica is melted and cooled<br />

quickly enough so that the silica tetrahedra cannot<br />

establish a pattern of structure<br />

– Crystalline matt glazes require slow cooling for this<br />

same reason<br />

– Glass is also referred to as non-crystalline silica<br />

• Glass sources in bodies include flint, feldspar, free<br />

silica and silica from clay minerals (i.e. kaolinite<br />

crystal)<br />

• Unlike quartz and cristobalite, silica glass does not<br />

go through inversions<br />

– No alpha or beta form<br />

– Stable throughout the firing process


• Glass Silica<br />

– AKA Amorphous<br />

silica; fused silica<br />

• Glass has a<br />

random structure<br />

• Cristobalite and<br />

Quartz are<br />

crystalline silica<br />

– Ordered,<br />

repeating<br />

structure<br />

Crystalline form<br />

Quartz<br />

Glassy form<br />

Glass


Glass expansion<br />

• Very low expansion


The Three<br />

Tenors<br />

(Like our three<br />

forms of silica,<br />

they’re related)


Minimizing the danger<br />

• Glass phase<br />

– No inversion…no problem<br />

• Quartz phase<br />

– Avoid adding excess free silica (I.e. silica-rich clays, flint<br />

and especially sand)<br />

– Fire slowly through inversion<br />

– Not as problematic as once thought<br />

• Cristobalite phase<br />

– Is not formed at low temperatures<br />

– Can be minimized at higher temps by proper mixing<br />

– Cool slowly through inversion<br />

– Avoid an excess of free silica / avoid soaking at high<br />

temperatures if possible


• Having examined silica’s phases, we will now take a<br />

chronological look at what happens during firing<br />

• Keep in mind that these overlap and that temperature can<br />

vary from one area of a piece to another during firing<br />

– Pyrometer readings can be off<br />

– Temperature at the pyrometer is different from temperature of<br />

the work<br />

– Temperature gradients throughout the work will vary during<br />

firing<br />

• Also, the extent to which these stages occur vary<br />

depending on mineralogy (Kaolinite is used as an ideal<br />

model, though it is not always the main clay mineral<br />

present in a given body)


Pore water removal<br />

• Up to 120 °C (248 °F)<br />

• The initial stages of firing can be seen as a<br />

continuation of the drying process<br />

(dehydration)<br />

• Drying is completed with the removal of the<br />

last traces of water on particle surfaces<br />

– Pore water is removed up to 120 °C<br />

• AKA “water smoking period”


• Explosions occur<br />

when pore water is<br />

removed too<br />

quickly<br />

– At 100 °C (212 °F)<br />

water turns to steam<br />

• Moisture condenses<br />

on a glassy surface<br />

placed above top<br />

spy hole until all<br />

water is removed<br />

– Hold below 100 °C<br />

until no more water<br />

condenses on glass


Organic decomposition<br />

• At approximately 200 °C (392 °F)<br />

• Organic matter, of mainly plant origins,<br />

breaks down<br />

– May cause a distinct odor (especially in<br />

secondary clays)<br />

• Slight expansion up to 1%<br />

– Not a problem during firing because body is still<br />

porous and somewhat resilient


Burning out<br />

• Carbon, Iron sulphide and Fluorine burn out<br />

– Combine with oxygen to form monoxide, dioxide and trioxide<br />

gases (CO, CO 2 , SO, SO 2 , SO 3 etc.)<br />

• Can lead to blistering and discoloration if fired too<br />

quickly<br />

• Starting point varies substantially with clay type<br />

– Carbon between 650-850 °C (1202-1652 °F)<br />

– Sulphur up to 1150 °C (2102 °F)<br />

• Remedies to bloating<br />

– Thoroughly mix the body<br />

– Slow down the firing – especially when once firing<br />

– Use a less dense body / add filler which allows gas to escape


Metakaolin formation<br />

• Occurs at about 550 °C (1022 °F)<br />

• Chemically bound water (crystal edge water +<br />

water of constitution) leaves the kaolinite crystal<br />

6(Al 2 O 3 • 2SiO 2 • 2H 2 O) 3(2Al 2 O 3 •4SiO 2 )+12H 2 O<br />

kaolinite metakaolinite water<br />

• Kaolin changes into metakaolin (very important)<br />

– Resulting in slight shrinkage<br />

– Very high porosity<br />

– 13.95% weight loss due to water<br />

– Plasticity is lost (a.k.a. “ceramic change”)


