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The significance of coherent flow structures for the turbulent mixing ...

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2.2 Generation <strong>of</strong> appropriate tracer-particles<br />

Air<br />

Liquid<br />

Air<br />

Liquid<br />

Air<br />

Liquid<br />

Feedholering<br />

Impactorring<br />

FIGURE 2.3: Principal side and top view <strong>of</strong> three utilised atomiser nozzles with different mechanisms<br />

<strong>for</strong> particle generation. From left to right: reference nozzle, Laskin nozzle and suction nozzle with<br />

impactor ring.<br />

‰ ‰ ‰ Š Š Š Š ‹ ‹ Œ Œ<br />

‰<br />

13320-1, see [34]. This is possible <strong>for</strong> spherical particles with known optical properties, when<br />

<strong>the</strong> particle concentration within <strong>the</strong> measurement domain is sufficiently low such that multiple<br />

scattering and optical interference between <strong>the</strong> scattered radiation from different particles can<br />

be neglected. O<strong>the</strong>rwise <strong>the</strong> measurements would be biased, as <strong>the</strong> diffraction pattern <strong>of</strong><br />

a particle ensemble is no longer identical to <strong>the</strong> superposition <strong>of</strong> <strong>the</strong> individual scattering<br />

patterns <strong>of</strong> all particles present.<br />

2.2.2 Particle size analysis<br />

To ensure controlled boundary conditions be<strong>for</strong>e starting <strong>the</strong> experiment, each nozzle was<br />

cleaned and <strong>the</strong> symmetry <strong>of</strong> <strong>the</strong> emerging jets was analysed, as any asymmetry would indicate<br />

damages at <strong>the</strong> nozzle exit due to deposition <strong>of</strong> old oil or burr, <strong>for</strong> example. In addition,<br />

all particles produced during <strong>the</strong> adjustment <strong>of</strong> <strong>the</strong> desired pressure level were completely<br />

removed from <strong>the</strong> generator and <strong>the</strong> tube leading to <strong>the</strong> optical system. <strong>The</strong> reproducibility<br />

<strong>of</strong> <strong>the</strong> generated particle distribution was finally confirmed by per<strong>for</strong>ming four independent<br />

measurements <strong>for</strong> each set <strong>of</strong> parameters. To exclude<br />

£–¥"!0¥G#./kg/(ms)<br />

<strong>the</strong> influence <strong>of</strong> physical properties <strong>of</strong><br />

<strong>the</strong> liquid to be atomised, only with‡ vegetable kg/m˜ oil and<br />

£¥"!0¥G#.-kg/(ms) with‡ DEHS used <strong>for</strong> all experiments, as both<br />

liquids behave very similarly.<br />

Figure 2.4 reveals <strong>the</strong> volumetric particle size distribution <strong>for</strong> <strong>the</strong> described nozzles <strong>for</strong> two<br />

typical pressure states (0.5 and*bar) and, in addition, <strong>the</strong> distribution generated by means <strong>of</strong> a<br />

smoke generator has been added <strong>for</strong> comparison. First, it can be seen that <strong>the</strong> per<strong>for</strong>mance<br />

andcp£–45(—<br />

<strong>of</strong><br />

<strong>the</strong> smoke generator is quite good with respect to <strong>the</strong> o<strong>the</strong>r atomisers, especially if <strong>the</strong> shape,<br />

bandwidth and upper limit <strong>of</strong> <strong>the</strong> particle size distribution are considered. Un<strong>for</strong>tunately,<br />

andcp£›š^*C#kg/m˜ were<br />

17

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