- 1. Chapter 3 Materials for supersonic civil transport aircraft
Yann Barbaux and Jacques Cinquin Introduction The consequences of
the drastic economical and technical requirements for future
supersonic civil transport [1] on the materials selection for the
dierent parts of the aircraft structure have been detailed and
discussed elsewhere [2]. As a result, Aerospatiale, BAe and DASA
decided to increase their eort on materials studies and to launch
specic research programmes on aluminium alloys and carbon bre
reinforced polymers (CFRPs). Major research programmes were
initiated on aluminium alloys in 1992 [3] and on organic matrix
composites in 1994 [4]. Aluminium alloys The work programme of
recent research was divided into two main tasks, corresponding to
the study of the two factors assumed to inuence directly the creep
resistance and the thermal stability of metals: . Task 1: selection
of the main precipitation system . Task 2: optimization of the
chemical composition and of the process para- meters. The critical
analysis of existing data resulted in the selection of 33 chemical
compositions, from the four alloy systems given in table 3.1. These
alloys were direct chill (DC) cast and rolled down to 14 mm thick
plates and 1.6 mm thick sheets on laboratory equipment at DERA,
British Aluminium and Pechiney. They were then tested for creep,
thermal stability and corro- sion. Based on the results obtained on
these alloys, a selection of 14 dierentCopyright 2001 IOP
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2. Table 3.1. Selected alloy systems. Alloy system Main
precipitation system Al-Cu (2001 type)0 (Al2 Cu) Al-Cu-Mg (2024 or
2618 type) S 0 (Al2 CuMg) Al-Mg-Si-Cu (6013 type)0 (Al5 Cu2 Mg8 Si7
) 3. 0 (Mg2 Si) Al-Li-Cu-Mg0 (Al3 Li)T1 (Al2 CuLi) compositions
from the S 0 and 0 4. 0 precipitation systems was made on which the
eect of minor alloying element and thermo-mechanical process
variations was studied. Results obtained in this project [5] were
very satisfactory: all the alloys tested presented a creep
behaviour and a fracture toughness much improved as compared with
CM003 alloy (enhanced 2618), which was, at that time, the best
reference in terms of creep/damage tolerance compromise. This is
illustrated by gure 3.1 and table 3.2, which present respectively
creep results in accelerated conditions and fracture toughnesses on
compact tension specimens of three of the alloys (labelled A1, C1
and D6), in comparison with creep results from CM003 and fracture
toughness results from 2024. Creep life times were extended by a
factor of up to seven under dierent 5CREEP ELONGATION (%) STRESS:
250 MPa TEMPERATURE: 175C 4A1C1D6CM003 3 2 1 0 050 100 150
200250TIME (HOURS) Figure 3.1. Creep curves at 1758C/250
MPa.Copyright 2001 IOP Publishing Ltd 5. Table 3.2. Fracture
toughness from R-curves on 400 mm widecompact tension specimens.
AlloyKc (MPa/m2 )Kc0 (MPa/m2 ) A1 T6 (mod. 2650)125 90 C1 T6 (mod.
6056)160110 D6 T6 (Al-Cu-Mg-Ag)158110 2024 T3130 90 creep test
conditions (including 1508C/250 MPa) compared with CM003, and
fracture toughness values from R-curves were equal to or better
than the damage tolerant 2024 T3 reference. Industrial sheets and
plates from the two most promising compositions, a modied version
of 2650 Al-2%Cu- Mg alloy and an optimized version of 6056 alloy,
entered an exhaustive evaluation programme in 1997, and the results
conrm the improvement in creep behaviour over CM003, although the
benet is reduced compared with the laboratory tests.In parallel
with the development of improved alloys, Aerospatiale has also
started studies on the interactions between creep and fatigue on
notched coupon specimens and on specimens representative of
technological details such as pocket recess or assemblies. These
studies are based on the develop- ment of two parallel methods: . a
modelling approach combining thermo-elasto-plastic nite elements
and physical/metallurgical prediction of creep damage . an
experimental approach with the development of specic test equipment
capable of reproducing close to real exposures on technological
specimens. The results obtained show a slight detrimental eect of
5000 and 10 000 hours of creep exposure at 1308C on the fatigue
behaviour of notched specimens in 2650 alloy. Carbon bre reinforced
polymers It has already been published [2] that composite materials
with carbon bres and polymeric matrices are candidates to achieve
the required weight savings on future supersonic civil transport.
