the coking properties of coal at elevated pressures. - Argonne ...
the coking properties of coal at elevated pressures. - Argonne ... the coking properties of coal at elevated pressures. - Argonne ...
Diminishing C-loss along with pressure rise is related to an increased 0 tration , whereas diminishing C-loss along with rising temperature is attr?b%?:i higher reaction velocity. Increasing fluidizing velocities reduce the residence time of the coal in the reactor and, thus, cause higher C-losses. If one found a means of extending this residence time -- be it by appropriate plant design or/and b coal preparation -- the specific heat release rate could be improved proportionate& to the fluidizing velocity. A longer residence time of the coal by means of increased bed height will diminish C-losses , too. C-loss may be influenced also by coal preparation measures. As shown on figure 3, the C-loss will, when fueling closely sized coal fractions, pass through a maximum as soon as the particle diameter approches the elutriation cut point. Coarse coal grains will remain in the bed up to the moment where they are burnt down to a size allowing their elutriution or preventing them from being recycled by the inertial separators. With sufficiently small fractions (coal dust) the reaction time is apparently shorter than the residence time in the reactor space so that the coal particles are almost completely burnt up. As far as industrial plants are concerned, the logical conclusion from this is to separate coal dust &om the coarser fractions and blow the dust pneumatically into the fluidized bed from below, in order to allow a maximum residence time of the dust and avoid erosion in the feed ducts, whereas the coarse fractions, being introduced from above, are allowed sufficient time to spread over the bed while being burnt up. In this case it can be taken from the diagrams, e.g. figure 3, where the preparation cut points for each specific plant are viz . which granular fraction should be separated and lor further comminuted. Examination of the carbon carry-over by means of screening for its size distribution does not yield accurate results since char aggregations will disintegrate. The results of figure 3 are, however, reconfirmed by this approximative evaluation. Moreover it can be verified from fly ash separation in two subsequent cyclones that the fine dust from the second cyclone is very low in carbon, whereas the "coarse dust" of the first one will always contain the bulk of the unburnt carbon. Apart from the determinable and adjustable operational parameters, C-loss is also a function of the specific plant parameters. Measuring data can best be reproduced in laboratory equipment. When doing so, one observes other and so far not measurable operational conditions which bear on the results. Among these have to be considered the size distribution of the fluidized bed ash particles which changes during opera- tion, or changing fluidity and cohesive properties of the bed ash when adding various gradations of limestone. A comparison of the C-loss measured in reactor no. 1 with that of the semi-technical Plant V (figure 5) -- the cross-section of the free-board has been enlarged in both units -- shows good coincidence. It should be borne in mind, however, that here varying particle gradations and bed heights compensate each other in a way not clearly identified so far. As was expected, there are differences also in the C-losses for the different laboratory reactor types since inertial separators are not optimized. This is not disturbing as long as feed materials, viz. types of limestone and coal, are compared by measurements in one reactor only. As soon as it comes to scaling up results, however, one has to know about the reasons and influences of specific operational conditions. 220
i \ ' 2.2. soz Emission and NOx Emission Statements on the pressure-dependences of SO and NO emissions (figure 2) are so far based on measurements of two pressure levels (13 and 4.5 bar). When moving to the higher pressure SO2 and NO emissions will be diminished by more than 50 %. The qualitative evaluations of ea%y orientation tests on the new pressure apparatus IV where measurements at several pressures between 1 and 10 bar are to be carried out, do reconfirm this improvement. Fi re 10 shows the stroig dependence of SO emissions on the size of the limestone *wed Ca/S ratio). It is, however, strhing and so far not explainable (figure 5) that varying sizes of one same type of limestone lead to different temperature dependencies. Dolomite shows a similar behaviour (figure 6). When adding coarse material, SO emission will slump with rising temperatures, whereas the opposite happens wgen material of