INAUGURAL–DISSERTATION zur Erlangung der Doktorwürde der ...
INAUGURAL–DISSERTATION zur Erlangung der Doktorwürde der ...
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.