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MIT’s N+3 Project:
The D8 Aircraft Concept
and Its Boundary Layer Ingestion Benefit
Technology Lead: Alejandra Uranga [email protected] Investigator: Edward Greitzer [email protected] Engineer: Mark Drela [email protected]
MIT / Aurora / Pratt & Whitney
4th International Workshop on Aviation and Climate ChangeUniversity of Toronto Institute for Aerospace Studies
May 28, 2014
Summary
I Closer integration of propulsion system and airframe provides newopportunities to reduce fuel burn and emissions of commercial aircraft
I Boundary layer ingestion (BLI)
I Novel configurations
I System optimization (airframe, engine, operations)
I Flow power and dissipation in power balance framework provide usefulmetrics for integrated configurations
MIT N+3 Phase 2 1 / 32
True OptimumOptimization of the aircraft as an integrated system can reach higher levels offuel e�ciency than separate optimization of airframe and propulsion system
. existing engines
existing airplanes
W/S , . . .
t 4
Λ ,
FPR,BPR,T
EngineParameters
AirframeParameters
true optimum
fuel burnisocontours
h cruise t/cM ,
OperatingParameters
.
.
. . .
airframer design domain
engine manufacturer design domain
apparent (false) optimum
MIT N+3 Phase 2 2 / 32
M. Drela
MIT N+3 Project
NASA N+3 Program, Fixed Wing Project
I Develop advanced aircraft concepts and enabling technologiesfor step improvements in fuel e�ciency and emissionsof commercial aircraft entering service in 2025 – 2035
Phase 1 (2008 – 2010)
I MIT-led team developed the double-bubble D8 aircraft concept
I Opportunity to impact the way the industry thinks about aircraft andpropulsion
MIT N+3 Phase 2 3 / 32
The D8 Aircraft ConceptMIT N+3 D8.2
MIT N+3 Phase 2 4 / 32
I B737-800/A320 class
I 180 PAX, 3,000 nm range
I Double-bubble lifting fuselagewith pi-tail
I Two aft, flush-mounted enginesingest ⇠ 40% of fuselage BL
I Cruise Mach 0.72
�37% fuel with current tech(configuration)
�66% fuel with advanced tech(2025-2035)
No “magic bullet”
E. Greitzer et al. 2010, NASA CR 2010-216794
MIT N+3 Phase 2 5 / 32Photos NASA/George Homich
System Impact of BLI
BLI benefitsI
Aerodynamic (direct) benefitsI Reduced jet and wake dissipationI Reduced nacelle wetted area
ISystem-level (secondary) benefits
I Reduced engine weightI Reduced nacelle weightI Reduced vertical tail sizeI Compounding from reduced overall weight
“Morphing” sequence: B737-800 7! D8I Features of D8 introduced one at a time
I Sequence of conceptual designs, optimized at each step (TASOPT)
MIT N+3 Phase 2 6 / 32
E. Greitzer et al. 2010, NASA CR 2010-216794
M. Drela 2011, AIAA 2011-3970
Morphing Sequence: B737-800 7! D8.2 7! D8.6
0
0.2
0.4
0.6
0.8
1
88 %
81 %
82 %
67 %
66 %
100 %
op
tim
ize
d7
37
-8
00
M=
0.8
,C
FM
56
en
gin
e
0
slow
to
M=
0.7
2
1
D8
fu
se
la
ge,
pita
il
2
re
ar
po
dd
ed
en
gin
es
3
in
te
gra
te
de
ng
in
es,
BL
I
4
op
tim
ize
en
gin
eB
PR
,F
PR
5
20
10
en
gin
es
8
Fuel
Burn
63 %
D8.2
6 7 9 10
20
35
en
gin
es
20
35
ma
te
ria
ls
win
gb
ot.
