principal investigator: prof. david g. bogard todd ... · todd davidson and david kistenmacher. ......
TRANSCRIPT
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1
Improving Durability of Turbine Components Through Trenched Film Cooling and Contoured
Endwalls
Principal Investigator: Prof. David G. Bogard
Todd Davidson and David KistenmacherUniversity of Texas at Austin
Co-Principal Investigator:Prof. Karen A. Thole
Alan Thrift and Amy MenschPennsylvania State University
Background image: [Hamed, A., Tabakoff, W., and Wenglarz, R., 2006]
DOE Award Number DE-FE0005540UTSR Project Number 07-01-SR127
UTSR Peer Review Workshop VIIOctober 25, 2011
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Project Objectives
a. Evaluate the degradation of performance for trench and crater film cooling configurations when subjected to active deposition of contaminants. This will be done on simulated vane and endwall models.
b. Design improved trench or crater film cooling configurations that mitigate the degradation effects of deposition of contaminants.
c. Determine the overall cooling effectiveness (including conjugate heat transfer effects) with and without thermal barrier coatings for the vane and endwall.
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Project Objectives, continued
d. Develop the knowledge needed to design film cooling configurations on contoured endwalls.
e. Perform detailed velocity and thermal field measurements along the vane, endwall, and downstream wake, with and without film cooling, to provide benchmarks to evaluate CFD simulations.
f. Develop improved cooling designs specifically for the vane-endwall junction including mitigation of deposition effects.
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Experiments were conducted to investigate effects of TBC and contaminant depositions on film cooling performance for a vane.
4
Test section:
• Performance was quantified in terms of overall effectiveness.
• Multiple hole geometries were investigated.
Flow direction
Turbulence grid / wax sprayer location
Test airfoil / deposition surface
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What is the overall effectiveness?
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The “overall effectiveness”, ϕ, is obtained using a conducting model and is defined as follows:
cm
TTTT−−
=∞
∞φwhere: Tm = “metal” temperature
T∞ = mainstream temperature
Tc = coolant temperature in the plenum
ϕ is a dimensionless surface temperature for a conducting model which takes into account conduction through the blade wall, film cooling, internal cooling, and convective cooling within coolant holes.
exitc
aw
TTTT
,−−
=∞
∞ηT∞ = mainstream temperature
Taw = adiabatic wall temperaturecoolant temperature at the exit of the hole
Tc,exit =
Adiabatic effectiveness is traditionally used to quantify film performance
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To achieve a properly scaled ϕ, certain parameters must be matched
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A simplified 1-D analysis using Taw as the driving temperature shows: Taw
Ti
TwT∞
qf”
qi”
Tc,i
ηηφ +++
−=
i
ehhBi1
1
with
kthBi e=
he = external heat transfer hi = internal heat transfer coefficient t = wall thicknessk = conductivity of the solid
Matched Bi was achieved using DuPont Corian®, k = 1.0 W/m.K
Also important to match the he /hi ratio. This is done even though the magnitudes of he and hi are much less than in the engine.
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Of particular interest was quantification of the improved overall effectiveness due to use of TBC • Although TBC is used extensively on actual engine hardware, there has
been little experimental study because of the reliance on adiabatic effectiveness measurements.
• Trench and crater configurations can potentially be formed using TBC
7
Computational study of the effects of hole blockage due to TBC (Na et al., 2007)
Adiabatic Conducting with TBC
ηηφ ++++
−+=
i
eVaneTBC
TBC
hhBiBi
Bi1
1)1(Overall effectiveness with TBC:
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Distributions of overall effectiveness with no film cooling, i.e. φ0, with and without TBC
TBC: t =2.3mm, t/d =0.55
Suction sidePressure side
φ increases with increasing internal coolant flow rates
Use of TBC results in as much as a factor of 3 increase in φ
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Film cooling configurations on suction side of the vane
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Trench Embedded round holes
t/d = 0.55 (cork thickness)
w/d = 2
Source: Bunker, 2002
Rounds Holes 24 holes
s/C = 0.23
d = 4.2 mm
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Overall effectiveness on the suction side with TBC –comparison of round and trench film cooling configurations.
