Joining of CrNi steel and AlMg alloy without interlayers/CrNi-terase ja AlMg-sulami vahekihita difusioonkeevitus.
Dahms, Steffen ; Kulu, Priit ; Veinthal, Renno 等
1. INTRODUCTION
The manufacture and application of innovative dissimilar material
joints with specific characteristics require continuous development of
the joining technology. Presently, however, there is a predominance of
similar material joints. Comprehensive investigations on the
substance-to-substance joining of dissimilar materials with dissimilar
characteristics still have to be conducted.
Diffusion joining in the solid state was used as a joining
technology for dissimilar material joints. The joints were created with
and without interlayer materials below the melting temperature of the
joining partners.
Composite constructions have become a focal point in the
optimization of lightweight constructions regarding their stability, due
to the fact that in this way the characteristics of dissimilar materials
can be optimally exploited. The joining of dissimilar materials, e.g.
CrNi steels and AlMg alloys poses a special challenge in the field of
joining technology. The following requirements on the joining are to be
met:
--manufacture of substance-to-substance joints,
--reduction of and avoiding the creation of intermetallic phases,
--balancing of different melting temperatures,
--reduction and absorption of stress in the joint.
A distinction between similar and dissimilar materials is made in
order to characterize joined components. Similar materials are
structural steels with different yield stresses. Dissimilar materials
are, e.g., steels with light or heavy metals such as the combination of
steel and aluminium [1,2].
Diffusion joining is currently a very promising joining procedure
to manufacture dissimilar material joints without creating a mutual
melt. That is why the creation of intermetallic phases from the melt can
be prevented within dissimilar material joints. Such phases influence
the strength in the material joint [3j. Besides intermetallic phases,
also various material properties have an impact on the joint strength.
With dissimilar material joints these are:
--thermal expansion,
--heat conductivity,
--melting temperature,
--porosity and hardness.
One important criterion in the diffusion joining of dissimilar
materials is the change of properties of the materials in the joining
zone. Gradual changes to the properties occur on boundary surfaces. They
strongly depend on the diffusion joining parameters (joining
temperature, joining force and joining time). Figure 1a shows the change
of properties of dissimilar materials before the diffusion joining
process. After the joining process the changes are no longer sudden.
Examinations have shown that the properties change gradually,
exponentially or parabolically (Fig. 1b). The creation of a diffusion
zone leads to a material concentration balancing depending on the
joining parameters. This results in a partial balancing of property
changes in dissimilar material joints. Stress in the joint is reduced,
which leads to a higher joint strength [4,5j.
Dissimilar material joints of ceramics, metals and monocrystals
with and without interlayers are studied in [6-8]. Dissimilar material
joints of CrNi steel and AlMg alloy are under examination for technical
applications in the field of nuclear technology. The joining zone must
not be influenced by additional alloy elements in order to guarantee a
high safety standard. A substance-to-substance joining without
interlayers is necessary in order to prevent material failure in the
joining zone. Diffusion welding provides an innovative approach where
the joint is created through solid state diffusion as well as
dislocations in the crystal structure. Joining in the solid state and
optimization of joining parameters enables the achievement of joint
strength and ageing stability similar to the base material. This is,
however, a precondition in order to meet the high quality requirements
for applications in the aerospace industry or for material joints in
nuclear technology.
2. EXPERIMENTAL
The material properties are essential for the definition of the
process parameters in the diffusion joining in order to manufacture
high-quality dissimilar material joints (Table 1).
The lowest melting temperature of the joining component AlMg3
(below 620[degrees]C) defines the joining temperature. Matching face
centred cubic (fcc) space lattices are advantageous in order to activate
diffusion processes in real crystals along dislocations or grain
boundaries. The diffusion is isotropic for joining partners with cubic
elementary cells irrespective of their orientation. Additionally,
vacancy mechanism and dislocation density are the primary joining
mechanisms with metals.
The number of primary slip systems in the face-centred cubic
lattice (Fig. 2) is limited to 12 in one elementary cell. Each of the 4
slip planes has 3 slip directions, along which the stress, necessary for
a deformation, is the lowest. Slip planes are those with the highest
number of atoms. Elastic as well as plastic deformations initially occur
along these slip directions. Thus a material, which is under pressure
during the diffusion process, is elastically deformed along these
directions. However, the deformation ability is limited by the size of
the interstitials.
[FIGURE 2 OMITTED]
A thermal process has to take place in order to initiate diffusion
processes between the joining partners. The joining force triggers a
forced diffusion. The diffusion in metals is a process where atoms are
moved due to concentration differences with a tendency to balance them.
The joining experiments were carried out in a high temperature
graphite furnace with integrated press (Fig. 3). The dimensions of the
test pieces were 20 x 20 x 5 mm, which corresponds to a joining surface
of 400 [mm.sup.2]. A joining force of 2000 N equates to a joining
pressure of 5 MPa. The heating and cooling rates were 10 K x
[min.sup.-1] in a pre-vacuum atmosphere at about [10.sup.-1] mbar.
Joining time and temperature were varied (Table 2). Solid dissimilar
material joints could be manufactured as a result of the joining
experiments. The joint strength and form stability strongly depended on
the joining temperature and joining force due to the low hot compressive
strength of the AlMg alloy.