The main requirements are acceptable properties regarding subsonic
ight specications (i.e. damage tolerance), and thermal stability in
supersonic ight conditions. Dierent types of matrices are under
investigation for Mach 2.05 applications with IM or HR bres,
including second generation epoxy, cyanate-based, thermoplastic and
bismaleimides, as shown in table 3.3. The work programme was
divided into two main research areas:Copyright 2001 IOP Publishing
Ltd 6. Table 3.3. Candidate polymer matrices for carbon bre
reinforced polymers.State of knowledge Second generation
epoxyWell-known processExpected service temperature: 1208C Cyanate
based systemsProcess similar to epoxy systemNew products on the
marketExpected service temperature: 1508C Thermo-plastic Potential
hot forming processExpected service temperature: 1808C
BismaleimidesProcessing generally with post-curingExpected service
temperature: 1808CLow damage tolerance compared with 2nd generation
epoxy . the inuence of long-term thermal ageing on carbon bre
reinforced poly- mer physical and mechanical properties . the
long-term behaviour of carbon bre reinforced polymers under complex
thermo-mechanical loading. The inuence of thermal ageing has been
studied by isothermal ageing up to 4000 hours at dierent
temperatures from 1008C to 1808C, and by thermal cycling over the
ranges 508C to 1208C or 1808C for up to 1000 cycles. The cumulative
time at the maximum temperature for 1000 thermal cycles is
equivalent to 4000 hours under isothermal conditions. Dierent
properties have been investigated after these thermal ageing
exposures, such as lled hole compression, compression after impact,
glass transition temperature and microstructure. The inuence of
thermal ageing on the mechanical properties can be related to the
degree of curing of the matrix, and also to the chemical type of
the matrix. Figures 3.2 and 3.3 clearly show a post-cure eect on
the second generation epoxy, not fully transformed during the
initial curing. For the cyanate system, there is a real mechanical
property degradation when isothermal ageing is performed above
1608C. Figures 3.3 and 3.4 show that the mechanical property
degradation, or the post-cure eect, appears during the rst 1000
hours of ageing. These rst tests were performed at a higher
temperature than the service tem- perature, corresponding to Mach
2.05, in order to obtain in a short time the rst indications of
thermal ageing response for the dierent families of matrix.Another
important point is the inuence of thermal ageing on the damage
tolerance properties of the carbon bre reinforced polymers. The
results, shown in gure 3.5, have been obtained with compression
after impact (CAI) tests performed on bismaleimide composites.
Dierent para- meters have been investigated such as the duration of
ageing up to 4000Copyright 2001 IOP Publishing Ltd 7. Figure 3.2.
Filled hole compression after 2000 hours of isothermal ageing.
hours, the thermal cycling eect, the position of the impact (before
or after thermal ageing), and the temperature of ageing, 1208C or
1808C. These results indicate that the position of the impact
before or after the thermal ageing is an important parameter. If
the maximum temperature is 1208C, Figure 3.3. Glass transition
temperature versus time of ageing at 1808C.Copyright 2001 IOP
Publishing Ltd 8. Figure 3.4. Filled hole compression at 1808C
after isothermal ageing at 1808C. no degradation of properties is
observed up to 4000 hours of ageing or 1000 cycles. In these
conditions, no oxidation or microcracks are observed in the
composite materials. If the temperature of ageing is 1808C, under
isothermal conditions we do observe oxidation on the exposed edges
of the samples, as shown in gure 3.6(a). If the ageing is done
under thermal cycling conditions Figure 3.5. Compression after
impact test performed after thermal ageing on bismaleimide
composite.Copyright 2001 IOP Publishing Ltd 9. (a) (b) Figure 3.6.
