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

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B.1 Experiment Operation Conditions for Droplet Array <strong>Combustion</strong><br />

produces as a link in an infinite droplet array. Never<strong>the</strong>less, gas exchange during<br />

<strong>the</strong> combustion and gas sampling processes needs to be accounted for.<br />

Since <strong>the</strong> sounding rocket flight <strong>of</strong> TEXUS-46 originally comprised only four<br />

combustion cycles, a statistical evaluation <strong>of</strong> <strong>the</strong> procedures for gas sampling<br />

and analysis became indispensable. Fur<strong>the</strong>rmore, diversification <strong>of</strong> <strong>the</strong> experiment<br />

parameters was essential for <strong>the</strong> scientific output. Consequently,<br />

parabolic flight and drop tower experiments were conducted as precursor experiments<br />

to investigate <strong>the</strong> reference case for <strong>the</strong> sounding rocket experiments<br />

as well as to gain additional knowledge about various technical aspects<br />

<strong>of</strong> <strong>the</strong> experiment. 1<br />

As mentioned above, <strong>the</strong> main focus <strong>of</strong> <strong>the</strong> study at hand was <strong>the</strong> degree <strong>of</strong> fuel<br />

vaporization Ψ. The extended microgravity duration <strong>of</strong> sounding rocket flight<br />

allowed to investigate larger values <strong>of</strong> Ψ compared to parabolic flight and<br />

drop tower. However, fur<strong>the</strong>r experiment parameters were studied within <strong>the</strong><br />

drop tower campaign to achieve a more complete understanding <strong>of</strong> droplet<br />

combustion and NO x formation. They included <strong>the</strong> preheating temperature<br />

T ∞ , initial droplet diameter D 0 , inter-droplet distance S, and total droplet<br />

number N. Table B.1 gives an overview <strong>of</strong> all experiments conducted under<br />

microgravity conditions. The reason for investigating such large droplets<br />

(0.840 – 1.608 mm) was to provide large spatial and temporal scales, and thus<br />

well-defined droplet combustion regimes. This approach in particular helped<br />

to restrain <strong>the</strong> relative deviations within fuel vapor formation around <strong>the</strong><br />

droplets. Experimental errors in <strong>the</strong> initial droplet diameter D 0 and/or prevaporization<br />

time t Ψ can be caused by <strong>the</strong> fuel-dosing pump, <strong>the</strong> fine glass<br />

tubes, <strong>the</strong> ignition system, and <strong>the</strong> hysteresis <strong>of</strong> <strong>the</strong> system itself.<br />

Precursor Experiments<br />

Parabolic flight experiments typically provide a microgravity level <strong>of</strong> 1×10 −2 g 0<br />

for approximately 20s. Major advantages <strong>of</strong> parabolic flight are direct access<br />

to <strong>the</strong> experiment by <strong>the</strong> scientist, multiple experiment runs within one<br />

campaign, absence <strong>of</strong> negative impact loads, minor restrictions in weight and<br />

power consumption, and moderate costs. However, <strong>the</strong> aircraft can normally<br />

1 In <strong>the</strong> meantime, Nomura et al. [318] and Oyagi et al. [327] were making efforts to investigate <strong>the</strong> combustion<br />

<strong>of</strong> moving droplets and droplet clusters, which is <strong>the</strong> next step towards <strong>the</strong> systematic investigation <strong>of</strong> complex<br />

sprays.<br />

209

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