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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 />

Fi igure 4.38:<br />

No ormalized Axial<br />

Vel locity Pr<strong>of</strong>iles for r<br />

L=4 4D, 6D, 8D (z1 -- z6).<br />

For L2a <strong>and</strong> L3 the tangential<br />

velocitty<br />

decays in allmost<br />

the samme<br />

manner as L3<br />

except at a z6. Figure 4.37 4 shows thhe<br />

V pr<strong>of</strong>iless<br />

for the remaaining<br />

positionns<br />

i.e. z7-z9 9 for L2 <strong>and</strong> z7 7-z13 for L1. Thhe<br />

swirl decay results in the decrease in thhe<br />

V valu ues downstrea am to z6 <strong>and</strong> iincrease<br />

in thee<br />

size <strong>of</strong> the vvortex.<br />

For botth<br />

<br />

Reynold ds number the t peak V value moves<br />

to larger rradial<br />

distancces<br />

<br />

downstream<br />

<strong>and</strong> at z1 11 for L1, it seemms<br />

that the prr<strong>of</strong>ile<br />

shape haas<br />

changed from<br />

Rankine/burger<br />

vort tex to nearly solid body rotational forrced<br />

vortex. In<br />

general,<br />

it can be concluded<br />

that V graduallyy<br />

decays downnstream<br />

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

<br />

vortex enlarges in size<br />

with a grradual<br />

transittion<br />

from Raankine/<br />

Burgeers<br />

vortex to t forced vorte ex pr<strong>of</strong>ile.<br />

4.3.2<br />

Axial Vel locity Pr<strong>of</strong>i file<br />

Chapter 4<br />

90<br />

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

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