Experimental and Numerical Study of Swirling ... - Solid Mechanics
Experimental and Numerical Study of Swirling ... - Solid Mechanics
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