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How	CFD*	and	EFD	complement	each	other	in	
development	of	the	D8	aircra9		
ASME	Interna>onal	Mechanical	Engineering	Congress	and	Exhibit	
Phoenix,	AZ.	15	November	2016	
H.	Doğuş	Akaydın	
Senior	Research	Scien>st/Engineer	
Science	and	Technology	Corpora>on		
at	NASA	Ames	Research	Center	
James	C.	Jensen	
Research	Scien>st/Engineer	
Science	and	Technology	Corpora>on		
at	NASA	Ames	Research	Center	
Shishir	A.	Pandya	
Aerospace	Engineer	
NASA	Ames	Research	Center	
*	CFD:	Computa>onal	Fluid	Dynamics	
			EFD:	Experimental	Fluid	Dynamics
/27	2	
NASA	is	ac>vely	sponsoring	research	and	development	of	
cleaner,	less	noisy	and	more	efficient	transport	aircra9	
NASA	Advanced	Air	Vehicles	Program,	AATT	(Advanced	Air	Transport	Technology)	Project	Briefing
/27	3	
An	overview	of	the	state	of	the	art:	
plan	
1960	1950	 2010	t	 ?	
Progress	in	commercial	transport	aircra9	has	been	driven	mainly	by	
-  Engines	(became	more	efficient,	more	powerful	and	more	reliable)	
-  Composite	structures	(became	more	reliable)		
-  Control	surfaces	and	avionics	(became	more	sophis>cated)	
	
Airframe	integra>on,	however,	lagged:	Thin-tube	fuselages	and	wing-mounted	engines	are	
s>ll	the	state	of	the	art.
/27	4	
MIT’s	vision:	The	D8	“Double	Bubble”	Aircra9	
Aurora	Flight	Sciences,	Inc.	www.aurora.aero	
MIT:	Lead	the	research,	design	the	aircra9,	perform	wind	tunnel	tests	
Aurora	Flight	Sciences:	Build	wind	tunnel	models	and	flight	demonstrators	
Prae	&	Whitney:	Develop	the	engines	
NASA:	Sponsor	the	project,	provide	wind	tunnel	and	computer	>me	for	advanced	analysis
/27	5	
40%	reduc>on	in	fuel	burn	due	to	the	synergis>c	integra(on	
of	airframe	components	
	Op>mized	
		engines	
Newer	
engines	
D8	fuse.,	
π-tail	
Slow	to	
M=0.72	
BLI*	
Rela>ve	Fuel	Burn	
Integrated	
engines	
Podded	
engines	
D8	variant:	
*BLI:	Boundary	Layer	Inges>on	
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
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Greitzer	et	al.,	N+3	Aircra@	Concept	Designs	and	Trade	Studies.	Volume	1,	2010,	NASA	CR-2010-216794/VOL1	
B737-800
/27	6	
How	does	BLI	(boundary	layer	inges>on)	work?		
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
Drela,	Development	of	the	D8	Transport	Configura(on,	2011,	AIAA-2011-3970	
Drela,	Power	Balance	in	Aerodynamic	Flows,	2009,	AIAA	Journal	47(7)	
Pk																																	= Φjet+	Φwake+	Φfuse.	+	Φvortex	+	Ė					= Φ
PK = p0∞−p0( )
!
V ⋅
!
n dS
propulsor
"∫∫ Φ = p0∞−p0( )
!
V ⋅
!
n dS
wake plane
− prop. reg.
"∫∫ + 1
2
V−V∞( )
2
ρ
!
V ⋅
!
n dS
wake plane
"∫∫
Consider	two	configura>ons	at	cruise	(zero-net	force):	
⇥⇤⌅
⇥⇤⌅⇧
⌃⌥ ⌦
 ⇥
⇥⇤⌅
⇤ ⌅⇥
⌃⌥ ⌦
 ⇧
⇥⇤⌅
↵ ⇥⇤ ⇤✏
⇣⌥ ⌃⌥ ⌦
◆ ⇥⇤  ⌅⇧⌃⇥  ⌥ ⇥  ⌦↵ ⇤⇥  ⇥⇥⇤⌅
⌃⌥ ⌦
⌥⌘⇧ ⌥⌅ ✓◆
⌫ ⌘⌥
⌫ ⌘⌥ ⇠⇥ ⇡⌥⇢
⇠⇥ ⇡⌥⇢⇣⌅⌥
⇣⌅⌥
⌧⌥⇡
⌧⌥⇡
⇥⇤⌅⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
 ⌫⇠⇡ ⇢⇥⇤ ⌧ ⇤⌦ ⇡ ! "##
⌃⌥ ⌦↵ ✏⇣ ⌘✓⌘⌘ ◆ ↵ ⌫⇠⇡⇠⇢
Ė	
Podded	(non-BLI)	configura>on
/27	7	
How	does	BLI	(boundary	layer	inges>on)	work?		