NL
F
sm
art
stru
ct
48 %
38 %
35 %
34 %
D8.6
- 15 %
MIT N+3 Phase 2 7 / 32
Phase 2: Nov. 2010 – Nov. 2014
Research thrusts
I Airframe-propulsion system integration (Task 1)
I Define/design aft section of D8 (integration of engines into fuselage)
I Quantify aerodynamic benefit of BLI
I Propulsor performance with distortion from BLI
I Phenomena, expected (and unexpected) behavior
I High e�ciency, high pressure ratio small core engines (Task 2)
I Limits to performance
I Technology opportunities for performance enhancement
I Innovative propulsion system architectures
MIT N+3 Phase 2 8 / 32
NASA N+3 Phase 2
How
I Direct, back-to-back comparisonof non-BLI and BLI configurations(podded) (integrated)
I Turbomachinery characterization
Tools
I Experiments at NASA Langley14⇥22 wind tunneland MIT tunnels
I Computational studies
I Close collaboration with NASA
MIT N+3 Phase 2 9 / 32
Outline
1 Introduction
2 MethodologyPerformance Metric for BLIConfigurationsApproach
3 Results
4 Summary
MIT N+3 Phase 2 10 / 32
Nomenclature
FX , CX =FX
q1SNet stream-wise force (“drag minus thrust”)
PE , CPE =PE
q1SV1Electrical power supplied to propulsors
PK , CPK =PK
q1SV1Mechanical flow power through propulsors
V1 , q1 =1
2⇢1V 21 Free-stream (tunnel) speed, dynamic pressure
S Reference area (1686 in2, 1.088 m2 at 1:11 scale)
D Propulsor fan diameter (5.67 in, 0.072m at 1:11 scale)
MIT N+3 Phase 2 11 / 32
BLI Analysis
I Ambiguous decomposition into drag and thrust(airframe) (propulsion system)
I Use power balance method instead of force accounting
I BLI reduces wasted KE in combined jet+wake (mixing losses)
wake, or “draft”
WastedKinetic Energy
Zero NetMomentum
combined wake and jet
propulsor jet
+
+
+
+
+
+
+
-
-
-
MIT N+3 Phase 2 12 / 32
M. Drela 2009, AIAA Journal 47(7)
Power Balance method
Consider mechanical energy sources and sinks: [ Power In ] = [ Dissipation ]
⇢⇢PS|{z}shaftpower
+ ⇢⇢PV|{z}p dVpower
+ PK|{z}mechanicalflow power
= �jet
+ �wake
+ �fuse
+ �vortex
+ Ė|{z}power
out of CV
PK
�wake
�wake �vortex
�vortex�fuse
�fuse
PK
�jet
�jet
Non-BLI Configuration
BLI Configuration
MIT N+3 Phase 2 13 / 32
M. Drela 2009, AIAA Journal 47(7)
Power Balance methodAerodynamic (direct) benefit of BLI configuration
Reduced jet + wake dissipation, reduced nacelle wetted area
P
BLI
K � �BLIjet| {z }Net propulsive power
= PBLIK ⌘BLI
p|{z}>⌘p
= �BLIwake| {z }
(1�fBLI)�wake
+ �BLIfuse
+ �vortex
PK
�wake
�wake �vortex
�vortex�fuse
�fuse
PK
�jet
�jet
Non-BLI Configuration
BLI Configuration
MIT N+3 Phase 2 14 / 32
M. Drela 2009, AIAA Journal 47(7)
BLI Benefit
BLI benefit (aerodynamic)
Savings in power required for given net stream-wise force
with BLI engines relative to non-BLI engines
Power metric
Mechanical flow power transmitted to the flow by the propulsors
PK =
I(po � po1)V · n̂ dS
BLI benefit ⌘ PKnon-BLI � PKBLIPK
non-BLI
����at given FX
MIT N+3 Phase 2 15 / 32
