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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4.4. Two-dimensional Evaporating PVP/Water Spray in Air 93<br />
Fig. 4.44: Photograph of the PVP/water spray formation with 112 kg/h liquid inflow<br />
rate in experiment [206].<br />
4.4.1 Experiment and Initial Data Generation<br />
The PVP/water spray in air experiments have been carried out by the group of<br />
Prof. G. Brenn by spraying a solution of 20% PVP and 80% water (by mass) through<br />
the Delavan nozzle SDX-SE-90 at room temperature. The droplet sizes and velocities<br />
are recorded at the cross sections of 0.08, 0.12 and 0.16 m away from nozzle orifice<br />
using PDA, which provides both droplet size and velocity distributions, similar to the<br />
water spray in air measurements. The liquid mass flow rate of these experiments is<br />
112 kg/h and other conditions of the experiment such as gas velocity, gas temperature<br />
and pressure are same as the water spray in air. Figure 4.44 displays the PVP/water<br />
spray formation in experiment [206]. To generate the initial data for simulating the<br />
PVP/water spray in air, the same procedure as outlined in two-dimensional water spray<br />
in air is followed here. Figure 4.45 shows the experimental droplet size distribution<br />
and the corresponding DQMOM approximation at the radial position 0.036 m from<br />
the spray axis and 0.08 m downstream of the nozzle orifice.<br />
4.4.2 Results and Discussion<br />
PVP/water spray flow in air is modeled using the DQMOM where the bi-component<br />
droplet evaporation of PVP/water droplets [172, 225, 226] are accounted through the<br />
single droplet evaporation and solid formation model presented in Chapter 2 and the<br />
results are discussed in Subsection 4.3.3. For droplet motion, droplet coalescence, the