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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4.1. One-dimensional Evaporating Water Spray in Nitrogen 63<br />
The variations in Sauter mean diameter with axial position of the spray for two different<br />
liquid inflow rates of 80 kg/h and 150 kg/h are shown in Fig. 4.9. The results for<br />
80 kg/h show an increasing Sauter mean diameter with evaporation. Inclusion of coalescence<br />
in addition to evaporation leads to excellent agreement between computational<br />
and experimental results. On the contrary, the computational results for 150 kg/h at<br />
x = 0.54 m seem to be deviating far away from the experimental data. The observed<br />
deviation is due to inconsistency in experimental data, which is evident from the fact<br />
that the experimental flow rate does not match the prescribed value of 150 kg/h at<br />
0.54 m. Therefore, the results from 80 kg/h will be discussed for the remaining part of<br />
this section.<br />
Figure 4.10 displays the profiles of the Sauter mean diameter (left) and mean droplet<br />
diameter (right) of water spray subjected to evaporation at 293 K and 313 K temperatures<br />
of surrounding gas as well as with and without coalescence. As expected, Sauter<br />
mean diameter increases substantially with evaporation that causes the decrease and<br />
eventual loss of small size droplets. Higher temperature imposes a rise in evaporation,<br />
which consi<strong>der</strong>ably accelerates the rate of increase of Sauter mean diameter. A comparison<br />
with experimental data reveals the importance of modeling the droplet coalescence,<br />
which not only improves the simulation results but also has excellent agreement with<br />
experiment (see left side of Fig. 4.10).<br />
Similar to Sauter mean diameter, the mean droplet diameter is an important physical<br />
quantity for several applications such as particle size analysis of pow<strong>der</strong> sampling<br />
in food and pharmaceutical industries [201]. Mean droplet diameter of a number density<br />
based distribution can be computed using the Eq. (2.18). Since very small size<br />
160<br />
150<br />
Experiment - 293 K<br />
Evaporation - 293 K<br />
Evaporation and Coalescence - 293 K<br />
Evaporation - 313 K<br />
Evaporation and Coalescence - 313 K<br />
90<br />
85<br />
Experiment - 293 K<br />
Evaporation - 293 K<br />
Evaporation and Coalescence - 293 K<br />
Evaporation - 313 K<br />
Evaporation and Coalescence - 313 K<br />
Sauter mean diameter [µm]<br />
140<br />
130<br />
120<br />
110<br />
D 10<br />
[µm]<br />
80<br />
75<br />
70<br />
65<br />
60<br />
55<br />
100<br />
0.14 0.28 0.42 0.56 0.7 0.84<br />
Position [m]<br />
50<br />
0.14 0.28 0.42 0.56 0.7 0.84<br />
Position [m]<br />
Fig. 4.10: Profiles of Sauter mean diameter (left) and mean droplet diameter (right)<br />
computed with and without coalescence at surrounding gas temperatures of<br />
293 K and 313 K.