Aeroelastic Characteristics Analysis of Helicopter Rotor s ...
m CR7J*G ,uc- THE AEROELASTIC CHARACTERISTICS OF THE ...
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m C R 7 J * G ' ,uc- THE AEROELASTIC CHARACTERISTICS
LAUNCH VEHICLE OF THE f lAlURH4B f $1-201
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Q 1 III i 1 R c I
M-37-65-2
THE AEROELASTIC CHARACTERISTICS OF THE SATURN-IB
SA-201 LAUNCH VEHICLE
August 1965
Aero-Hydrodynamics
Checked By: Lars-Eric Ericsson Flight Technology
APPROVED: M. Tucker, Manager Flibt Technology
Prepared Under Contract NAS €3-11238 for
Aerodynamic Division Aero-Astrodynamics Laboratory
George C. Marshall Space Flight Center National Aeronautics and Space Administration
Huntsville, Alabama
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M-37-65-2 r
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SUMMARY
The flow environment surrounding the Saturn IB SA-201 vehicle is dominated by
regions of separaied fiow in the transonic ?via& number range. The highly nm-hear
loadings resulting from flow separation coupled with the modal deflections of a long
flexible vehicle as the SA-201 have a dominant influence upon vehicle dynamics. A
quasi-steady method requiring an experimental static load distribution a s inplt has been used in analysis of the SA-201 vehicle to obtain the aerodynamic damping for the first three bendmg modes. The analytical results indicate that the SA-201 vehicle is aerodynamically damped over the critical Mach number range (0.8 5 M 5 2.0) and
therefore is expected to be damped over the entire ascent Mach number range.
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M-37-65-2
CONTENTS
1 1
Section
SUMMARY
ILLUSTRATIONS
NOTATION
1 INTRODUCTION
2 SATUFtN-IB SA-201 ANALYSIS
2.1 Static Aerodynamic Analysis 2.2 Aerodynamic Damping Analysis
8 c 3 CONCLUSIONS
4 REFERENCES
Appendix
iii
vi i
ix 1- 1
2- 1 2- 1 2- 1
3- 1
4- 1
A DOCUMENTATION OF SA-201 LUMPED LOADS
I A-1
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ILLUSTRATIONS
Figure
2-1
2-3
2-3
2-4
A-1
A-2
A-3
A-3
A-4
A-5
A-6
A-7
SA-201 Configuration
Cexnprisco ef S4-201 Integrated Lumped Lwds with Force Dzta Results at a = 0
Comparison of Saturn-lB and SA-201 Damping Characteristics atcr=O SA-201 Aerodynamic Damping
SA-201, Definition of Lumped Normal Force Vectors
SA-201 Local and Forebody-Dependent Command Module Loads atcr=O SA-201 Local Normal Force Derivatives at (Y = 0
SA-201 Local Normal Force Derivatives at Q! = 0 (Cont. )
SA-201 Induced Normal Force Derivatives a t (Y = 0
SA-201 Lumped Load Centers of Pressure at a = 0
SA-201 Local and Induced Command Module and Flare Axial Force Moment Derivatives a t a = 0
SA-201 Separated-Flow Velocity Ratios a t (Y = 0
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2-3
2-4
2-5
2-6
A-2
A-3
A-4
A-5
A-6
A-7
A-9
A- 10
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I
C
D~~~ M
m
P
4 S
N
CY
P
W
U U
P
-
e
~
M-37-65-2
NOTATION
2 force coefficient = Force/pm (um/2)S
Mach number
generalized mass (kg - sec2/m) 2 pressure @g/m )
dynamic pressure (kg/m2)
-caFnvnllc.cI L CLCl CUCU I€ag?il (6.5278 El for Saturii-fB w-201)
reference area = ?rD &F/4 (m2) angle of attack (deg or radian)
density (kg-sec2/m4)
free-free bending frequency ( r a d i d s e c )
velocity (m/sec) average velocity (m/sec)
equivalent spike deflection angle (deg or radian)
rotation angle (deg o r radian)
Subscripts
m pitching moment (kg-m)
N normal force (kg) S separated flow 00 undishrbed flow
Super scripts
i induced, e. g. , AiCN = separation induced normal force coefficient
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33-37-65-2
Section 1
INTRODU C TION
The present study of the Saturn JB SA-201 vehicle has been conducted in support of the
&brirn Fiqg-am ii; py-j~id% & ~ @ g &zac&ris;%cs; f ~ r in&i~;id~si fQ$t cecf@Lrg-
tions as required. The resuits presented herem provide the damping cnaracreristics,
in percent of critical, for the Saturn E3 SA-201 launch vehicle. As is characteristic
of the Saturn IB series, SA-201 is a long flexible vehicle over which large regions of separated flow exist in the transonic Mach number range. The highly nonlinear aero-
dynamic loads resulting from flow separation are known to considerably influence the
damping characteristics of such vehicles. A quasi-steady analytical method, described
in Ref. 1, which includes the effects of separated flow has been applied in the present
study to determine the SA-201 damping. The following section, in two parts, describes
the static aerodynamic loads used in the quasi-steady analysis and contains a discussion
of the damping results for the SA-201 vehicle.
