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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 4.39:<br />

No ormalized Axial<br />

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

L= 6D, 8D (z7 --- z13) ).<br />

Chapter 4<br />

The nor rmalized axial l velocity pr<strong>of</strong>i files at positionns<br />

z1-z6 for cyliinder<br />

lengths <strong>of</strong><br />

4D, 6D <strong>and</strong> 8D are sh hown in figurre<br />

4.38. The prr<strong>of</strong>iles<br />

are nearrly<br />

the same fo for<br />

a given position excep pt at z6 for cyllinder<br />

length 44D<br />

where due to the presence<br />

<strong>of</strong> cylin nder outlet an n increase in the axial veloocity<br />

is observved.<br />

Very smaall<br />

variatio ons in magnitu ude <strong>of</strong> axial velocity<br />

are obseerved<br />

in the annnular<br />

region. .<br />

At ReA <strong>and</strong> z7-z9, the Vz values in the vortex core<br />

are lower ffor<br />

L3 compareed<br />

to L2. Considering C th he Y-axis scalee<br />

this differencce<br />

however is very small. Foor<br />

ReB no such differen nce is observeed.<br />

With the decay in the swirl the axiial<br />

velocity y distribution for L2 <strong>and</strong> L3 gradually changes fromm<br />

a ‘wake-likke’<br />

91<br />

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

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