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0 0.2 0.4 0.6 0.8 1s/C
Round
Trench
No Film
Location of Coolant Holes
φ
M = 1.3
Surprisingly the trench does not show noticeable improvement, and has decreased overall effectiveness in the trench
Suction side
Notice the upstream cooling due to convective cooling in the holes
TBC thickness, t =2.3mm or t/d =0.55
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Evaluation of predictions of φ based on measured values of η and φ0
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0 0.2 0.4 0.6 0.8 1
s/C
M=1.30, TBC
M=1.30, No TBC
Predicted M=1.30, TBC
Predicted M=1.30, No TBC
Location of Coolant Holes
φ
ηηφφ +−= )1(0Prediction of overall film effectiveness using:
Predictions are poor near the coolant holes due to convective cooling in the holes.
Predictions are good farther downstream
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1d
2d
3d 30°
1.27 cm0.51 cm
2d
2d
½ d
Film cooling configurations used with pressure side coolant holes
Round
Crater
Modified trench
TBC
Corian
Row of holes
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Overall effectiveness on pressure side with showerhead and PS row of holes with no TBC
Pressure side
Increasing φ with increasing blowing ratio in showerhead region
Decreasing φ with increasing blowing ratio downstream of pressure side holes
Row of holes
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Overall effectiveness on pressure side with showerhead and PS row of holes with TBC
TBC: t =5.1mm , t/d = 1.21
Pressure side
Increasing φ with increasing blowing ratio in showerhead region
No change in φ with increasing blowing ratio downstream of pressure side holes
Row of holes
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Overall effectiveness on pressure side with showerhead and PS row of holes with and without TBC
Pressure sideTBC: t =5.1mm , t/d = 1.21
TBC has a more substantial effect than film cooling on the overall cooling effectiveness
Row of holes
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Overall effectiveness with varying film cooling configurations with TBC
Pressure side
Modified trench configuration provides slightly higher overall cooling effectiveness.
Row of holes
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• Turbine depositions: Molten/softened ash particles impact and solidify on cooled airfoils and endwalls.
• This study simulates this in a wind tunnel using molten wax particles.
Contaminant depositions simulated using wax spray technique
17
Schematic of the wax spray device:Photo of wax spray device in turbulence grid:
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Images of deposition with film cooling with round holes
Pressure side Showerhead
Pressure side round holes blocked by depositions
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Images of deposition with film cooling with the crater configuration in TBC
Pressure side Craters are not blocked by depositions, but large buildup of depositions upstream and downstream of coolant holes.
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Images of deposition with film cooling with the modified trench configuration in TBC
Again, holes are not blocked by depositions, but large buildup of depositions upstream and downstream of coolant holes.
Appears that coolant interaction with molten particles has stimulated growth of depositions
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Effect of depositions on overall cooling effectiveness for a film cooled vane with TBC
Pressure side
Row of holes
Depositions cause an increase in overall cooling effectiveness!
Little effect on the suction side because deposition thickness is small
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A range of interface slot geometries were evaluated in the large scale, closed loop wind tunnel at PSU
Leakage Slot
Cax
4530
65
0.17Cax
0.17Cax 90
0.17Cax
Slot Geometries
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Net heat flux reduction characterized the durability of the vane endwall for leakage MFR and I
−−=
−=
ϕη
1hh
1q
qqNHFR
c
o''o
''c
''o
2
2cc
UρUρ
(I) ratio flux momentum∞∞
=∞
=mm
(MFR) ratio flux mass c
overall effectiveness (metal temperature), assumed uniform value of 0.6
T∞
Tc
Nearly adiabatic wallTaw
T∞
Tc
Heat flux wallTw
c
w
TTTT
−−
=∞
∞ϕc
aw
TTTT
η−−
=∞
∞
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The stagnation plane flow field was measured using a high-image-density TRDPIV system
High speed camera
Light sheet
x
y
Flowfield was sampled at 1000Hz(12t1*) for 250t1
*
x
z Vane
