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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 />

Chapter 5<br />

At z 5 in figure 5.21 the fluctuations in u <strong>and</strong> v velocity components are<br />

higher in the region around cylinder axis <strong>and</strong> lower at large radial positions<br />

near cylinder wall. Due to increase in the size <strong>of</strong> the vortex core this region<br />

with higher values is large. However, the relative difference between the<br />

minimum <strong>and</strong> maximum values is small. Fluctuations in the axial velocity<br />

component w is still dominant. The cylinder center region has minimum<br />

ww values <strong>and</strong> the near wall region has the highest values. For all the<br />

normal Reynolds stress components, the decrease in magnitude from z to z 1 5<br />

is by an order <strong>of</strong> 10. Compared to fully open port, the magnitude <strong>of</strong> all the<br />

normal Reynolds stress components are nearly twice the value at z . 5<br />

The effect <strong>of</strong> wall at z has changed the distribution <strong>of</strong> Reynolds stress<br />

1<br />

components v v <strong>and</strong> vrv r in the cross-sectional plane. The region around<br />

the vortex core location still has higher values but the region with low<br />

magnitude <strong>of</strong> v v <strong>and</strong> vrv r ,as in case <strong>of</strong> 25% closure, is distorted.<br />

However, at z a more clear picture can be seen where their values increase<br />

5<br />

from large radial positions in the direction <strong>of</strong> cylinder axis region where the<br />

vortex core is resided.<br />

75% Port Closure<br />

When the intake port is 75% closed, the variance in the axial velocity is very<br />

large at z 1 compared to u <strong>and</strong> v velocity components (Figure 5.23). The<br />

spatial distribution is also very anisotropic for ww . For all aforementioned<br />

cases where the axial velocity has a jet-like pr<strong>of</strong>ile, the fluctuations in axial<br />

velocity are comparatively low at the center <strong>of</strong> the jet. The gradual increase in<br />

the outward radial direction decreases again towards the wall, after attaining<br />

a high value. The radial location <strong>of</strong> this peak ww region seems to exist at<br />

the outer periphery <strong>of</strong> the jet where a mixing occurs with the fluid near the<br />

wall region. In the current case, this peak region is at a smaller distance from<br />

the jet center than previous cases possibly because the wall recirculation zone<br />

has comparatively grown in case <strong>of</strong> 75% port closure at z . uu <strong>and</strong> vv <br />

1<br />

components have lowest values at large radial positions from the vortex core.<br />

There is radially large region around the cylinder axis where patches <strong>of</strong> high<br />

<strong>and</strong> low values are observed. The peak values <strong>of</strong> uu <strong>and</strong> vv are nearly<br />

half the value <strong>of</strong> ww .<br />

A resultant <strong>of</strong> the uu <strong>and</strong> vv components given in figure 5.23 with the<br />

same color scale as figure 5.22 shows that the in-plane Reynolds normal<br />

stresses are higher in the central region around cylinder axis <strong>and</strong> decreases<br />

towards the wall region.<br />

128<br />

Effect <strong>of</strong> Piston Position

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