Obtaining PK
Method 1: Integration of the flow over cross-section of the stream-tubeupstream and downstream of the propulsor: flow survey data
PK =
Z
exit
(po � po1)V · n̂ dS �Z
inlet
(po � po1)V · n̂ dS
exit
inlet inlet
exit
Method 2: From electrical power provided to the propulsor motor,which is related to mechanical flow power through fan and motor e�ciencies
PK|{z}mechanicalflow power
= ⌘f|{z}fan
e�ciencyPK/PS
⇥ ⌘m|{z}motor
e�ciencyPS/PE
⇥ PE|{z}electricalpower
MIT N+3 Phase 2 16 / 32
Podded (non-BLI) Configuration
MIT N+3 Phase 2 17 / 32
Photo NASA/George Homich
0 50 in10
Integrated (BLI) Configuration
MIT N+3 Phase 2 18 / 32
Photo NASA/George Homich
0 50 in10
Back-to-Back Comparison
MIT N+3 Phase 2 19 / 32
Podded(non-BLI)
Integrated(BLI)
BLI benefit =CPK
podded
� CPKintegrated
CPKpodded
�����at given CX
Bases for ComparisonGiven a BLI propulsor with some jet velocity, mass flow, nozzle area,
how do you choose an “equivalent” non-BLI propulsor as basis for comparison?
1 1.2 1.4 1.6 1.8
1
1.02
1.04
1.06
1.08
1.1
0.98
0.8
CPKCPK , BLI
A
A
BLI propulsor
Non−BLI propulsorswith same net force
same Vjet
same
same fanm
A
same PK
.
smaller propulsor
nozzle
nozzle
nozzle, BLI
lowerpropulsorpower
MIT N+3 Phase 2 20 / 32
(=
Scaling Considerations for Low Speed Study
No dynamic symilarity between full-size D8 and experiments:Reynolds number and Mach number are not matched
) How do we ensure BLI benefit results are representative of full-size conditions?
I Airframe scaled geometrically by 1:11 from full-size, current-technology D8(fuselage, wing and tail planforms, fan diameter)
I Wing profiles and sweep designed for low speed (low Mach, low Re)
I Propulsion system scaling
I Use same propulsion system for both BLI and non-BLII Data taken with varying nozzle area to bracket design power and
propulsive e�ciency at cruise condition
I Investigate o↵-design points
MIT N+3 Phase 2 21 / 32
Experimental Approach
I NASA Langley 14⇥22 Foot Subsonic Wind TunnelV1 = 70 mph, M1 = 0.09, Rec = 570,000
I 1:11 scale, 13.4 ft span, powered D8 model
I Podded and integrated configurations share a large part of hardwareI Common wings and front 80% of fuselageI Common propulsor units plug into interchangeable tails
(fan stage, motor, center-body, housing, nozzle, electronics)I All model surfaces tripped
I Data collectionI Forces and moments (internal NASA balance)I Electrical powerI Fan wheel speedI Rake system for total and static pressure surveys
MIT N+3 Phase 2 22 / 32
Outline
1 Introduction
2 Methodology
3 ResultsBLI BenefitFlow SurveysDissipation
4 Summary
MIT N+3 Phase 2 23 / 32
BLI BenefitCPK BLI < CPK non-BLI for any given CX
or CX BLI > CX non-BLI for any given CPK
0 0.02 0.04 0.06 0.08 0.1
-0.03
-0.02
-0.01
0
0.01
0.02
0.03
C
PKMechanical flow power coe↵.
integrated
podded
6% BLI benefit
at simulated cruise
C
X
Streamwise
force coe↵.
