Experimental and Numerical Study of Swirling ... - Solid Mechanics
Experimental and Numerical Study of Swirling ... - Solid Mechanics
Experimental and Numerical Study of Swirling ... - Solid Mechanics
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<strong>Experimental</strong> <strong>and</strong> <strong>Numerical</strong> <strong>Study</strong> <strong>of</strong> <strong>Swirling</strong> Flow in Scavenging Process for 2-Stroke<br />
Marine Diesel Engines<br />
Table 4.2:<br />
Radial Position <strong>of</strong><br />
Measuring points along<br />
X-axis for LDA<br />
measurements.<br />
4.1 LDA Measurements (Inlet Section)<br />
Chapter 4<br />
Two components LDA measurements were conducted at different locations<br />
in the swirl generator as described in Section (3.6). The main reason for<br />
using LDA technique has been the possibility <strong>of</strong> conducting measurements<br />
at locations where PIV measurement becomes very difficult to be conducted<br />
due to guide vanes blocking the laser light (see section 3.1). The<br />
measurements are conducted at volume flow rate <strong>of</strong> 0.154 m 3 /s.<br />
Different radial positions from origin see figure 3.18, between inlet to swirl<br />
generator <strong>and</strong> contraction section, are selected <strong>and</strong> then measurements are<br />
conducted at same radial positions along each <strong>of</strong> the axes lines (Table 4.2).<br />
Axis<br />
Radial Positions from origin (mm)<br />
275 230 215 200 185<br />
X <br />
-X <br />
This must be mentioned here that in the real swirl generator the assumed<br />
axes lines, while crossing the blade row, do not lie on similar location<br />
between the two adjacent guide vanes e.g. the measurement at the radial<br />
position <strong>of</strong> 235 mm for negative Y axis is not possible due to the laser beam<br />
being blocked by a guide vane whereas for other axes measurements can be<br />
conducted at the same radial position.<br />
The measured radial velocity pr<strong>of</strong>iles for each half axis are shown in figure<br />
4.1a (flow direction is from radial position at 275 mm to 180 mm). The halflength<br />
<strong>of</strong> each error bar is one st<strong>and</strong>ard deviation. It can be seen that the<br />
radial velocity distribution is not symmetric. Flow accelerates while passing<br />
through the row <strong>of</strong> guide vanes <strong>and</strong> further downstream due to the<br />
contraction section. Due to wake behind the guide vanes a decrease in the<br />
magnitude is also observed for radial positions <strong>of</strong> 200 mm along positive X.<br />
The tangential velocity pr<strong>of</strong>iles are shown in figure 4.1b. For both half axes,<br />
at radial position <strong>of</strong> 275 mm, a non-zero tangential velocity is observed<br />
which demonstrates either the flow feeling the presence <strong>of</strong> the guide vane<br />
being at downstream position or the blade edge facing the inlet section<br />
outlet is not perfectly aligned with the radius. Moreover, different values <strong>of</strong><br />
tangential velocity <strong>and</strong> angle between radial <strong>and</strong> tangential velocity<br />
components along the axis lines indicate that there exists a small relative<br />
difference in alignment <strong>of</strong> guide vanes (Figure 4.1c).<br />
49<br />
<strong>Swirling</strong> Flow in a Pipe