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

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5.5 Final Evaluation <strong>of</strong> Results<br />

Second, <strong>the</strong> combustion <strong>of</strong> partially pre-vaporized droplets was studied carrying<br />

out numerical experiments, too. Here, <strong>the</strong> atmosphere was air with an<br />

initial temperature in <strong>the</strong> range <strong>of</strong> 500 to 700 K. As this temperature is too low<br />

for auto-ignition, <strong>the</strong> droplets were ignited using an external energy source<br />

after <strong>the</strong> pre-vaporization time t Ψ was reached. The energy introduced into<br />

<strong>the</strong> numerical domain was methodically re-extracted upon onset <strong>of</strong> reaction<br />

and before temperatures leading to substantial NO x formation were attained.<br />

These numerical simulations yielded an almost constant NO x production up<br />

to a pre-vaporization rate <strong>of</strong> around 50%. If more than half <strong>of</strong> <strong>the</strong> droplet mass<br />

is vaporized before ignition takes place (Ψ> 0.5), lean, partially premixed areas<br />

develop and NO x emissions decrease with an increase in Ψ. <strong>During</strong> <strong>the</strong><br />

period <strong>of</strong> heat introduction, <strong>the</strong> droplet burning behavior is dominated by <strong>the</strong><br />

influence <strong>of</strong> <strong>the</strong> volumetric heat source. Thus, it is crucial to choose energy<br />

and location <strong>of</strong> <strong>the</strong> ignition source in a way that <strong>the</strong> influence on total NO x<br />

generation is negligible. Compared to previous studies, <strong>the</strong> precise supply<br />

and removal <strong>of</strong> energy by a source term turned out to be a beneficial feature to<br />

control ignition. As a result <strong>of</strong> improving <strong>the</strong> ignition method, <strong>the</strong> amount <strong>of</strong><br />

heat introduced can be kept constant from case to case. This generic ignition<br />

procedure is energetically neutral. It allows to study NO x formation without<br />

artificial, <strong>the</strong>rmal effects stemming from ignition. None<strong>the</strong>less, modeling ignition<br />

will remain a general problem in droplet combustion modeling. This<br />

becomes apparent when comparing different ignition approaches.<br />

In summary, <strong>the</strong> overall agreement – in a qualitative manner – between experiments,<br />

numerical simulations, and analytical approximations is very good.<br />

There is also a very good reproducibility within <strong>the</strong> experimental results. The<br />

model, as employed in <strong>the</strong> numerical simulations, is in good agreement with<br />

literature. However, due to <strong>the</strong> different setups <strong>of</strong> spherically symmetric single<br />

droplets and linear droplet arrays, it is hard to develop correlations between<br />

numerical and experimental results. Significant heat losses in <strong>the</strong> experiment<br />

contribute to an absolute deviation in <strong>the</strong> NO x values by a factor <strong>of</strong> 5 to 10.<br />

The strong coupling between droplet ignition and NO x formation highlights<br />

<strong>the</strong> need for a reasonable modeling <strong>of</strong> <strong>the</strong> ignition position for pre-vaporized<br />

droplets. It is not possible to use <strong>the</strong> single droplet model for modeling <strong>the</strong><br />

interaction <strong>of</strong> droplets in sprays.<br />

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