• Temperature range varies<br />

– Occurs after the formation<br />

of metakaolin and before<br />

glass formation begins<br />

• Particle are barely held<br />

together<br />

– Not fused but barely<br />

welded at very fine points<br />

of contact<br />

• Overall structure remains<br />

very open<br />

– Very little overall strength<br />

• This is what happens<br />

when we do a low bisque<br />

for glazing<br />

Sintering


Vitrification<br />

• Begins at around 800 °C (1472 °F)<br />

– Composition dependent<br />

– Particle size dependent<br />

• Soda and potash start to flux the quartz<br />

– Glass formation begins<br />

– Quartz grains convert to glass on outer<br />

edges and progress inwards as heat-work<br />

increases<br />

• Shrinkage increases<br />

– Pore volume decreases (voids collapse)<br />

– Density/strength increases


Spinel formation<br />

• Forms around 980 °C (1800 °F)<br />

• Metakaolin layers condense and re-crystallize,<br />

forming spinel crystals<br />

3(2Al 2 O 3 •4SiO 2 ) 3(2Al 2 O 3 •3SiO 2 )+ 3SiO 2<br />

metakaolinite spinel phase free silica<br />

• Silica is released from metakaolinite and<br />

contributes to glass formation


Mullite formation<br />

• Begins above 980 °C (1798 °F)<br />

– Really starts to grow past C. 6<br />

(1200 °C or 2194 °F)<br />

• Alumina from clay and feldspar<br />

dissolves into surrounding glass;<br />

When glass is saturated with<br />

alumina, extra alumina crystallizes<br />

into mullite<br />

• More free silica is also released; more glass is formed<br />

3(2Al 2 O 3 •3SiO 2 ) 2(3Al 2 O 3 •2SiO 2 )+ 5SiO 2<br />

spinel phase mullite free silica


Firing changes


Commercial porcelain after<br />

polishing and etching<br />

Pores<br />

Quartz<br />

Quartz<br />

Primary<br />

Mullite<br />

Secondary<br />

Mullite<br />

10 m


Mineralogical<br />

changes in a<br />

40% kaolinite<br />

30% quartz<br />

30% feldspar<br />

body


Cooling down<br />

• Top temperature down to 573 °C (1063 °F )<br />

– Contraction rate is gradual down to quartz inversion<br />

• At 573 °C<br />

– 1% contraction as beta quartz reverts back to alpha<br />

quartz<br />

• 573 °C - 500 °C (1063-932°F )<br />

– Glazes solidify<br />

• 226 °C (439 °F)<br />

– 3% contraction as cristobalite reverts from beta to alpha<br />

form<br />

– Paper burns at 451 °F


My bisque cycle<br />

Temp °F Rate/hr Hold<br />

0-190 100 Varies (overnight)<br />

190-950 150 -<br />

950-1200 100 -<br />

1200-1940 150 -<br />

1940-2079 100 -<br />

-Suitable for my body (heavily grogged;1/2” walls)<br />

This cycle could easily be sped up for thinner work


Bisque cycle<br />

2500<br />

Final<br />

Soaking<br />

2000<br />

2140 ºF<br />

Temp. (F)<br />

1500<br />

1000<br />

Ceramic<br />

change<br />

500<br />

Steam<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17<br />

Time (hrs.)


