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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 />

Figur re 4.47:<br />

Pressure e Taps Location<br />

on Scav venging Flow Test t<br />

model.<br />

4.4<br />

Cylinder r Wall Prressure<br />

MMeasureme<br />

ents<br />

For eac ch measuring g position annd<br />

at a giveen<br />

Reynolds number, stattic<br />

differen ntial pressure is i measured beetween<br />

a poinnt<br />

close to the swirl generator<br />

inlet (radial<br />

distance e <strong>of</strong> 1 cm froom<br />

inlet ) as the referencee<br />

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

cylinder<br />

wall at that given g positionn<br />

(Figure 3.2).<br />

Where P in is the pr ressure at thee<br />

inlet <strong>and</strong> P z is the presssure<br />

at a giveen<br />

measuring<br />

position as<br />

mentioned iin<br />

(Table 4.1).<br />

The pre essure taps are e mounted at single point oon<br />

the circummference<br />

<strong>of</strong> eacch<br />

measuring<br />

cross sec ctional planee<br />

(Figure 4.447).<br />

The meaasured<br />

pressuure<br />

differen nce at differen nt positions tthus<br />

providess<br />

pressure droop<br />

downstreaam<br />

along th he cylinder len ngth with resppect<br />

to test moodel<br />

inlet.<br />

The me easurements are a conducted using a high resolution Fuurness<br />

digital differential micro m manommeter.<br />

For eaach<br />

position<br />

measure ed for a time period <strong>of</strong> 3-5 min with dataa<br />

acquisition f<br />

The me easured differe ential pressuree<br />

will represennt<br />

an average v<br />

case <strong>of</strong> three dimensional<br />

swirlingg<br />

flows especiaally<br />

flow with<br />

helical behavior <strong>of</strong> th he vortex, the pressure at thhe<br />

wall change<br />

followin ng the vortex behavior insidde<br />

the cylinderr<br />

<strong>and</strong> a measu<br />

<strong>of</strong> 1s may m not resolve e the high freqquency<br />

fluctuaation<br />

<strong>of</strong> wall s<br />

high Re e.<br />

® FC05110<br />

the pressure is<br />

frequency <strong>of</strong> 11s.<br />

value because in<br />

h asymmetric oor<br />

es with time i. .e.<br />

urement intervval<br />

tatic pressure at<br />

Pressure<br />

Tap<br />

P<br />

<br />

P<br />

P <br />

inn<br />

z<br />

Chapter 4<br />

(4. 1)<br />

98<br />

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

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