small grain sizes is added. Excess air (figure 7) has a weak influence on SO2 emission, while its effect on NOx emission is strong since in this case the oxygen concentration is decisive for the conversion of that proportion of fuel-nitrogen which is transformed to NO. (Due to the low temperatures in a fluidized bed plant, 10 to 30 % only of the fuel-nitrogen and no nitrogen from the air is converted to NO.) A lack of O2 favours rather the competing reaction which yields molecular N2. The dependencies of SO and NO emissions are mostly active in opposite directions (figure 2). A good insigit into tze conditions leading to NO formation is possible with the secondary air reactor. When plotting the NOx emission against different incremental primary airlsecondary air ratios, a NO mmimum is met at a distribution of primary versus secondary air of 50 : 50. This &fect was most obvious in reactor no. 1 (4), whereas it was less pronounced in the bigger reactor no. 111 where, at the same time, the maximum emission values were reduced. The lowest values were abserved in the semi-technical reactor (figure 8); they were in the same order of magnitude which prevails also in other larger plants. From this may be concluded that the NO emissions measured in the laboratory reactors are atypically high. The formation of coarse bubbles in big reactors bring about a certain distribution of O2 as high as into the upper bed zones. Such by-pass effect can be compared with the feed of secondary air. Consequently, the way how oxygen acts on the coal and, possibly, the removal of reducing volatile coal components are main determinants for NO emission. Emissions from the semi-technical plant may be considered typicalXfor NO emissions from full-scale plants (figure 8), with 1 g NOZ/kWh being approxizately equivalent to 200 ppm NO. So, even though the numerical values obtained from laboratory measurements are exaggerated in respect of their absolute value and do not allow any generalization as to NOx emissions, one may nonetheless derive certain tendencies (e.g. dependence on excess air) which can be scaled-up to bigger plants. Typical figures for SO emissions cannot be identified since the main influential 2 factor on SO emission will be the amount of limestone added. SO emission, there- 2 fore, is only to a small extent typical for a given plant. Fi re 3 shows a dependence on the limestone/sulphur mole ratio when feeding di erent coals high in ash and with varying sulphur contents, but adding one same limestone at pressures of 1.1 and 4.5 bar. It is the spontaneous desulphurization of coals rather than their sulphur content which brings about the difference in SO emissions, -- emissions which on a laboratory scsle can be reduced to zero. To And out the limestone with optimum sulphur capturing efficiency (i .e. accomplishing the desired desulphurization with admixture of the possible minimum sorbent amount), some three dozens of limestomes of different geological formations, deposits, and trade marks were tested (5). Geologically young and porous limestones appear to be best suited. 221
- Page 169 and 170: E 6 i i h \ 1 1 \ on the XRF is cau
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i<br />
\<br />
'<br />
2.2. soz Emission and NOx Emission<br />
St<strong>at</strong>ements on <strong>the</strong> pressure-dependences <strong>of</strong> SO and NO emissions (figure 2) are<br />
so far based on measurements <strong>of</strong> two pressure levels (13 and 4.5 bar). When<br />
moving to <strong>the</strong> higher pressure SO2 and NO emissions will be diminished by more<br />
than 50 %. The qualit<strong>at</strong>ive evalu<strong>at</strong>ions <strong>of</strong> ea%y orient<strong>at</strong>ion tests on <strong>the</strong> new pressure<br />
appar<strong>at</strong>us IV where measurements <strong>at</strong> several <strong>pressures</strong> between 1 and 10 bar are<br />
to be carried out, do reconfirm this improvement.<br />
Fi re 10 shows <strong>the</strong> stroig dependence <strong>of</strong> SO emissions on <strong>the</strong> size <strong>of</strong> <strong>the</strong> limestone<br />
*wed Ca/S r<strong>at</strong>io). It is, however, strhing and so far not explainable<br />
(figure 5) th<strong>at</strong> varying sizes <strong>of</strong> one same type <strong>of</strong> limestone lead to different temper<strong>at</strong>ure<br />
dependencies. Dolomite shows a similar behaviour (figure 6). When adding<br />
coarse m<strong>at</strong>erial, SO emission will slump with rising temper<strong>at</strong>ures, whereas <strong>the</strong><br />
opposite happens wgen m<strong>at</strong>erial <strong>of</strong> small grain sizes is added.<br />