Cooling cycle<br />

2500<br />

2000<br />

1500<br />

1000<br />

Quartz<br />

500<br />

0<br />

Cristobalite<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15


Complete cycle<br />

2500<br />

2000<br />

1500<br />

1000<br />

500<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32


Re-firing schedule<br />

(I.e. Glaze schedule)<br />

• Differs from bisque firing because body is<br />

now less elastic (it is more dense)<br />

• Unlike bisque firing, cristobalite and quartz<br />

inversions need to be considered during<br />

heat-up<br />

– Especially true for large/thick work<br />

• Also generally no need for soaking at the<br />

start unless piece is damp from glazing


Glaze cycle<br />

2500<br />

2000<br />

1500<br />

1000<br />

Quartz<br />

500<br />

0<br />

Cristobalite<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14


Heat transfer during firing (in chronological order)<br />

1- Convection heat<br />

• Air is heated as it passes by the element; hot air rises, cool air sinks; air<br />

currents are created; air currents distribute heat<br />

– Not a very even source of heat (especially at lower temperatures)<br />

2- Conduction heat<br />

• Heat is transferred through direct contact<br />

– The main way to get even heating in a kiln<br />

– Outside wall of a piece heats the inside of the piece (or kiln shelf heats bottom<br />

of piece, which, in turn, heats middle and top of piece)<br />

– Requires time, especially with thicker work<br />

3- Radiant heat<br />

• Heat is transferred from hot to cold areas through radiation<br />

• Requires line of sight (like the rays of the sun)<br />

– something in the shadow of the heat source will not heat up as efficiently<br />

• Objects that heat up, in turn, become sources of radiant heat (I.e. elements,<br />

shelves, and the work itself)<br />

• Pieces that are too close to elements can result in scorching due to too much<br />