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
Drela,	Development	of	the	D8	Transport	Configura(on,	2011,	AIAA-2011-3970	
Drela,	Power	Balance	in	Aerodynamic	Flows,	2009,	AIAA	Journal	47(7)	
Pk																																	= Φjet+	Φwake+	Φfuse.	+	Φvortex	+	Ė					= Φ
PK = p0∞−p0( )
!
V ⋅
!
n dS
propulsor
"∫∫ Φ = p0∞−p0( )
!
V ⋅
!
n dS
wake plane
− prop. reg.
"∫∫ + 1
2
V−V∞( )
2
ρ
!
V ⋅
!
n dS
wake plane
"∫∫
With	BLI,	the	terms	Φjet	,	Φwake	and	Ė	become	smaller.	
Consider	two	configura>ons	at	cruise	(zero-net	force):	
⇥⇤⌅
⇥⇤⌅⇧
⌃⌥ ⌦
 ⇥
⇥⇤⌅
⇤ ⌅⇥
⌃⌥ ⌦
 ⇧
⇥⇤⌅
↵ ⇥⇤ ⇤✏
⇣⌥ ⌃⌥ ⌦
◆ ⇥⇤  ⌅⇧⌃⇥  ⌥ ⇥  ⌦↵ ⇤⇥  ⇥⇥⇤⌅
⌃⌥ ⌦
⌥⌘⇧ ⌥⌅ ✓◆
⌫ ⌘⌥
⌫ ⌘⌥ ⇠⇥ ⇡⌥⇢
⇠⇥ ⇡⌥⇢⇣⌅⌥
⇣⌅⌥
⌧⌥⇡
⌧⌥⇡
⇥⇤⌅⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
 ⌫⇠⇡ ⇢⇥⇤ ⌧ ⇤⌦ ⇡ ! "##
⌃⌥ ⌦↵ ✏⇣ ⌘✓⌘⌘ ◆ ↵ ⌫⇠⇡⇠⇢
Ė	
Ė	
Podded	(non-BLI)	configura>on	
Integrated	(BLI)	configura>on
/27	8	
Experimental	and	Computa>onal	Tools	
Pandya,	External	Aerodynamics	Simula(ons	for	the	MIT	D8	“Double-Bubble”	Aircra@	Design,	2012,	ICCFD7-4304	
EFD:	NASA	Langley	14x229	Wind	Tunnel.	3D-printed	skin	and	modular	components	
Overflow	2.2,	NASA’s	workhorse	flow	solver	for	structured	curvilinear	overset	grids.		
Chimera	Grid	Tools	(CGT)	for	to	generate	these	CFD	grids.	
CFD:	
Nichols	and	Buning,	Users	Manual	for	OVERFLOW	2.2,	heps://overflow.larc.nasa.gov			
Chan,	Gomez,	Rogers	and	Buning,	Best	Prac(ces	in	Overset	Grid	Genera(on,	2002,	AIAA-2002-3191	
M∞≈0.1
/27	9	
EFD	serves	to	validate	and	improve	the	CFD	simula>ons	
Pandya,	External	Aerodynamics	Simula(ons	for	the	MIT	D8	“Double-Bubble”	Aircra@	Design,	2012,	ICCFD7-4304	
80	million	grid	points.	35	near-body	grids.	Wall	y+≈1	
24	hours	of	wall-clock	>me	spent	per	solu>on	on	380		Sandy	Bridge	cores	on	
Pleiades	Supercomputer.	
Unpowered	(no-propulsor)	D8	model.	
SS-RANS	(Steady-state	Reynolds-Averaged	Navier	Stokes)	solu>ons.	
0 5 10 15
α
0.5
1
1.5
2
L
WT
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.5
1
1.5
2
L
WT
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.5
1
1.5
2
L
WT
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.05
0.1
0.15
0.2
0.25
CD
WT
Cart3D
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.05
0.1
0.15
0.2
0.25
CD
WT
Cart3D
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.05
0.1
0.15
0.2
0.25
CD
WT
Cart3D
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
0.5
1
1.5
2 WT
Overflow - Spalart-Allmaras
Overflow - SST
CL	 CD
/27	10	
CFD	provides	further	insights	on	the	design	
(and	validates	the	design	concepts)	
0	 0.5	 1	
π-Tail	
Wing	
Fuse.	
