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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<br />

2.1:<br />

Classif fication <strong>of</strong> Swirl<br />

Types (Moene, ( 2003).<br />

swirling g flow. Thus the t focus in thhis<br />

chapter is on the theoreetical<br />

aspects <strong>of</strong><br />

confine ed swirling flow ws.<br />

2.1<br />

Classif fication <strong>of</strong> Confinned<br />

Swirliing<br />

Flowss<br />

Swirl fl lows mostly are a classified based on theeir<br />

tangential velocity pr<strong>of</strong>iile<br />

(Vanyo 1993, Steenbergen<br />

et al. 19998,<br />

H<strong>of</strong>fmannn<br />

et al. 2002) ). Moene (2003)<br />

has giv ven a rough classification <strong>of</strong> different tangential vvelocity<br />

pr<strong>of</strong>illes<br />

(Figure 2.1).<br />

(a a)<br />

(c c)<br />

r a<br />

(a) For rced Vortex: Flow<br />

essentiallly<br />

has a solid body rotationn<br />

i.e. the lineear<br />

(tan ngential in th his case) veloocity<br />

increasees<br />

with the iincrease<br />

in thhe<br />

dist tance from th he vortex cennter<br />

(Figure 22.1a).<br />

In case <strong>of</strong> a confineed<br />

swi irling flow, the t tangentiall<br />

velocity inccreases<br />

with radius until it<br />

reaches<br />

the wall boundary layyer<br />

where it ddecreases<br />

to zeero<br />

at the waall.<br />

(b)<br />

(d)<br />

Chapter 2<br />

12<br />

<strong>Swirling</strong> Flows

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