radiant heat


Thermal gradient of work during firing<br />

• Outside of work always heats up before the inside<br />

– Analogous to a moisture gradient during drying


• Thermal gradient effect leads to differential<br />

expansion/contraction through the walls of a piece


Thermal gradients<br />

• Very problematic from top to bottom of pieces and<br />

possibly from side to side<br />

– Especially in large pieces<br />

– Can happen both in heating and in cooling<br />

• Why<br />

– Hotter part of the piece goes through quartz/cristobalite<br />

inversion before cooler part<br />

• Stress develops, possibly leading to dunting (firing<br />

cracks)<br />

• Solution<br />

E v e n h e a t i n g


Even heating<br />

• Thermal gradients can be minimized<br />

– Slow down firing rate<br />

– Distribute load in kiln evenly (tall and short<br />

pieces on each shelf) and don’t pack too tightly<br />

• Visualize airflow (Convection heating)<br />

• Visualize mass (Conduction heating)<br />

– Elevate your work off kiln shelves<br />

» Kiln shelves store heat (last to heat up, last to cool)<br />

» Elevate the work using stilts, rolled up balls, soft brick or<br />

other low mass materials<br />

• Visualize lines of sight (Radiant heating)<br />

– Use kilns with multiple pyrometers<br />

• Large electric kilns fire more evenly top to bottom<br />

than medium electrics because of this feature


Stilts<br />

• NOT suitable<br />

for high firing


Stilts<br />

• Metal tipped stilts can bend under too much<br />

weight/temperature – for heavier work and hotter<br />

temperatures, use alumina stilts (what we sell) or<br />

make your own


• Ball-shaped stilts help<br />

minimize heat transfer<br />

and allow work to<br />

expand and contract


Using bars instead of shelves…


• Firing to a hot bisque, and then glazing at lower<br />

temps allows the work to be strategically<br />

supported throughout its shrinkage/slumping<br />

• Work will not shrink further during glaze


Cones / Heat-work<br />

• Temperature is not heat<br />

• Heat, or ‘heat-work’, is a measure of time<br />

and temperature<br />

– We know this through experience<br />

I.e. Cheese on a pizza will not instantly melt<br />

when placed in a warm oven-it will take some<br />

time<br />

• Pyrometers measure temperature<br />

• Cones measure heat-work<br />

– They are sensitive to the firing rate (time) and<br />

final temperature


• Cones are rated for<br />

specific temperatures<br />

at specific firing rates


By setting the base of<br />

the cone on a flat<br />

surface it will lean at an<br />

8° angle. Release it and<br />

it will fall on the<br />

"bending face.“ Use this<br />

to predict where cones<br />

will fall in the firing


Weird reactions<br />

• Can be caused by airflow, or by close proximity to<br />

heat source<br />

– Keep cones away from a flame’s path, elements, and<br />

spy-holes


• Sometimes higher cones bend before lower<br />

ones<br />

– Due to effect of drafts (stalling)<br />

– Avoid drafts on the cones during firing<br />

• Don’t place too close to spy-hole<br />

• Don’t blow into kiln during firing


Check out the eyes on this one…


Crashing kilns<br />

• Note: While the proceeding outlines how to<br />

safely crash-cool work, most kilns<br />

(including those at Alfred) are not designed<br />

for this extreme kind of cooling cycle<br />

– Crashing slowly destroys the integrity of the<br />

kiln, and when done carelessly, can melt<br />

controllers on the side of kilns<br />

– Don’t crash unless you absolutely have to;<br />

think before you act; if you’re not sure, ask!


Re: crashing a kiln<br />

A.K.A.<br />

“dumping heat”<br />

• Correlation between<br />

temperature and color<br />

of the kiln<br />

• Quartz inversion<br />

occurs just below<br />

visible heat<br />

• Our work can be<br />

safely cooled down to<br />

red heat


Safe crashing<br />

• When determining<br />

temperature of ware,<br />

look at the ware, not the<br />

environment<br />

– Color of elements,<br />

bricks, shelves etc. do<br />

not reflect temp. of the<br />

work<br />

• When crashing, extremities cool first<br />

• As edges of the work darken, they are approaching<br />

inversion<br />

• Don’t go past this point!<br />

• Close up the kiln and allow heat to redistribute<br />

• Repeat until work is dark red, then cool normally through quartz<br />

inversion


Safe crashing<br />

• When work has dropped below quartz<br />

inversion kiln can be slightly opened<br />

• Cold air drafts must be kept to a minimum,<br />

as they can upset equal cooling throughout<br />

the piece (especially at lower temps.)<br />

• Close the door well before reaching<br />

cristobalite inversion (439 °F)<br />

• How can you tell if you are safely past<br />

cristobalite


• Paper burns at 451 °F<br />

• Stick paper in the spy-hole; if it even starts to curl or change<br />

color, chances are good that you are too close to 439 °F (i.e.<br />

still too hot to open)


A baffle helps shield the work from drafts during crash cooling


Happy Crashing!


Next week...


Field Trip Next Week!<br />

• Meet next Wednesday outside the<br />

back loading dock of Binns<br />

– We leave at 7 am sharp!<br />

– We will be back by 1 pm<br />

• Bring<br />

– Closed shoes<br />

– A lunch<br />

– A camera


References<br />

Ceramics for the Artist Potter<br />

F. H. Norton<br />

Addison-Wesley Publishing Company, Inc., Reading, MA<br />

1956<br />

Ceramic Science for the Potter<br />

W. G. Lawrence<br />

Chilton Book Company, Radnor, Philadelphia<br />

Second Edition, 1982<br />

<strong>Clay</strong>s and Ceramic Raw Materials<br />

by W.E. Worrall<br />

Elsevier Applied Science Publishers, London and New York<br />

Second Edition, 1986<br />

Cushing’s Handbook<br />

by Val Cushing<br />

Third Edition, 1994


References<br />

Elements of Ceramics<br />

by F. H. Norton<br />

Addison-Wesley Press, Inc., Cambridge, MA<br />

1952<br />

Fine Ceramics: Technology and Applications<br />

by F.H. Norton<br />

Robert E. Krieger Publishing Company, Malabar, Florida<br />

1978<br />

Glass Phase Composition in Porcelains and Correlation with Pyroplastic Deformation<br />

by William Carty<br />

Presentation for the 104 th Annual Meeting of the American Ceramic Society<br />

2002<br />

Pottery Science: materials, processes, and products<br />

by Allen Dinsdale<br />

Ellis Horwood Limited, Chichester, England<br />

1986


References<br />

Structural <strong>Clay</strong> Products<br />

by W.E. Brownell<br />

Springer-Verlag, Wien and New York<br />

1976<br />

The Potter’s Dictionary of Materials and Techniques<br />

by Frank and Janet Hamer<br />

A&C Black Publishers Ltd., London, England<br />

Third Edition, 1993<br />

WWW.ORTON.COM<br />

Knowledge library<br />

2003

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