Excess air (figure 7) has a weak influence on SO2 emission, while its effect on<br />
NOx emission is strong since in this case <strong>the</strong> oxygen concentr<strong>at</strong>ion is decisive for<br />
<strong>the</strong> conversion <strong>of</strong> th<strong>at</strong> proportion <strong>of</strong> fuel-nitrogen which is transformed to NO. (Due<br />
to <strong>the</strong> low temper<strong>at</strong>ures in a fluidized bed plant, 10 to 30 % only <strong>of</strong> <strong>the</strong> fuel-nitrogen<br />
and no nitrogen from <strong>the</strong> air is converted to NO.) A lack <strong>of</strong> O2 favours ra<strong>the</strong>r <strong>the</strong><br />
competing reaction which yields molecular N2.<br />
The dependencies <strong>of</strong> SO and NO emissions are mostly active in opposite directions<br />
(figure 2). A good insigit into tze conditions leading to NO form<strong>at</strong>ion is possible<br />
with <strong>the</strong> secondary air reactor. When plotting <strong>the</strong> NOx emission against different<br />
incremental primary airlsecondary air r<strong>at</strong>ios, a NO mmimum is met <strong>at</strong> a distribution<br />
<strong>of</strong> primary versus secondary air <strong>of</strong> 50 : 50. This &fect was most obvious in reactor<br />
no. 1 (4), whereas it was less pronounced in <strong>the</strong> bigger reactor no. 111 where, <strong>at</strong><br />
<strong>the</strong> same time, <strong>the</strong> maximum emission values were reduced. The lowest values were<br />
abserved in <strong>the</strong> semi-technical reactor (figure 8); <strong>the</strong>y were in <strong>the</strong> same order <strong>of</strong><br />
magnitude which prevails also in o<strong>the</strong>r larger plants. From this may be concluded<br />
th<strong>at</strong> <strong>the</strong> NO emissions measured in <strong>the</strong> labor<strong>at</strong>ory reactors are <strong>at</strong>ypically high. The<br />
form<strong>at</strong>ion <strong>of</strong> coarse bubbles in big reactors bring about a certain distribution <strong>of</strong> O2<br />
as high as into <strong>the</strong> upper bed zones. Such by-pass effect can be compared with <strong>the</strong><br />
feed <strong>of</strong> secondary air. Consequently, <strong>the</strong> way how oxygen acts on <strong>the</strong> <strong>coal</strong> and,<br />
possibly, <strong>the</strong> removal <strong>of</strong> reducing vol<strong>at</strong>ile <strong>coal</strong> components are main determinants<br />
for NO emission. Emissions from <strong>the</strong> semi-technical plant may be considered<br />
typicalXfor NO emissions from full-scale plants (figure 8), with 1 g NOZ/kWh<br />
being approxiz<strong>at</strong>ely equivalent to 200 ppm NO. So, even though <strong>the</strong> numerical values<br />
obtained from labor<strong>at</strong>ory measurements are exagger<strong>at</strong>ed in respect <strong>of</strong> <strong>the</strong>ir absolute<br />
value and do not allow any generaliz<strong>at</strong>ion as to NOx emissions, one may none<strong>the</strong>less<br />
derive certain tendencies (e.g. dependence on excess air) which can be scaled-up<br />
to bigger plants.<br />
Typical figures for SO emissions cannot be identified since <strong>the</strong> main influential<br />
2<br />
factor on SO emission will be <strong>the</strong> amount <strong>of</strong> limestone added. SO emission, <strong>the</strong>re-<br />
2<br />
fore, is only to a small extent typical for a given plant. Fi re 3 shows a dependence<br />
on <strong>the</strong> limestone/sulphur mole r<strong>at</strong>io when feeding di erent <strong>coal</strong>s high in ash<br />
and with varying sulphur contents, but adding one same limestone <strong>at</strong> <strong>pressures</strong> <strong>of</strong><br />
1.1 and 4.5 bar. It is <strong>the</strong> spontaneous desulphuriz<strong>at</strong>ion <strong>of</strong> <strong>coal</strong>s ra<strong>the</strong>r than <strong>the</strong>ir<br />
sulphur content which brings about <strong>the</strong> difference in SO emissions, -- emissions<br />
which on a labor<strong>at</strong>ory scsle can be reduced to zero. To And out <strong>the</strong> limestone with<br />
optimum sulphur capturing efficiency (i .e. accomplishing <strong>the</strong> desired desulphuriz<strong>at</strong>ion<br />
with admixture <strong>of</strong> <strong>the</strong> possible minimum sorbent amount), some three dozens <strong>of</strong><br />
limestomes <strong>of</strong> different geological form<strong>at</strong>ions, deposits, and trade marks were tested<br />
(5). Geologically young and porous limestones appear to be best suited.<br />
221