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the coking properties of coal at elevated pressures. - Argonne ...

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I<br />

Coal Ash Sintering Model and <strong>the</strong> R<strong>at</strong>e Measurements<br />

E. Raask<br />

Central Electricity Research Labor<strong>at</strong>ories<br />

Kelvin Avenue<br />

Lea<strong>the</strong>rhead, Surrey, UK<br />

INTRODUCTION<br />

In spite <strong>of</strong> innumerable labor<strong>at</strong>ory investig<strong>at</strong>ions and <strong>the</strong> wealth <strong>of</strong> practical<br />

experience, <strong>the</strong>re remains some enigm<strong>at</strong>ic facets in <strong>the</strong> form<strong>at</strong>ion <strong>of</strong> sintered ash and<br />

slag deposit on he<strong>at</strong> exchange surfaces in <strong>coal</strong>-fired boilers. Th<strong>at</strong> is, occurrences<br />

<strong>of</strong> massive build-up <strong>of</strong> ash deposits can take boiler design and oper<strong>at</strong>ion engineers<br />

by surprise. This would suggest th<strong>at</strong> <strong>the</strong> engineers are receiving incomplete or<br />

incorrect inform<strong>at</strong>ion on <strong>the</strong> deposit-forming propensity <strong>of</strong> ash in different <strong>coal</strong>s.<br />

Traditional methods <strong>of</strong> assessing <strong>the</strong> behavior <strong>of</strong> deposit-forming impurities in<br />

high temper<strong>at</strong>ure boiler plants are based on ash fusion tests as described in different<br />

n<strong>at</strong>ional standards for <strong>coal</strong> analysis and testing, e.g., ASTM (1968), British Standard<br />

(1970), DIN (1976) and Norme Francaise (1945). These ash fusion tests have been<br />

developed from refractory m<strong>at</strong>erial technology, and are based on observ<strong>at</strong>ions <strong>of</strong> <strong>the</strong><br />

change in shape and size <strong>of</strong> an ash sample on he<strong>at</strong>ing. It has been realized th<strong>at</strong> <strong>the</strong><br />

results <strong>of</strong> ash fusion tests are frequently imprecise, and can lead to a mistaken<br />

assessment <strong>of</strong> <strong>the</strong> likely severity <strong>of</strong> boiler fouling and slagging.<br />

There has been a number <strong>of</strong> suggestions made for ash fouling and slagging indices<br />

to predict more accur<strong>at</strong>ely <strong>the</strong> r<strong>at</strong>e <strong>of</strong> deposit build-up with different <strong>coal</strong>s as<br />

reviewed by Winegartner (1974). The empirical formulae, e.g., silica r<strong>at</strong>io, basic<br />

to acidic oxide r<strong>at</strong>io, and sodium and sulphur contents <strong>of</strong> <strong>coal</strong>, are based on <strong>the</strong><br />

chemical analysis and have a limit<strong>at</strong>ion th<strong>at</strong> <strong>the</strong>y apply to particular <strong>coal</strong>s. Th<strong>at</strong> is,<br />

<strong>the</strong>re is no universal formula <strong>of</strong> predicting <strong>the</strong> severity <strong>of</strong> boiler fouling based on<br />

ash fusion tests and chemical analysis with all types <strong>of</strong> <strong>coal</strong>.<br />

It is <strong>the</strong>refore evident th<strong>at</strong> fur<strong>the</strong>r research is necessary on <strong>the</strong> mechanism <strong>of</strong><br />

ash particle-to-particle bonding <strong>at</strong> high temper<strong>at</strong>ures. This work sets out to redefine<br />

an ash sintering model in terms <strong>of</strong> measurable parameters, surface tension, viscosity,<br />

electrical conductance, temper<strong>at</strong>ure, particle size and time.<br />

In <strong>the</strong> experimental work,<br />

novel methods <strong>of</strong> measuring <strong>the</strong> r<strong>at</strong>es <strong>of</strong> ash sintering were applied, in order to test<br />

<strong>the</strong> validity <strong>of</strong> <strong>the</strong> sintering model.<br />

SINTERING MODEL<br />

Frenkel (1945) has derived an equ<strong>at</strong>ion rel<strong>at</strong>ing <strong>the</strong> growth <strong>of</strong> <strong>the</strong> interface between<br />

two spherical particles:<br />

where x is <strong>the</strong> radius <strong>of</strong> <strong>the</strong> interface, r is <strong>the</strong> original radius <strong>of</strong> <strong>the</strong> spheres, Y is<br />

<strong>the</strong> surface tension and t is <strong>the</strong> time. Rearranging <strong>the</strong> equ<strong>at</strong>ion in terms <strong>of</strong> x/r and t,<br />

it becomes:<br />

and it is applicable when < 0.3.<br />

145

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