Micrographic observation of a bismaleimide composite. (a) 4000
hours at 1808C under isothermal conditions. (b) 1000 cycles with
Tmax 1808C and Tmin 508C. with Tmax 1808C and Tmin 508C, we do
observe microcracks inside the composite material, as shown in gure
3.6(b).Additionally to the study of the eect of thermal ageing,
Aerospatiale developed specic creep test procedures on 4584S
specimens to test the creep behaviour of various composite
materials. Figure 3.7 presents the creep behaviour of the dierent
candidate composites for supersonic aircraft.Aerospatiale is also
beginning a research programme to assess the long term behaviour of
carbon bre reinforced polymers under complex thermo- mechanical
loading. The typical ight spectrum for the future supersonic civil
transport in the hypothesis of Mach 2.05 is presented in gure 3.8.
This ight spectrum induces strong creepfatiguethermal cycling
interactions. In order to test the degrading eects of coldhot
thermal cycling and low frequency fatigue cycling compared with
classical creep testing, on the residual proper- ties of the
composites after exposure, three specic accelerated thermo-
mechanical cycling conditions were dened, as shown in gure 3.9.
Each cycling type corresponds to 10 000 hours at 1208C. Compared
with typical ight conditions, the maximum temperature has been
increased by 208C and the maximum stress has been doubled for test
acceleration.A specic testing apparatus has been developed to
perform the three cycling spectra (gure 3.9). These cycling spectra
have been applied to three composite systems with the same bre: one
bismaleimide, one cyanateCopyright 2001 IOP Publishing Ltd 10.
Figure 3.7. Creep testing on 4584S laminates at 1208C, 70 MPa. and
one epoxy. First results are available on the cyanate matrix
composite. Table 3.4 presents residual properties after cycling
exposure on quasi- isotropic open hole tension (OHT) and lled hole
compression (FHC) specimens. These results tend to show that
coldhot thermal cycling deter- mines the composite compression
properties. The duration of exposure is limited compared with what
has to be justied (at least 60 000 hours). This means that
long-term tests have to be carried out and special care has to be
paid to the development of reliable models, able to predict
long-term behaviour from short-term accelerated tests. Figure 3.8.
Typical ight spectrum of supersonic aircraft.Copyright 2001 IOP
Publishing Ltd 11. Temp (C) 120 Stress Time 0,3 S010000 hrsTimeType
1 TempCold-Hot thermal (C)cycle120x 2500 Temp0,5 h4 hrs0,5
h(C)120Time - 55StressStress Time0,3 S00,3 S0 x 2500 4 hrsTime
TimeType 2 Type 3 Figure 3.9. Creep facilities with thermal cycling
chamber (558C 2008C). Table 3.4. Eect of cycling on the residual
proper-ties of cyanate matrix composites.Loss of stress(% of
initial stress)FHC OHT Type 1 (creep)3.9 2 Type 2 (thermal cycle)
10.4 2.9 Type 3 (fatigue)5.7 1.9Copyright 2001 IOP Publishing Ltd
12. Summary The pre-design studies conducted at Aerospatiale, BAe
and DASA indicate that, because of the drastic economical and
technical requirements dened for future supersonic civil transport
aircraft, an important share of the struc- ture of this aircraft
will have to be made out of polymeric matrix composites and
advanced lightweight aluminium alloys.For the aluminium alloys,
studies were oriented in two directions: . the development of
improved alloys . the analysis of the behaviour of aluminium
components in creepfatigue interaction conditions. Concerning the
rst topic, recent research has resulted in the development of new
low density alloys, derived from 2650 and 6056 families, with much
better creep resistance than the 2618A Concorde alloy, combined
with a frac- ture toughness better than the reference 2024 T3
subsonic alloy. For the carbon bre reinforced polymers, the test
procedure for evaluating the damaging of these materials in real
cycling conditions has been established, and pilot test equipment
has been designed and built. Key points that will need to be
studied in more detail have been identied, such as the inuence of
thermal ageing on the damage tolerance properties of the composite
materials and the creepfatiguethermal ageing interactions.
References [1] Swadling S J 1993 J. de Physique IV 3 1130 [2]
Barbaux Y et al 1994 Proceedings of EAC 94 Toulouse 2527 October,
pp 433439 [3] Patri G and Frison G 1994 Revue Aerospatiale 108 [4]
Barbaux Y and Polmear I J 1995 Proceedings of PICAST 2-AAC 6
Melbourne 2023 March 2 pp 515520 [5] Barbaux Y et al 1995
Proceedings of EUROMAT 95 Padova, SeptemberCopyright 2001 IOP
Publishing Ltd