Double pulsed laser
t1* = δ/U∞
Flow seeded with DEHS
Image 1
U(t), V(t)
Image 2t
t +Δt
Cross correlation
LaVision
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The pressure side of the passage remains uncooled for all injection angles at low MFR
η90 45
MFR = 0.5%, I = 0.7
3065
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As injection angle was decreased, endwall effectiveness improved for higher MFR
η90 45
MFR = 1.0%, I = 2.8
3065
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Nusselt number contours are less affected by slot orientation at the case with lower MFR
90 45 3065
1300120011001000900800700600500400300
air
axc
kCh
Nu =MFR = 0.5%, I = 0.7
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Nusselt number contours for orientation angles less than 45° had a more pitchwise uniform distribution
90 45
MFR = 1.0%, I = 2.8
3065
1300120011001000900800700600500400300
air
axc
kCh
Nu =
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NHFR contours were mostly influenced by adiabatic effectiveness
90 45 3065MFR = 0.5%, I = 0.7
−−=ϕη
1hh
1NHFRc
o
2.01.81.61.41.21.00.80.60.40.20-0.2-0.4
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High momentum flux ratio results indicated most of the passage had a positive benefit from the slot
90 45 3065
−−=ϕη
1hh
1NHFRc
o
2.01.81.61.41.21.00.80.60.40.20-0.2-0.4
MFR = 1.0%, I = 2.8
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The highest area averaged net heat flux reduction was measured for I = 2.8, MFR = 1.0%, with a 45° slot
90 65 45 30Slot Orientation (°)
Area
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Cooling of the vane endwalls is complicated by secondary flows originating in the boundary layer
Endwall crossflow
Counter vortex
EndwallInlet boundary layer
Passage vortex
Vane
[Langston, 1980]
Endwall
(y)ρU21(y)P(y)P 2
11o1 +=(y)P(y)P o1o2 =
0(y)U2 =
(y)P(y)P o12 =
0dy
(y)dP1 = 0dy
(y)dP2 >
0(y)U1 ≠
1 2
U1Horseshoe vortex
A
2AA
A RUρ
np
=
∂∂
AR BR>
A
BB
2BB
B RUρ
np
=
∂∂
BA np
np
∂∂
=
∂∂
The viscous layer ensures that UA > UB , therefore
Vane
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Far from the vane an elongated HSV was measured, close to the vane the HSV was smaller
x/Cax = -0.34 Vane
x/Cax = -0.17
x/Cax
x/Cax = -0.05
Z/0.5S0.15
0.1
0.05
0
-0.4 -0.35 -0.3 -0.25 -0.2 -0.15 -0.1 -0.05 0
0.15
0.1
0.05
00.15
0.1
0.05
0
0.6
0.5
0.4
0.3
0.2
0.1
0
∞
+=
Uvu
Tu2rms
2rmsVane
MFR = 1.0%, I = 2.8U/U∞
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MFR = 1.0%, I = 2.8
90 65
3045
NoSlot
0.15
0.1
0.05
0-0.25 -0.2 -0.15 -0.1 -0.05 0
x/Cax
Z/0.5S U/U∞ 0.6
0.5
0.4
0.3
0.2
0.1
0
∞
+=
Uvu
Tu2rms
2rms
Intensity of the flowfield phenomenon increased with an increase in the MFR and I
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3535
90 65
3045
NoSlot
0.15
0.1
0.05
0-0.25 -0.2 -0.15 -0.1 -0.05 0
x/Cax
Z/0.5S U/U∞ 0.6
0.5
0.4
0.3
0.2
0.1
0
∞
+=
Uvu
Tu2rms
2rms
MFR = 0.5%, I = 0.7
Flow injection increased turbulence, but reducing the slot orientation to 45 reduced the HSV
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An oil flow visualization technique was used to draw streaklines of the flow along the endwall
Incoming Flow Direction Exit
Flow Direction
Top ViewPack-B Blade Cascade
No. of airfoils 7
Scale 8.6x
Axial chord (Cax) 0.218 m
Pitch/chord (P/Cax) 0.89
Aspect ratio (S/Cax) 2.5
Exit Reynolds number 200,000
Exit Mach number 0.04
Zweifel loading coefficient (Z) 1.15
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Conjugate heat transfer effects can be modeled by matching endwall Bi and ho/hi to engine parameters
ηhhBi1
1η-TT
TTφ
ic
wall +++
=−−
=∞∞
∞Overall effectiveness,
c
aw
TTTT
η−−
=∞
∞
wallkthBi ∞=
Top view of endwall
Bottom view of impingement plate
Top view
Tc ~ 25 C Coolant Plenum
hi
conducting endwall, kwall
impingement plate
t
BladeMainstream flow
h∞
T∞ ~ 55 C
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38
Conclusions
Measurements of the overall cooling effectiveness show the relative benefits of TBC and film cooling.
Cooling benefit of TBC dominated to the extent that there will little effect of the improved film cooling from crater and trench configurations.
Ironically the insulating effect of simulated depositions improved overall cooling effectiveness.
Reducing the angle below 45 for high momentum injection improved endwall cooling effectiveness.
Coolant injected at the lower momentum flux ratio was unable to cool the pressure side of the passage.
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39Background image: [Hamed, A., Tabakoff, W., and Wenglarz, R., 2006]
Questions?