Total	
0	 0.05	 -0.1	 0	 0.1	 0.2	
CL	 CD	 CM	α=4°	
Pandya,	External	Aerodynamics	Simula(ons	for	the	MIT	D8	“Double-Bubble”	Aircra@	Design,	2012,	ICCFD7-4304	
•  Tail	of	D8	creates	posi>ve	li9	or	less	nega>ve	li9	than	a	comparable	transport	aircra9.	
•  Fuselage	creates	a	fair	amount	of	li9	and	a	substan>al	amount	of	pitch-up	moment…	
•  …which	is	balanced	by	the	pitch-down	moment	from	wing	and	tail.
/27	11	
EFD	and	CFD	complement	each	other.	
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
Computa>on	of	propulsor	power	by	experimental	methods	
Greitzer	et	al.,	Aircra@	and	Technology	Concepts	for	an	N+3	Subsonic	Transport	–	Phase	2.	Year	3	Status	Review,	2014	
PK = p0∞−p0( )
!
V ⋅
!
n dS
propulsor
"∫∫
Integrated	(BLI)	configura>on:
/27	12	
EFD	and	CFD	complement	each	other.	
Greitzer	et	al.,	Aircra@	and	Technology	Concepts	for	an	N+3	Subsonic	Transport	–	Phase	2.	Year	3	Status	Review,	2014	
Stream	tube	into	the	propulsor	is	determined	by	CFD	
PK = p0∞−p0( )
!
V ⋅
!
n dS
propulsor
"∫∫
/27	13	
EFD	and	CFD	complement	each	other.	
⇥⇤⌅⇧⌃⇧⌃⌥ ⌦↵ ⌅ ✏⇣ ⌘ ✓ ◆ ⇤ ⌦ ⌫⇠
⇥⇤ ⌅⇧⌃⌥
⌦⇥↵
✏⇣⌘✓◆  ⌫✓⇣◆⇠⇡⇢ ⇡⇠⇡
⇥ ⇥⇤⇥ ⌅⇤⌅ ⇧ ⌃
⇡⇢⇢ ⇢✏⌧ ⇡◆⇠✓⇠✓
⇥ ⇥⇤⇥ ⌥⌅ ⇤⌅ ⇧ ⌃
⇡◆⇠✓⇠✓ ✏ ✓◆⇠⌫ ⇠
⇤ ⌦⌅ ↵
!⇧" ⌦#⇥⌥⌅" "⇥
"⇥"⌅⌥ ⌦⌅$ ⌃⌦!%
!⇧" ⌃⌦⌅"!⇥⇧
⌅⌦ ⌅
!⇧" ⌃⌦⌅"
⇠✏⇠⇡⇢ ⌫⇡&
⌫'( ⇡⇠⇡
⇥ ⇧ ⌃
⇠⇡⇠✓ ⌫⇡&
⌫'( ⇡⇠⇡
⇧ ⌃
⇠⇡⇠✓ )⌫✓⇠✏⇠⇡⇢ )⌫✓
*+ , + + ,
*+ ,
+
+ ,
⌅⌃
✏
*+ -
+
+ -
+ .
/ 0
/ ,
⇣⇤ ⌅⌃
⌘
⇧
✓
⇥⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆  ⌫⇠⇠
Pandya,	External	Aerodynamics	Simula(ons	for	the	MIT	D8	“Double-Bubble”	Aircra@	Design,	2012,	ICCFD7-4304	
Greitzer	et	al.,	Aircra@	and	Technology	Concepts	for	an	N+3	Subsonic	Transport	–	Phase	2.	Year	3	Status	Review,	2014	
Local	flow	direc>ons	on	the	rake	survey	
plane	is	determined	by	CFD	
PK = p0∞−p0( )
!
V ⋅
!
n dS
propulsor
"∫∫
/27	14	
EFD	and	CFD	complement	each	other.	