(“drag � thrust”)
MIT N+3 Phase 2 24 / 32
Survey Propulsor Inlet and Outlet
MIT N+3 Phase 2 25 / 32
Rotating rake systemin wind tunnel experiments
Total Pressure
Inlet Rake
Total Pressure
Exit Rake
Integrated Propulsor Ingested Flow
MIT N+3 Phase 2 26 / 32
Experiments Left propulsor Right propulsor BL profile
Total pressure coe�cient Cpt =pt � pt1
q1
z
Dfan
y/Dfan-0.6 -0.4 -0.2 0 0.2 0.4 0.6
0
0.2
0.4
0.6
0.8
1
1.2
-0.75 -0.5 -0.25 0
0
0.2
0.4
0.6
0.8
1
1.2
Left
Right
-1
-0.8
-0.6
-0.4
-0.2
0
-0.6 -0.4 -0.2 0 0.2 0.4 0.6
y/Dfan
z
Dfan
y/Dfan-0.6 -0.4 -0.2 0 0.2 0.4 0.6
0
0.2
0.4
0.6
0.8
1
1.2
-0.75 -0.5 -0.25 0
0
0.2
0.4
0.6
0.8
1
1.2
Left
Right
-1
-0.8
-0.6
-0.4
-0.2
0
-0.6 -0.4 -0.2 0 0.2 0.4 0.6
y/Dfan
↵ = 2�
11 kRPM(cruise)
↵ = 6�
13 kRPM(climb)
“Benign” stratified flow
Integrated Propulsor Exit Flow
MIT N+3 Phase 2 27 / 32
Experiments Left propulsor Right propulsor Jet profile
Total pressure coe�cient Cpt =pt � pt1
q1
0 1 2
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
Left
Right
-0.6 -0.4 -0.2 0 0.2 0.4 0.6-0.6 -0.4 -0.2 0 0.2 0.4 0.6
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
z
Dfan
y/Dfan y/Dfan
-0.4
0
0.4
0.8
1.2
1.6
0 1 2
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
Left
Right
-0.6 -0.4 -0.2 0 0.2 0.4 0.6
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
z
Dfan
y/Dfan
-0.4
0
0.4
0.8
1.2
1.6
-0.6 -0.4 -0.2 0 0.2 0.4 0.6
y/Dfan
↵ = 2�
11 kRPM(cruise)
↵ = 6�
13.5 kRPM(climb)
Clean exit flow
Dissipation as a Measure of Configuration Performance
Cut X=130
0 0.005 0.01 0.015 0.02 0.025 0.03 0.035 0.04
Integrated
Podded
Unpowered
⇣
wing
fuselage
nacelle
jet
MIT N+3 Phase 2 28 / 32
Dissipation as a Measure of Configuration Performance
Both podded and integrated configurations show separation at thejunctures of vertical tails and horizontal tail: ⇠ 1.2% of total dissipation
MIT N+3 Phase 2 29 / 32
Dissipation computed
on wake plane down-
stream of separation
Outline
1 Introduction
2 Methodology
3 Results
4 Summary
MIT N+3 Phase 2 30 / 32
Conclusion
I Aero BLI benefit: 6%± ? saving in power (fuel) with BLI at cruise
I Estimated total, system-level fuel burn savings of 15% enabled by BLI
I D8 with estimated 37% fuel saving over conventional tube-and-wingcan be built “today”
Data supports feasibility of using BLI to improve fuel e�ciencyand viability of D8 concept
An exciting project aimed at
changing the way industry thinks about aircraft and propulsion,
and the look of civil transport aircraft
MIT N+3 Phase 2 31 / 32
Acknowledgments
NASA Fundamental Aeronautics Program, Fixed Wing ProjectCooperative Agreement NNX11AB35A
MIT N+3 team
Partners at Aurora Flight Sciences, Pratt & Whitney, NASA
Harold (Guppy) Youngren of Aerocraft Inc.
Sta↵ at NASA Langley 14⇥22 Foot Subsonic Wind Tunnel
NASA Fixed Wing Project management
MIT N+3 Phase 2 32 / 32
1IntroductionMIT N+3 ProjectSystem Impact of BLINASA N+3 Phase 2
2MethodologyPerformance Metric for BLIConfigurationsApproach
3ResultsBLI BenefitFlow SurveysDissipation
4Summary