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Experimental and Numerical Study of Swirling ... - Solid Mechanics

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Experi imental <strong>and</strong> <strong>Numerical</strong> N Stud dy <strong>of</strong> <strong>Swirling</strong> g Flow in Scaveenging<br />

Processs<br />

for 2-Stroke<br />

Marin ne Diesel Engin nes<br />

Figure F 4.26: :<br />

Normalized N Reynolds<br />

Stress<br />

Component t<br />

@ z5 L3=4D<br />

Chapter 4<br />

The hig gh uv ´´ zones s weaken in inntensity<br />

<strong>and</strong> mmove<br />

further radially<br />

outwarrd<br />

resultin ng in region near n to cylindder<br />

axis with low values (FFigure<br />

4.26). In<br />

general,<br />

the overall spatial<br />

distribuution<br />

<strong>of</strong> uv ´ ´ is in the formm<br />

<strong>of</strong> patches <strong>of</strong><br />

fluid re egions with high<br />

values in the middle o<strong>of</strong><br />

them <strong>and</strong> mmoving<br />

radiallly<br />

outward d as the swirl decays d downsttream<br />

<strong>and</strong> vorrtex<br />

core size increases.<br />

Figures 4.24-26, des scribes that iinitially<br />

at z11<br />

the Reynollds<br />

shear streess<br />

compon nent v v r is higher in thee<br />

vortex core region. The peak values aare<br />

observe ed at the radia al position at tthe<br />

interface o<strong>of</strong><br />

forced vorttex<br />

core <strong>and</strong> thhe<br />

outer an nnular region.<br />

In the annullar<br />

region, thee<br />

core has veryy<br />

small values <strong>of</strong><br />

77<br />

<strong>Swirling</strong> Flow in a Pipe

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