Pandya	et	al.,	Computa(onal	Assessment	of	the	Boundary	Layer	Inges(ng	Nacelle	Design	of	the	D8	Aircra@,	AIAA-2014-0907	
⇤⌅⇧⌃⌥⇤⌅ ⌃⌦↵ ⌦⌃ ⇥⇧⌅ ⇤⌅ ✏ ⌦⇣
⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆  
⇥
⇤⌅⇧⌃ ⌥ ⌥⌦↵ ✏⇣⌃ ⌥ ⌥⌦↵ ⌘⇤ ⌥ ✓↵⌅
◆ ⌃↵ ⌥ ⌅ ⌦ ⌅ ⌅ ⌅⌫⌃ ⇥
⇥⇥ ⇥⇥
⇤
⇥⌘⌥⇥
⇤⌅⇥⌘⌥⇥
⇥⇤⌅ ⇥⇤⇧ ⇥⇤⌃ ⇥ ⇥⇤⌃ ⇥⇤⇧ ⇥⇤⌅
⇥
⇥⇤⌃
⇥⇤⇧
⇥⇤⌅
⇥⇤⌥
⇤⌃
⇥⇤ ⌦ ⇥⇤⌦ ⇥⇤⌃⌦ ⇥
⇥
⇥⇤⌃
⇥⇤⇧
⇥⇤⌅
⇥⇤⌥
⇤⌃
↵
✏⇣⌘✓
⇥⇤⌥
⇥⇤⌅
⇥⇤⇧
⇥⇤⌃
⇥
⇥⇤⌅ ⇥⇤⇧ ⇥⇤⌃ ⇥ ⇥⇤⌃ ⇥⇤⇧ ⇥⇤⌅
⇤⌅⇥⌘⌥⇥
⇥⌘⌥⇥
⇤⌅⇥⌘⌥⇥
⇥⇤⌅ ⇥⇤⇧ ⇥⇤⌃ ⇥ ⇥⇤⌃ ⇥⇤⇧ ⇥⇤⌅
⇥
⇥⇤⌃
⇥⇤⇧
⇥⇤⌅
⇥⇤⌥
⇤⌃
⇥⇤ ⌦ ⇥⇤⌦ ⇥⇤⌃⌦ ⇥
⇥
⇥⇤⌃
⇥⇤⇧
⇥⇤⌅
⇥⇤⌥
⇤⌃
⇥⇤⌥
⇥⇤⌅
⇥⇤⇧
⇥⇤⌃
⇥
⇥⇤⌅ ⇥⇤⇧ ⇥⇤⌃ ⇥ ⇥⇤⌃ ⇥⇤⇧ ⇥⇤⌅
⇤⌅⇥⌘⌥⇥
⌥⌅ ⇢⌅⌫⌃
⇤
⇢⌥⌦⌃⌃ ⌫
⇤
⇠⇡ ⌅↵↵⌅⌫⌃ ⇢⌥ ⌫⇥⇤⌅⇧⌃⌥⇤⌅ ⌃⌦↵ ⌦⌃ ✏⇣⌘⇤ ✓ ⌦◆
⇥⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆
⇥
⇤⌅⇧⌃ ⌥ ⌥⌦↵ ✏⇣⌃ ⌥ ⌥⌦↵
◆ ⌃↵ ⌥ ⌅ ⌦ ⌅ ⌅ ⌅⌫⌃ ⇥
⇥⇥
⇤
⌅ ⇧⌃ ⌅ ⇧⌥ ⌅ ⇧⇤ ⇧⇤ ⇧⌥ ⇧⌃⌅ ⇧⌃ ⌅ ⇧⌥ ⌅ ⇧⇤ ⇧⇤ ⇧⌥ ⇧⌃
⌅ ⇧⌃
⌅ ⇧⌥
⌅ ⇧⇤
⇧⇤
⇧⌥
⇧⌃
⇥⌥⇥
⇤⌅⇥⌥⇥ ⇤⌅⇥⌥⇥
⌅ ⇧⌥
⇧⌥
⇧⇣
⇥⇧⇤
⇥⇧⌃
⌅ ⇧⌃ ⌅ ⇧⌥ ⌅ ⇧⇤ ⇧⇤ ⇧⌥
⌅ ⇧⌃
⌅ ⇧⌥
⌅ ⇧⇤
⇧⇤
⇧⌥
⇧⌃
⇥⌥⇥
⇤⌅⇥⌥⇥
⌅ ⇧⌥
⇧⌥
⇧⇣
⇥⇧⇤
⇥⇧⌃
⌅ ⇧⌥ ⌅ ⇧⇤ ⇧⇤ ⇧⌥ ⇧⌃
⇤⌅⇥⌥⇥
⇧⌃ ⌅ ⇧⌃
⇠⇡⌥⌅ ⇢⌅⌫⌃
⌃ ⇤
⌧ ⇢⌥⌦⌃⌃ ⌫
⌃ ⇤
⌧ ⇧⌫ ⌅⇧⇧⌃⌅
Greitzer	et	al.,	Aircra@	and	Technology	Concepts	for	an	N+3	Subsonic	Transport	–	Phase	2.	Year	3	Status	Review,	2014	
EFD:	
CFD:	
Inlet	 Outlet	
L	 R	
Total	pressure	coefficients.	L:	Le9	propulsor,	R:	Right	propulsor.	Views	from	rear	of	the	model.	