1-1
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I
Section 2
SATURN IB SA-201 ANALYSIS
2 . 1 STATIC AERODYNAMIC ANALYSIS
~~
M-37-65-2
I 1
A s is characteristic of the Saturn IB series vehicles, the Apouo payioaci is responsive
for the major effects of flow separation on the SA-201 vehicle. (See Fig. 2-1. ) The
escape-rocket wake represents the most prominent single region of flow separation
Furthermore, due to the large modal deflections occurring a t the forward portion of the
vehicle, the Apollo-payload has a significant influence on the vehicle damping. Subse-
quently, the analytic and ewr imen ta l effort was in great part directed toward obtaining
an accurate description of the loading over the Apollo-payload portion of the vehicle.
The static aerodynamic load characteristics for SA-201, presented in Appendix A, cor-
respond to the Saturn-IB characteristics presented in Ref. 2. A small difference in
length of the lunar excursion module, on the order of 2 .5 percent, has no measureable
effect on the static load characteristics and thus the inclusion of the results of the
Saturn-If3 analysis is expedient. Within the Saturn-IB analysis, pressure data were
correlated with segmented force data such that the magnitudes of the ill-defined negative
load peaks were varied until agreement with force data was achieved for both normal
force and center of pressure. Experimental data used in the analysis were obtained
from Refs. 3 through 16. Excellent agreement between summed, lumped force distribu-
tions and overall force data for SA-201 is shown in Fig. 2-2.
2 . 2 AERODYNAMIC DAMPING ANALYSIS
The damping derivatives obtained as a result of the quasi-steady analysis may be con-
fidently discussed by considering the geometric and elastic characteristics of the
vehicle in relation to the loadings generated by the surrounding flow. The static load
2-1
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M-37765-2
distribution provides a knowledge of the location and magnitude of the important non-
linear loads resulting from flow separation.
tics of the vehicle constitute the primary factors influencing the equivalent damping
distribution resulting from the quasi-steady analysis.
This coupled with the modal characteris-
The SA-201 damping, as in the case of the Saturn-IB of Ref. 2, is most heavily
influenced by the Apollo command module. occur for this portion of the vehicle. As seen in Fig. 2-3 the damping curves at Q! = 0' for Saturn-IB and SA-201 are very similar for all three bending modes. In
the first mode SA-201 exhibits slightly smaller command module deflections causing the damping to fall below that of the Saturn-ZB.
relate primarily to the smaller critical damping factor, -pUsoS/4wG , for the SA-201
vehicle.
were taken from Refs. 17 and 18. The results of the SA-201 analysis a re indicated in
Fig. 2-4 which presents the damping in percent of critical for 0, 4 and 8 degrees angle-
of-attack, In all cases SA-201 exhibits positive damping characteristics indicating
that the vehicle is dynamically stable.
