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8/10/2019 Lab3 Lecture
1/24
Purpose
Test design
Measurement system and Procedures
Uncertainty Analysis
8/10/2019 Lab3 Lecture
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Purpose
Examine the surface pressure distribution and wakevelocity profile on a Clark-Y airfoil
Compute the lift and drag forces acting on the airfoil
Specify the flow Reynolds number
Compare the results with benchmark data
Uncertainty analysis for Pressure coefficient
Lift coefficient
8/10/2019 Lab3 Lecture
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Test Design
Facility consists of:
Closed circuit verticalwind tunnel.
Airfoil
Temperature sensor
Pitot tubes
Load cell
Pressure transducer
Automated data acquisition
system
8/10/2019 Lab3 Lecture
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Test Design (contd.)Airfoil(=airplane surface: as wing) is placed in
test section of a wind tunnel with free-stream velocity of 15 m/s. This airfoil isexposed to: Forces acting normal to free stream = Lift Forces acting parallel to free stream = Drag
Only two dimensional airfoils are considered:Top of Airfoil: The velocity of the flow is greater than the free-
stream. The pressure is negative
Underside of Airfoil: Velocity of the flow is less than the free-stream. The pressure is positiveThis pressure distribution contribute to the lift
8/10/2019 Lab3 Lecture
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Measurement systems
Instrumentation
Protractorangle of attack
Resistance temperature detectors
(RTD) Pitot static probevelocity
Vertical Pitot probe traverse
Scanning valvescans pressureports
Pressure transducer (Validyne) Digital Voltmeter (DVM)
Load celllift and drag force
Airfoil Model
Pitot Tube(Free
Stream)
Pressure Taps
Bundle oftubes
Digitali/o
A/DBoards
SerialComm.(COM1)
Software- Surface Pressure- Velocity- WT Control
PC
ScanivalvePosition
Circuit (SPC)
RTD
MetrabyteM2521Signal
Conditioner
ScanivalveSignal
Conditioner(SSC)
ScanivalveController
(SC)
Scanivalve
PressureTransducer(Validyne)
DigitalVoltimeter
(DVM)
PressureInput
8/10/2019 Lab3 Lecture
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AOA, and Pressure taps positions
8/10/2019 Lab3 Lecture
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Data reduction
In this experiment, the liftforce, L on the Airfoil willbe determined byintegration of the
measured pressuredistribution over the
Airfoils surface. Thefigure shows a typicalpressure distribution onan Airfoil and itsprojection .
8/10/2019 Lab3 Lecture
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Data reduction
Calculation of lift force The lift force L is determined by integration of the
measured pressure distribution over the airfoilssurface.
It is expressed in a dimensionless form by the
pressure coefficient Cpwhere, pi = surface pressuremeasured, = P pressure in the free-stream The lift force is also measured using the load cell and
data acquisition system directly.
U
= free-stream velocity, r = air density(temperature),
pstagnation= stagnation pressure measured at the tip ofthe pitot tube, L = Lift force, b = airfoil span, c =airfoil chord
cU
dspp
C sL2
2
1
sin
r
2
21
U
ppC ip
r
r
ppU
stagnation2
bcU
LCL 2
2
r
dsppLs
sin
8/10/2019 Lab3 Lecture
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Data reduction
The drag force, D on theAirfoil will be determinedby integration of themomentum loss found by
measuring the axialvelocity profile in thewake of the Airfoil. Thefigure shows how the wakeof the airfoil affects the
velocity profile.
8/10/2019 Lab3 Lecture
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Data reduction
Calculation of drag force The lift force D is determined by integration of the
momentum loss found from the velocity profilemeasurement.
The velocity profile u(y) is approximated by
measuring uiat predefined locations The drag force is also measured using the load celland data acquisition system directly.
U= free-stream velocity, r = air density
(temperature),pstagnation= stagnation pressure measured at the tip of
the pitot tube, D = Lift force, b = airfoil span, c =airfoil chord
dyuUucU
C i
y
y
iD
U
L
2
2
r
pypyu
stagnation )(2)(
bcU
D
CD 2
2
r
dyyuUyuDU
L
y
y
)()( r
8/10/2019 Lab3 Lecture
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Calibration of load cellmass (kg) Volts
0 -0.021
0.295 -0.1525
0.415 -0.203
0.765 -0.3565
1.31 -0.5935
1.635 -0.7385
Calibration program
Program output
Curve fitting method
8/10/2019 Lab3 Lecture
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Data acquisition
Setting up the initial motor speed Visualization of wind tunnel conditions
8/10/2019 Lab3 Lecture
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Data acquisition (contd.)
Data needed:
Observation point list
Sampling Rate
Settling Time
Length of each Sample
Angle of attack
Airfoil pressure visualization
8/10/2019 Lab3 Lecture
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Calculation of lift force
Program to measure lift force in volts
8/10/2019 Lab3 Lecture
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Calculation of drag force
Program to measure velocity in volts
8/10/2019 Lab3 Lecture
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Uncertainty analysis
8/10/2019 Lab3 Lecture
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Uncertainty analysisPressure coefficient Lift coefficient
),,( UppfC ip r
222
CpCpCp PBU
2
)(
2
)(
2
1
22
ppippiij
i
iCp BBB
2_2
Upp
C
i
p
ppi r
MSP CpCp 2
),,,,( cUppfC iil r
222
CLCLCL PBU
2
)(
2
)(
2
1
22
ppippiij
i
iCL BBB
MSP CLCL 2
8/10/2019 Lab3 Lecture
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Benchmark data
Distribution of the pressure coefficients for
= 0
, 4
, 8
, 16
and Re = 300,000
8/10/2019 Lab3 Lecture
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Benchmark data continued
Reference data for CL
Reference data for CD
8/10/2019 Lab3 Lecture
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ePIV
Measurements ofcomplete flow field witha small Clark-Y
Re1000
Chord length 20 mm
AoA of 0 and 16
Plot the following
Contour of velocitymagnitude
Vector field
Streamlines
Two models: AoA 0and 16
8/10/2019 Lab3 Lecture
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ePIV-Post Processing
Streamlines
Contour ofvelocity
magnitude
Velocity
vectors
8/10/2019 Lab3 Lecture
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ePIVPost Processing continued
Flow conditions
Re 1000
AoA = 16
PIV setting
Brightness = 35
Exposure = 100
Gain = 100
Frames = 9Window size = 30
Shift size = 15
PIV pairs = 9
AirfoilWake
Wall
Wall
Flow
8/10/2019 Lab3 Lecture
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ePIVAnalysisFlow features
Optical hindrance
Fast moving flow
Low pressureregion
Stagnation points
Slow moving flowHigh pressure
region
8/10/2019 Lab3 Lecture
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ePIVCFD ComparisonePIV CFD