L R
/27	15	
CFD	and	EFD	reassures	confidence	in	results:	⇧⌃⌥ ⇥ ⇥⌦ ↵ ✏ ⇣⌘⌅ ⌃⌥⇤ ⇧ ✓ ◆
⇥⇤ ⌅⇧⌃⇧⌥ ⌃ ⇧⌦↵ ⇥ ✏
⌘ ✓◆◆ ⌦ ⌃ ⇧ ⌫⇧⌦ ↵⇧⌃ ⇠↵⇧ ⇡  ⇢ ⌧ ⌘ ✓◆◆ ⌦ ⌃
⇥ ⇤ ⇥ ⌅ ⇥ ⇧ ⇥ ⌃ ⇥⌥ ⇥⌥⇤
⇥
⇥ ⌅
⇥ ⌦
⇥ ⇤
⇥ ⌥
⇥ ⌥
⇥ ⇤
⇥ ⌦
⇥ ⌅
⇥
↵
↵
✏⇣⌘⌘✓⌘◆
⌫✓⇠⇡⇢⌫✓⌘◆
✏⇣⌘⌘✓⌘◆↵ ⌧
⌫✓⇠⇡⇢⌫✓⌘◆↵ ⌧
⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆  ⌃ ⌫⌫
ΔCPk=	-9%	
ΔCPk=	-8%	
cruise	
EFD	predicts	an	8%	±	0.7%		
reduc>on	in	power	to	sustain	cruise.	
	
CFD	predicts	a	9%	reduc>on.	
A	very	good	agreement	between	experimental	and	computa>onal	
predic>ons	of	BLI	benefit:	
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
Greitzer	et	al.,	Aircra@	and	Technology	Concepts	for	an	N+3	Subsonic	Transport	–	Phase	2.	Final	Review,	Dec.	2014	
Pandya	et	al.,	Computa(onal	Assessment	of	the	Boundary	Layer	Inges(ng	Nacelle	Design	of	the	D8	Aircra@,	AIAA-2014-0907
/27	16	
CFD	facilitates	in-depth	and	alternate	analysis	methods	
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
Drela,	Development	of	the	D8	Transport	Configura(on,	2011,	AIAA-2011-3970	
Drela,	Power	Balance	in	Aerodynamic	Flows,	2009,	AIAA	Journal	47(7)	
Pk																																	= Φjet+	Φwake+	Φfuse.	+	Φvortex	+	Ė					= Φ
PK = p0∞−p0( )
!
V ⋅
!
n dS
propulsor
"∫∫ Φ = p0∞−p0( )
!
V ⋅
!
n dS
wake plane
− prop. reg.
"∫∫ + 1
2
V−V∞( )
2
ρ
!
V ⋅
!
n dS
wake plane
"∫∫
Φ can	be	computed	in	separate	zones	in	the	wake	planes	
to	analyze	Φ	in	terms	of	Φjet,	Φwake,	Φfuse	…	etc.	