Large loadings and large modal deflections
Second and third mode differences
The modal characteristics and trajectory information used in the analysis
2- 2
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1
-
1 2-3
M-37-6 5-2
T 4 0 cu
I s rl
I @a
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I- O
10
M -37 -65-2
REF. DIA. = 6.5278 h
0 FORCE DATA; REF. 12 A INTEGRATED LUMPED LOADS
1 I I I 1
1 I I I I 0.8 1 .o 1.2 1.4 1.6
MACH NUMBER 1.8 2.0
Fig. 2-2 Comparison of SA-201 Integrated Lumped Loads with Force Data Resul ts a t Q = O
2 -4
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! 1 I 1 '1
0.8
0.4
1.2
-
3RD BENDING MODE
-
0.E
0.4
z UJ 0.4 2 n w Y
-SATURN 1B
2ND BENDING MODE
Fig. 2-3 Comparison of Saturn 1B and SA-291 Damping aaracteristics at =O
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0.8
0.4
I 1 I I I
2ND BENDING MODE
0 I I I I I
0.8
0.4
0
3RD BENDING MODE -
-- - ---- -- 8 1 .o 1.2 1.4 1.6 1.8 2
MACH NUMBER
Fig. 2-4 SA-201 Aerodynamic Damping
2-6
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M-37-652
0
8
Section 3
CONCLUSIONS
The Saturn-IB SA-201 vehicle has been sludied using a quasi-steady analysis to deter-
mine he damping &;irackri&ics. i*esdts h-L&czte h\& M-201 is ~ ~ y & ~ ~ ~ ~ f i J v
damped over the critical Mach number range (. 8 5 M 5 2.0) for the first three bending
modes. It may be concluded that the vehicle will be damped throughout atmospheric
ascent.
3-1
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Section 4
REFERENCES
1. Lockheed Missi les & Space Company, Report on Saturn I - Apollo Unsteady Aerodynamics. by Lars-Eric Ericsson and J. Peter Reding, LMSC A650215, c,8&9~*~m.r&, cssf., FCt ; 1964 (E)
2. ----- , The Aeroelastic Characteristics of the Saturn IB and Saturn v Launch
Vehicles, by Iars-Eric Ericsson and J. Peter Reding, LMSC M-37-65-1, Sunnyvale, Calif., March 1965 (U)
3. NASA Ames Research Center, Turbulent Boundary-Layer Separation Induced by Flares on Cylinders at Zero Angle of Attack, by Donald M. Keuhn, NASA TR R-117, Moffett Field, Calif., 1961 (U)
4. Jet Propulsion Laboratory, California Institute of Technology, The Fluctuating Pressure Field in a Supersonic Turbulent Boundary Layer, by A. L. Kistler and W. S. Chin, TR 62-277, Pasadena, Calif., Aug 1962 (U)
Brown Engineering Company, Inc. , Wind Tunnel Investigation to Determine
Transonic Stabilitv Characteristics on a 0.8117 Percent Scale Model of the
5.
Saturn IB and V Upper Stages with Several Service Module Lengths and LEM
Adapter Angles, by W. Dewayne Radford, Tech Memo AA-8-64-1, Huntsville,
Ala, 3 Aug 1964 (U)
6. --__- , Wind Tunnel Investigation to Determine Transonic Stability Character-
istics on a 0.8117 Percent Scale Model of the Saturn IB and V Upper Stages
with Several Service Module Lengths and LEM Adapter Angles; Series II, by
W. Dewayne Radford, Tech Memo AA-11-64-9, Huntsville, Ala, 30 Nov 1964
(U)
7. The Boeing Company, Saturn V Upper Stages Pressure Distribution W/APS
Units Lonrritudinal Pressure Distribution and Local Normal Forces for Future
Studies in S-II and S-IVB Region of Separation (0.505% Scale), by J. Wright,
Project AD-5-63, 6 Apr 1964 (U)
4-1
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8.
9.
10.
11.
12.
13.
14.
15.
16.
