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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 />

4.48:<br />

Avera age Static Pressur<br />

Drop p along the Cylin<br />

@ Re e = 1.2 x 10 5 re<br />

der<br />

.<br />

Fig gure 4.49:<br />

Average<br />

Static Pressu<br />

Drop p along the Cylin<br />

@ Re R = 0.6 x 10 5 ure<br />

nder<br />

.<br />

Chapter 4<br />

Figures 4.48 <strong>and</strong> 4.49 9 show the noormalized<br />

presssure<br />

drop aloong<br />

the cylindder<br />

for diffe ferent cylinder r lengths at ReeA<br />

<strong>and</strong> ReB resspectively.<br />

It ccan<br />

be seen thhat<br />

for bot th Reynolds numbers n the pressure dropp<br />

along the ccylinder<br />

decaays<br />

rapidly for the first 4 positions.<br />

The pre essure drop at position z1 is rrelatively<br />

highh<br />

compared to o other positionns<br />

<strong>and</strong> at the t next positi ion z2 the presssure<br />

drop redduces<br />

significaantly.<br />

A possibble<br />

reason is the shape <strong>of</strong> o inlet to thee<br />

cylinder whhere<br />

the flow from the swiirl<br />

generat tor (Inlet Sect tion) gets a shharp<br />

bendingg<br />

<strong>and</strong> creates a near cylindder<br />

wall re-circulating<br />

zone<br />

(Figure 3.44).<br />

For cyl linder length L3 at positioon<br />

z6, the prressure<br />

drop rreduces<br />

furthher<br />

indicati ing the effects <strong>of</strong> cylinder ouutlet<br />

wall, as tthis<br />

position foor<br />

L3 is closer to<br />

99<br />

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

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