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298 94 307/02 Untersuchungen zum Stand der Umsetzung des ...

298 94 307/02 Untersuchungen zum Stand der Umsetzung des ...

298 94 307/02 Untersuchungen zum Stand der Umsetzung des ...

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combustion chamber; the lower boundary is formed by the air diffuser. Swirling air, which<br />

at the same time serves as incineration air, flows through the fluidisation bed mass in an<br />

upward direction. At a certain air velocity, the individual particles of the layer lift from one<br />

another somewhat. Through the air stream and the resultant turbulence, these are placed<br />

into irregular and undirected motion and bump and rub against one another in rapid suc-<br />

cession. During this process, the layer mass is intensively and evenly mixed and in the<br />

process achieves an exchange of material and heat that is characteristic and practically<br />

ideal in terms of the fluidised bed. The heating of the oven takes place through natural gas<br />

or heating oil that is ignited in the swirl chamber by means of start-up burners or heat the<br />

turbulent air in a pre-incineration chamber. After reaching the ignition temperature, addi-<br />

tional fuel can be introduced directly into the hot fluidised bed through lances. The fuel is<br />

introduced directly into the hot fluidisation bed through helixes, where it is liberated<br />

through sudden heating, dried and then comminuted by the turbulent particles. The com-<br />

bustible components are gasified through the intense heat transfer and already largely<br />

burn up in the fluidisation bed. The expansion of the combustion chamber upwards guar-<br />

antees that only tiny small-grained solid matter particles can be discharged. Above the<br />

fluidisation bed, secondary air is injected through nozzles, which ensures that even the<br />

last remaining combustible components are incinerated at a temperature of at least 850<br />

degrees C.<br />

Using animal meal as an example fuel, it can be shown that at an assumed heating<br />

value fluctuation range of 17 to 21 MJ/kg, a thermal load range of approx. 9-12 MW and a<br />

throughput performance of 1.550 to 2.550 kg/h can be attained.<br />

If, in the same fluidisation bed oven on which the incineration performance diagram was<br />

based, raw material is incinerated, a throughput performance of 2.500 – 7.500 kg/h of raw<br />

material and a thermal output of 4,8 – 9,7 MW is attained in this fluidisation bed oven. At a<br />

fixed thermal output, the throughput performance is determined by the heating value of<br />

the fuel, so that the maximum throughput is attained at the lowest fuel heating value of<br />

4MJ/kg, whereas the highest heating value corresponds to the lowest throughput per-<br />

formance.<br />

Achieved environmental benefits<br />

Cross media effects<br />

Operational data Applicability<br />

Economics<br />

Which plant setting represents the most economical and sensible solution is strongly in-<br />

fluenced by local factors (supply volume, transportation routes etc.) In the following table,<br />

only a few important economic criteria are therefore contrasted. A comprehensive plant is<br />

in each case assumed. Location dependent inflow volumes are not taken into account<br />

here. For the purposes of simplification, a raw material volume of 100.000 t/a and a corre-<br />

sponding volume of animal meal of 20.000 t/a is assumed in the following illustration.<br />

Raw material incineration Animal meal incineration<br />

Basis 100.000 t/a raw material 20.000 t/a animal meal

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