M-37-65-2
NASA Marshall Space Flight Center, Wind Tunnel Investigation to Determine the
Effect of an Axial Rod in the LES Tower on the Static Longitudinal Stability
Characteristics of the Saturn IB Upper Stage Components, by William C. Pope,
J r . , MSFC T N AA-12-64-1, 3 Dec 1964 (U)
Chrysler Corporation, Space Division, Static Pressure and Normal Force Co-
efficient Distributions on the Saturn IB Launch and Aborted Launch Configura-
tions as Determined by Wind Tunnel Tests, by F. Chianese, J r . , TN-AE-63-12,
New Orleans, La, 30 Dec 1963 (U)
----_ , Results of a Wind Tunnel Investigation to Determine the Pressure and
Local Normal Force Distribution Over the Saturn IB Vehicle, by H. B. Reese,
TN-AE-63-3, New Orleans, La, 1 Aug 1963 (U)
----A , Unpublished Data for Wind Tunnel Tests Described in "Test Plan to
Determine the Stability and Axial Force Characteristics of the Saturn IB Launch
Vehicle and Components,
16 Nov 1964 (U)
by F. Chianese, TN-AE-64-61, New Orleans, La,
NASA Marshall Space Flight Center, Static Longitudinal Stability and Axial
Force Characteristics of the Saturn IB/Apollo Launch Vehicle as Determined
from Tests of a 1.32 Percent Scale Model at Langley Research Center, by
J. Johnson, MSFC Memo NR: R-AERO-AD-64-94, Huntsville, Ala, 15 Oct
1964 (U)
----- , Experimental Static Longitudinal Stability and Drag Characteristics of
the Saturn IB/Apollo Vehicle, by Robert E. Pitcock, MSFC Memo NR: R-AERO-
A-108-63, Huntsville, Ala, 7 Oct 1963 (U)
Cornel1 Aeronautical Laboratory, Transonic Wind Tunnel Tests of a .0175 Scale Pressure Model of the Saturn C-1, Block I1 Launch Vehicle, by D. L. Millikan,
Cornel1 Report No. HM-1510-V-8, Buffalo, N.Y., 1 Jul 1963 (u) Lockheed Missiles & Space Company, Preliminary Data Release for the Tran-
sonic Wind Tunnel Tests of the Saturn-Apollo 5% Model, by J. P. Reding, LMSC/802367 (TM 53-40-122), Sunnyvale, Calif., Nov 1962 (U)
----- , Preliminary Data Release for the Supersonic Wind Tunnel Tests of the
Saturn-Apollo 5% Model, by J. P. Reding, LMSC/802393 (TM 53-40-123),
Sunnyvale, Calif., Dec 1962 (U)
4-2
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8 8 I I 1 1 I
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17. NASA Marshall Space Flight Center, Bending Vibrations, First Stage Saturn IB, Vehicle 201, by George F. McDonough, Memo No. R-AERO-DD-14-65, Hunts- ville, Ala. , 19 Jan 1965 (U)
9 SA 201 Launch Vehicle Reference Trajectow, by J. W. Credn 18.
and W. M. GilES: TM)(-5.?242, H1l&gy:uea -Ala; , 1s !?+'Til 1965 (c.1
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M-37-65-2
Appendix A
DOCUMENTATION OF SA-201 LUMPED LOADS
The a = 0' , lumped load representation used in computing lhe SA-201 damping is documented in this ApLDendix, Figure A-1 r e l a t ~ e the hmped back tc &e g e r e r d fi-231 force &tzib-utiGrl. ZG*, 'leal iiid-uced lump& ar.e pi"ii& in Figs. A-1
through A-4, and their centers of pressure appear in Fig. A-5. Figure A-6 presents
the local and induced axial force moments on the command module and interstage
flares, and Fig. A-7 shows the velocity ratios for each of the separated regions.
A-1
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M-37-65-2 8 v, Z
VI k 0 JJ 0 Q) 3 Q) u k 0 Lc
a Q)
4 4 w 0
c 0 a d JJ
4 I 4
b;, *rl k
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1
I 8
Id I 1 I 1 I I 8
i .a
0.8 - 0.6 d
2 s Z U
E
0" 0.2
c a L &
Lu
Y 0 LL
2 5 0 c Z
4.2
-0.4
0.8
8 I
1 .o 1.2 1.4
k C H NUMBER 1.6 1.8 2.0
F i g . A-2 SA-201 Local and Forebody-Dependent Command Nodule Loads at 01 =O
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M-37-65-2 1
Z- V W 1.2
0.8
0.4
0
-0.4
-0.8 0.8 1 .o 1.2 1.4 1.6
MACH NUMBER
F i g . A - 3 SA-201 Local Normal Force Derivatives at a! =O
A-4
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1.8 2.0
1 8 II
8 1 1
1 1 1 1 1
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8 ~1 ,I I II 0 I 8 8 8 8 8 1 1 II S 1 il 8
M-37-65-2
4.0
3.6
3.2
2.8
2.4
2 .o
t
0.4
0
-0.4
0.8 1 .o 1.2 1.4 1.6
MACH NUMBER
F i g . A - 3 SA-201 Local Normal Force Derivatives at a =O 1 (cont.)