⇥⇤⌅
⇥⇤⌅⇧
⌃⌥ ⌦
⇥⇤⌅
⇤ ⌅⇥
⌃⌥ ⌦
⇥⇤⌅
↵ ⇥⇤ ⇤✏
⇣⌥ ⌃⌥ ⌦
⇥⇤⌅
⌃⌥ ⌦
⌥⌘⇧ ⌥⌅ ✓◆
⌫ ⌘⌥
⌫ ⌘⌥ ⇠⇥ ⇡⌥⇢
⇠⇥ ⇡⌥⇢⇣⌅⌥
⇣⌅⌥
⌧⌥⇡
⌧⌥⇡
⇥⇤⌅⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
 ⌫⇠⇡ ⇢⇥⇤ ⌧ ⇤⌦ ⇡ ! "##
⌃⌥ ⌦↵ ✏⇣ ⌘✓⌘⌘ ◆ ↵ ⌫⇠⇡⇠⇢
Ė	
Ė	
Podded	(non-BLI)	configura>on	
Integrated	(BLI)	configura>on	
Understanding	the	losses:
/27	17	
CFD	facilitates	in-depth	and	alternate	analysis	methods	
Wake	planes	to	compute	Φ terms	
Podded	(non-BLI)	configura>on	 Integrated	(BLI)	configura>on	
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
⇥⇤⌅
⇥⇤⌅⇧
⌃⌥ ⌦
 ⇥
⇥⇤⌅
⇤ ⌅⇥
⌃⌥ ⌦
 ⇧
⇥⇤⌅
↵ ⇥⇤ ⇤✏
⇣⌥ ⌃⌥ ⌦
◆ ⇥⇤  ⌅⇧⌃⇥  ⌥ ⇥  ⌦↵ ⇤⇥  ⇥⇥⇤⌅
⌃⌥ ⌦
⌥⌘⇧ ⌥⌅ ✓◆
⌫ ⌘⌥
⌫ ⌘⌥ ⇠⇥ ⇡⌥⇢
⇠⇥ ⇡⌥⇢⇣⌅⌥
⇣⌅⌥
⌧⌥⇡
⌧⌥⇡
⇥⇤⌅⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
⇧⌃⌥ ⇥⇤ ⌦↵ ✏⇥⇤
 ⌫⇠⇡ ⇢⇥⇤ ⌧ ⇤⌦ ⇡ ! "##
⌃⌥ ⌦↵ ✏⇣ ⌘✓⌘⌘ ◆ ↵ ⌫⇠⇡⇠⇢
Ė	
Ė	
Podded	(non-BLI)	configura>on	
Integrated	(BLI)	configura>on	
Understanding	the	losses:
/27	18	
CFD	facilitates	in-depth	and	alternate	analysis	methods	
Podded	Configura>on	
Wing	region	
fuselage		
region	
Jet	region	
Wing	region	
Integrated	Configura>on	
Zoning	of	the	wake	plane	to	break-down	Φjet,	Φwake,	Φfuse	contribu>ons	to	Φ
/27	19	
α=2°	
Uranga	et	al.,	Preliminary	Experimental	Assessment	of	the	Boundary	Layer	Inges(on	Benefit	for	the	D8	Aircra@,	AIAA-2014-0906	
Real	and	digital	tu9s	help	iden>fy	local	flow	direc>on	into	the	propulsors.		
CFD	helps	plan	and	improve	the	experiments
/27	20	
CFD	helps	plan	and	improve	the	experiments	
⇥ ⇤ ⌅⇧⌃⌥ ⌦⌅↵⇥ ⇥ ✏⇣⇧⌃ ✏⌅⌘ ⇣✓ ⇣⇧⌃ ✓⇥ ◆  ⌦↵ ⌦ ⌥✓ ↵
⌫ ◆◆ ◆ ⌦↵ ⌦ ⌥✓ ↵ ⇠⌅  ↵⌅⇣✓ ◆ ⇥ ⌅⇡ ⇣◆ ⇣⇧⇥ ↵⌅⇢⇥⇣ ⇧ ✏⇣⇥ ✏⇣⇧⌃ ✏⌅⌘
⇥⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆ 
⌧
⇤
Greitzer	et	al.,	Aircra@	and	Technology	Concepts	for	an	N+3	Subsonic	Transport	–	Phase	2.	Year	3	Status	Review,	2014	
Wing	wake	would	par>ally	
ingested	by	podded	propulsor	
at	α=6°	but	not	at	α=2°.	
A	suitable	dihedral	angle	θ	for	the	
pods	were	found	by	simula>ng	
mul>ple	models	(not	by	building	
and	tes>ng	mul>ple	models).	
θ=0°	 θ=30°	 …	(	and	other	θ angles	simulated)
/27	21	
CFD	helps	plan	and	improve	the	experiments	
Separa>on	regions	were	iden>fied	by	CFD	simula>ons.	
Elimina>on	of	these	regions	will	reduce	dissipa>on	losses	of	the	next	designs
/27	22	
EFD	and	CFD	complement	each	other.	
Source	Diagnos>c	Test	by	NASA	&	GE	
EFD	enables	development	of	advanced	CFD	models	
Simple	actuator	disk	model	 Advanced	actuator	zone	model	
Hall,	Greitzer	and	Tan,	Analysis	of	Fan	Stage	Design	AZributes	for	Boundary	
Layer	Inges(on,	ASME	Turbo	Expo	2016:	GT2106-57808.		
