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INAUGURAL–DISSERTATION zur Erlangung der Doktorwürde der ...

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62 4. Results and Discussion<br />

3<br />

3<br />

Veloctiy [m/s]<br />

2.5<br />

2<br />

1.5<br />

1<br />

u[1] = 1.09 m/s, r[1] = 24 µm<br />

u[2] = 1.94 m/s, r[2] = 86 µm<br />

u[3] = 2.76 m/s, r[3] = 143 µm<br />

Velocity [m/s]<br />

2.5<br />

2<br />

1.5<br />

1<br />

u[1] = 1.09 m/s, r[1] = 24 µm<br />

u[2] = 1.94 m/s, r[2] = 86 µm<br />

u[3] = 2.76 m/s, r[3] = 143 µm<br />

0.5<br />

0.5<br />

0<br />

0 0.2 0.4 0.6 0.8 1<br />

Time [s]<br />

0<br />

0 1 2 3 4 5<br />

Time [s]<br />

Fig. 4.8: Velocity profiles of three droplets with different initial radii and velocities<br />

un<strong>der</strong> the influence of drag alone (left) and drag and gravity (right).<br />

follow the streamlines of the gas after reaching a steady value, cf. left side of Fig. 4.8.<br />

On the other hand, when the droplets encounter gravity in addition to drag force applied<br />

by the surrounding gas, the droplet velocity initially decreases due to drag and<br />

then increases linearly due to gravity as seen in right part of Fig. 4.8. In a previous<br />

study [198, 200], it has been shown that the mo<strong>der</strong>ate droplet evaporation un<strong>der</strong> the<br />

present conditions does not significantly influence droplet velocity.<br />

140<br />

130<br />

Experiment - 80 kg/h<br />

Evaporation - 80 kg/h<br />

Evaporation and Coalescence - 80 kg/h<br />

Experiment - 150 kg/h<br />

Evaporation - 150 kg/h<br />

Evaporation and Coalescence - 150 kg/h<br />

Sauter mean diameter [µm]<br />

120<br />

110<br />

100<br />

90<br />

80<br />

70<br />

0.14 0.28 0.42 0.56 0.7 0.84<br />

Position [m]<br />

Fig. 4.9: Effect of liquid inflow rates on Sauter mean diameter computed with and<br />

without coalescence.

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