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On the Formation of Nitrogen Oxides During the Combustion of ...

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5.2 <strong>Combustion</strong> <strong>of</strong> Partially Pre-Vaporized Droplets<br />

tracted. The amount <strong>of</strong> fuel referred to is ei<strong>the</strong>r <strong>the</strong> reacting fuel mass, that is<br />

consumed until simulation end (Eq. (4.46)), or <strong>the</strong> initial mass <strong>of</strong> <strong>the</strong> droplet.<br />

In general, NO x emissions are almost constant for Ψ< 0.5. This tendency suggests<br />

that combustion behavior is similar in this range. As <strong>the</strong> radial pr<strong>of</strong>ile<br />

<strong>of</strong> <strong>the</strong> fuel mass fraction Y C10 H 22<br />

(r ) is steep in <strong>the</strong> gas phase, <strong>the</strong> amount <strong>of</strong><br />

flammable, premixed gas is low. Most <strong>of</strong> <strong>the</strong> pre-vaporized fuel is oxidized<br />

in a diffusion flame. However, at large degrees <strong>of</strong> pre-vaporization (Ψ> 0.5),<br />

<strong>the</strong> amount <strong>of</strong> fuel under flammable, partially premixed conditions increases.<br />

Immediately after ignition, <strong>the</strong> flame type tends more and more towards a premixed<br />

flame. The NO x emissions decrease. Besides those effects due to fuel<br />

premixing and pre-vaporization, <strong>the</strong> temporal and spatial scales are important<br />

in terms <strong>of</strong> NO x formation, as well. Their impact is discussed in detail in<br />

<strong>the</strong> context <strong>of</strong> <strong>the</strong> verification <strong>of</strong> <strong>the</strong> ignition position (Chap. 5.2.2).<br />

As can be seen in Figure 5.3, it is not relevant to distinguish between <strong>the</strong> two<br />

fuel masses referred to within one and <strong>the</strong> same ignition method, as long as<br />

<strong>the</strong> pre-vaporization rate is low (Ψ< 0.5). However, this becomes important<br />

for larger values <strong>of</strong> Ψ. Comparing <strong>the</strong> two referencing methods, <strong>the</strong> emission<br />

index EI NOx generally decreases with an increase in Ψ, which is due to an overall<br />

decreasing NO x production. Still, it decreases at a slower rate, when referring<br />

to <strong>the</strong> reacting fuel mass instead <strong>of</strong> to <strong>the</strong> initial droplet mass. This trend<br />

is not an indicator <strong>of</strong> insufficient convergence. Vaporized fuel simply diffuses<br />

outwards in <strong>the</strong> radial direction. Thus, with an increase <strong>of</strong> Ψ, more gaseous<br />

fuel is shifted towards regions with an equivalence ratio remaining below <strong>the</strong><br />

lower flammability limit. This fuel is lost as far as <strong>the</strong> spherical droplet flame<br />

is concerned. However, given an appropriate design <strong>of</strong> <strong>the</strong> combustion zones<br />

within a technical application, it can be consumed in <strong>the</strong> subsequent combustion<br />

zone at a lower partial pressure <strong>of</strong> oxygen, resulting in a significant<br />

overall NO x reduction.<br />

5.2.2 Impact <strong>of</strong> Ignition Position<br />

Generally, heat introduction to initiate ignition is conducted within a region<br />

spanned by <strong>the</strong> flammability limits and <strong>the</strong>ir outer proximities, taking a wide<br />

variation <strong>of</strong> droplet pre-vaporization Ψ as a basis. Two feasible approaches are<br />

outlined in <strong>the</strong> related model description <strong>of</strong> Chapter 4.3. The first approach<br />

163

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