A-5
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0.4
0
v Z U 0
e -0.4
1.2
0.E
0.4
0
-0.4
-0.8
M-37-65-2
0.8 1 .o 1.2 1.4 1.6 1.8 2.0 MACH NUMBER
Fig. '4-4 SA-201 Induced N o r m a l Force Derivatives at Q! =O
A-G
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I I I 1 I 1 8 I 8 I u 1 8 I 1 8 I 8 8
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8 8 8
0 t 0 hl
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M-37-65-2 .
0 0 0 t f QD
t s: 0 9 t
13131H3A
Fig. A-5 SA-201 Lumped Load Centers of Pressure at * =O
A- 7
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1 1 I 8 I 8 I
M-37-65-2
0
-0.04
-0.08
-0.12 0
-0.04
-0.08
-0.12 0.8 1 .o 1.2 1.4 1.6 1.8 2 .o
M4CH NUMBER
Fig. A-5 SA-201 Local and Induced Comand Module and Flare Axial Force Moment Derivatives at cy =O
A-9
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0.8 1 .o
M-37-65-2
.2 1.4
MACH NUMBER
.6 1.8 2.0
Fig. 21-7 :';X-231 Separa ted-Flow Velocity Xatios at Q! =O
A-10
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t'
THE AEROELASTIC CHARACTERISTICS OF THE SATURN-1B
SA-202 LAUNCH VEHICLE
(Addendum to LMSC Report M-3'7-65-2)
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I - M-37-65-2
ADDENDUM
Analysis of the Saturn IB SA-202 Launch Vehicle
The results of the SA-202 damping analysis a re presented herein as an addendum to
LMSC report M-37-65-2.
structural characteristics of the Saturn IB vehicle between the flight vehicles SA-201
and SA-202, both the aerodynamic characteristics, presented in Appendix A, and the
structural characteristics documented in Ref. 17 and 18 for SA-201 vehicle apply as
well to the SA-202 vehicle. The launch trajectory data, secured from Ref. 19, has
been used in the calculation of the damping characteristics presented (in percent of
critical) in Fig. 1 of this addendum. It is observed from the quasi-steady method
that perturbations in launch trajectory will affect only the relative magnitude of the
damping and will not change the sign. This is confirmed by the results in Fig. 1-ADD
which predict positive damping for the SA-202 which is characteristically similar to the
SA-201.
atmospheric ascent.
Since there have been no changes in the configuration or the
It is concluded that the SA-202 vehicle will be dynamically stable throughout
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c *
1.2
0.8
M-37-65-2
Q = 00 o! = 4 O ----
-.- a = 8 O - *\ h
a G 8 t
I! !=
Y
Y
5 (3 Z
4 a n
0
1ST BENDING MODE
1 I I I I
O l I I I I I
0.8
O S 8 t
* -
2ND BENDING MODE
3RD BENDING MODE
0.8 1 .o 1.2 1.4 1.6
MACH NUMBER
1.8 2.0
*
Fig. 1-ADD SA-202 Aerodynamic Damping
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I 8 I 0 8 8 8 8 I 8 I 8 8 8 8
-~ ~~
M -37 -65-2
17. NASA Marshall Space Flight Center, Bending Vibrations, First Stage Saturn IB, Vehicle 201, by George F. McDonough, Memo No. R-AERO-DD-14-65, Hunts- ville, Ala. , 19 ;Tnn 1965 (U)
19. Marshall Space Flight Center/Manned Spacecraft Center, Joint MSFC/MSC SA-202/ AFRM 011 Reference Trajectory, Document No. 65-FMP-1, Huntsville, Ala. / Houston, Texas, 12 April 1965 (C)
4 -3
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