Akaydin	and	Pandya,	An	Advanced	Actuator	Zone	Model	for	Propulsor	
Simula(ons	with	OVERFLOW,	(in	review	for	AIAA	Avia>on	2017)	
Hughes,	Aerodynamic	Performance	of	Scale-Model	Turbofan	Outlet	Guide	
Vanes	Designed	for	Low	Noise,	AIAA-2002-0374
/27	23	
Summary	&	Discussion	
0 5 10 15
α
0.5
1
1.5
2
CL
WT
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.5
1
1.5
2
CL
WT
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.5
1
1.5
2
CL
WT
Overflow - Spalart-Allmaras
Overflow - SST
0 5 10 15
α
0.5
1
1.5
2
CL
WT
Overflow - Spalart-Allmaras
Overflow - SST
⇥⇤⌅⇧⌃⌥ ⇥ ⇥⌦ ↵ ✏ ⇣⌘⌅ ⌃⌥⇤ ⇧ ✓ ◆
⇥⇤ ⌅⇧⌃⇧⌥ ⌃ ⇧⌦↵ ⇥ ✏
⇣⌘ ✓◆◆ ⌦ ⌃ ⇧ ⌫⇧⌦ ↵⇧⌃ ⇠↵⇧ ⇡  ⇢ ⌧ ⌘ ✓◆◆ ⌦ ⌃
⇥ ⇤ ⇥ ⌅ ⇥ ⇧ ⇥ ⌃ ⇥⌥ ⇥⌥⇤
⇥
⇥ ⌅
⇥ ⌦
⇥ ⇤
⇥ ⌥
⇥ ⌥
⇥ ⇤
⇥ ⌦
⇥ ⌅
⇥
↵
↵
✏⇣⌘⌘✓⌘◆
⌫✓⇠⇡⇢⌫✓⌘◆
✏⇣⌘⌘✓⌘◆↵ ⌧
⌫✓⇠⇡⇢⌫✓⌘◆↵ ⌧
⇥⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆ 
ΔCPk=	-9%	
ΔCPk=	-8%	
cruise	
•  In	D8	project,	u>liza>on	of	EFD	and	CFD	methods	goes	beyond	cross-check	&	valida>on.	
CL
/27	24	
Summary	&	Discussion	
⇥⇤⌅⇧⌃⇧⌃⌥ ⌦↵ ⌅ ✏⇣ ⌘ ✓ ◆ ⇤ ⌦ ⌫⇠
⇥⇤ ⌅⇧⌃⌥
⌦⇥↵
✏⇣⌘✓◆  ⌫✓⇣◆⇠⇡⇢ ⇡⇠⇡
⇥ ⇥⇤⇥ ⌅⇤⌅ ⇧ ⌃
⇡⇢⇢ ⇢✏⌧ ⇡◆⇠✓⇠✓
⇥ ⇥⇤⇥ ⌥⌅ ⇤⌅ ⇧ ⌃
⇡◆⇠✓⇠✓ ✏ ✓◆⇠⌫ ⇠
⇤ ⌦⌅ ↵
!⇧" ⌦#⇥⌥⌅" "⇥
"⇥"⌅⌥ ⌦⌅$ ⌃⌦!%
!⇧" ⌃⌦⌅"!⇥⇧
⌅⌦ ⌅
!⇧" ⌃⌦⌅"
⇠✏⇠⇡⇢ ⌫⇡&
⌫'( ⇡⇠⇡
⇥ ⇧ ⌃
⇠⇡⇠✓ ⌫⇡&
⌫'( ⇡⇠⇡
⇧ ⌃
⇠⇡⇠✓ )⌫✓⇠✏⇠⇡⇢ )⌫✓
*+ , + + ,
*+ ,
+
+ ,
⌅⌃
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*+ -
+
+ -
+ .
/ 0
/ ,
⇣⇤ ⌅⌃
⌘
⇧
✓
⇥⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆  ⌫⇠⇠
•  In	D8	project,	u>liza>on	of	EFD	and	CFD	methods	goes	beyond	cross-check	&	valida>on.	
	
•  The	methods	also	complement	each	other:	CFD	facilitates	the	duty	of	EFD	and	vice	versa.
/27	25	
Summary	&	Discussion	
•  In	D8	project,	u>liza>on	of	EFD	and	CFD	methods	goes	beyond	cross-check	&	valida>on.	
	
•  The	methods	also	complement	each	other:	CFD	facilitates	the	duty	of	EFD	and	vice	versa.	
↵ ⇥⌃ ⌃ ⌅✏ ⌅⇤ ⇣⌘⇥✓
⇥ ✏⇣⇧⌃ ✏⌅⌘ ⇣✓ ⇣⇧⌃ ✓⇥ ◆  ⌦↵ ⌦ ⌥✓ ↵
⇠⌅  ↵⌅⇣✓ ◆ ⇥ ⌅⇡ ⇣◆ ⇣⇧⇥ ↵⌅⇢⇥⇣ ⇧ ✏⇣⇥ ✏⇣⇧⌃ ✏⌅⌘
 ⌫⇠⇠
/27	26	
Summary	&	Discussion	
•  In	D8	project,	u>liza>on	of	EFD	and	CFD	methods	goes	beyond	cross-check	&	valida>on.	
	
•  The	methods	also	complement	each	other:	CFD	facilitates	the	duty	of	EFD	and	vice	versa.
/27	27	
Summary	&	Discussion	
⇥⇤⌅⇧⌃⇧⌃⌥ ⌦↵ ⌅ ✏⇣ ⌘ ✓ ◆ ⇤ ⌦ ⌫⇠
⇥⇤ ⌅⇧⌃⌥
⌦⇥↵
✏⇣⌘✓◆  ⌫✓⇣◆⇠⇡⇢ ⇡⇠⇡
⇥ ⇥⇤⇥ ⌅⇤⌅ ⇧ ⌃
⇡⇢⇢ ⇢✏⌧ ⇡◆⇠✓⇠✓
⇥ ⇥⇤⇥ ⌥⌅ ⇤⌅ ⇧ ⌃
⇡◆⇠✓⇠✓ ✏ ✓◆⇠⌫ ⇠
⇤ ⌦⌅ ↵
!⇧" ⌦#⇥⌥⌅" "⇥
"⇥"⌅⌥ ⌦⌅$ ⌃⌦!%
!⇧" ⌃⌦⌅"!⇥⇧
⌅⌦ ⌅
!⇧" ⌃⌦⌅"
⇠✏⇠⇡⇢ ⌫⇡&
⌫'( ⇡⇠⇡
⇥ ⇧ ⌃
⇠⇡⇠✓ ⌫⇡&
⌫'( ⇡⇠⇡
⇧ ⌃
⇠⇡⇠✓ )⌫✓⇠✏⇠⇡⇢ )⌫✓
*+ , + + ,
*+ ,
+
+ ,
⌅⌃
✏
*+ -
+
+ -
+ .
/ 0
/ ,
⇣⇤ ⌅⌃
⌘
⇧
✓
⇥⇤ ⌅⇧⌃ ⌥ ⌦↵ ↵ ✏ ⌃ ⇣↵⌘✓↵◆  ⌫⇠⇠
•  In	D8	project,	u>liza>on	of	EFD	and	CFD	methods	goes	beyond	cross-check	&	valida>on.	
	
•  The	methods	also	complement	each	other:	CFD	facilitates	the	duty	of	EFD	and	vice	versa.	
•  Ul>mately,	this	interplay	between	the	CFD	and	EFD	shortens	the	design	cycle	and	reduces	tes>ng	costs.		
↵ ⇥⌃ ⌃ ⌅✏ ⌅⇤ ⇣⌘⇥✓
⇥ ✏⇣⇧⌃ ✏⌅⌘ ⇣✓ ⇣⇧⌃ ✓⇥ ◆  ⌦↵ ⌦ ⌥✓ ↵
⇠⌅  ↵⌅⇣✓ ◆ ⇥ ⌅⇡ ⇣◆ ⇣⇧⇥ ↵⌅⇢⇥⇣ ⇧ ✏⇣⇥ ✏⇣⇧⌃ ✏⌅⌘
 ⌫⇠⇠
Acknowledgements:	Thanks	to	MIT	team	(Edward	Greitzer,	Mark	Drela,	Alejandra	Uranga,	Arthur	Huang	and	
David	Hall)	for	technical	discussions	and	many	of	the	material	presented	here.	Compu>ng	resources	for	CFD	
simula>ons	were	provided	by	NASA	Advanced	Supercompu>ng	Division	at	NASA	Ames	Research	Center.	
This	work	is	funded	by	NASA	AATT	(Advanced	Air	Transport	Technologies)	Project

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