[FIGURE 3 OMITTED]
3. RESULTS AND DISCUSSION
Expansion and contraction of the joining parts in a thermal process
define the state of stress in the joint. Metals can absorb stress due to
their ductile behaviour.
Examination on dissimilar material joints showed that, depending on
the material behaviour, different expansions of up to [DELTA][alpha] =
10 x [10.sup.-6] [K.sup.-1] can be compensated. Figure 4 illustrates the
expansion progression of the dissimilar material joint of CrNi steel and
AlMg alloy from room temperature to joining temperature. Expansion
coefficients CTE were measured by means of an Absolut-Dilatometer
Linseis L 75/20 under air with a heating and cooling rate of 5 K x
[min.sup.-1]. With the above-mentioned material joint the expansion
coefficients differ from 6 to 8 x [10.sup.-6] [K.sup.-1] up to the
joining temperature range. No hysteresis effects in the expansion
behaviour could be observed after the measurements. Depending on the
temperature, expansion and contraction are almost constant, which
permits to join the surfaces and minimizes the creation of cracks.
[FIGURE 4 OMITTED]
The surfaces of the joining parts or their atoms have to come as
close as 10-6 to 10-7 mm in order to achieve atomic interaction. In
reality this closeness is impeded by microroughnesses, form
imperfections and layers of dirt and/or adsorption layers. All types of
form deviations, which restrict the number of possible bonds in the
joining zone, are reduced in the activation phase, i.e., physical
interactions occur, in order to manufacture a high-quality joint. This
can be achieved by surface pre-treatment or cleaning. At the same time
the surface is extremely altered depending on the degree of deformation,
which also affects pollution layers on the surface as well as layers
near the surface. The procedures are very complex and the joining
parameters are mutually linked.
The joining surfaces were mechanically ground and polished with a
diamond paste in order to meet these requirements. The surface analysis
was carried out by means of an autofocus sensor AF16, made by OPM GmbH
Karlsruhe, coupled with an optical measuring system and it was used for
optical length and profile measurement (topography illustration).
Manufacturing quality and final state of the joining surfaces were
measured (Table 3).
The mean roughness Ra and the arithmetical mean deviation of the
filtered roughness profile over the measurement range were analysed,
resulting in [R.sub.a] [less than or equal to] 0.225 gym, which meets
the surface requirements for the diffusion joining of metals.
The joining and diffusion zones were characterized by means of SEM
examinations. All the tests showed the same characteristic. Closed and
flawless diffusion zones were achieved. Figure 5 shows the joint at a
temperature of 500[degrees]C and a joining time of 12 h. The material
structure of the CrNi steel is compact, the structure of the AlMg alloy,
however, is porous. The surfaces were homogeneously joined and a
diffusion zone can be seen. The results of the joining tests showed no
cracks parallel to the joining zone due to the different expansion
behaviour. The ductile behaviour of the joining partners compensated the
stress in the joining zone.
EDX-analysis in the diffusion zone or in neighbouring areas enables
a qualitative examination of the diffusion behaviour of dissimilar
material joints. Figure 6 illustrates the element distribution over the
joining zone. The analysis showed that the concentration difference of
the alloy elements forms a step in the measurement area. The left side
of the diagram shows the CrNi steel with Fe, Cr, Si, Ni and a low Mn
proportion. The right side of the diagram shows the AlMg alloy with high
Al and low Mg proportion. The concentrations on the left (CrNi steel
with alloy elements) are nearly constant. The concentration progressions
from maximum to minimum exhibit a diffusion range x of over 100
[micro]m.
Distribution of the joining parameters helps to optimize the
joining process and to meet the requirements of the practice. The
development of the diffusion areas x of the dissimilar material joints
depends on the joining pressure, joining time and joining temperature,
as shown in Fig. 7. The diffusion distance depends also on the joining
time and the joining force. The joint stability cannot be concluded from
the width of the diffusion zone and has yet to be proved in stability
tests.
The microsection of the diffusion joined dissimilar material joint,
shown in Fig. 8, shows the indents in the joining materials and in the
joining zone. The Vickers hardness HV 0.1 of the dissimilar material
joint was determined with the joining parameters T = 500[degrees]C, t=
12 h by means of a small load hardness measuring device Zwick in
compliance with EN ISO 6507-1.
[FIGURE 6 OMITTED]
[FIGURE 7 OMITTED]
[FIGURE 8 OMITTED]
In diffusion joining the material is stressed through a thermal
process. This can either lead to an increase or decrease of the
hardness, which affects the joint strength. Prior to the experiments the
initial hardnesses were determined (CrNi steel 178 HV 10, AlMg alloy 60
HV 10) on thermally non-stressed joining partners. Figure 9 shows the
hardness progression of the dissimilar material joint after the
diffusion joining.
The examinations showed that the hardness in the joining materials
is nearly constant. The hardness of the CrNi steel increases sharply
near the joining zone up to 250 HV0.1. The Vickers hardness forms a step
in the joining zone. This hardness increase is a sign of intermetallic
phases in the joining zone. The thickness of these phases strongly
depends on the joining time (Fig. 10). The intermetallic phase is about
20 [micro]m thick. On the steel side it is mainly [Fe.sub.2][A1.sub.5]
and on the aluminium side Fe[Al.sub.3]. The intermetallic phase
Fe[Al.sub.3] forms above 350[degrees]C, has an aluminium concentration
between 74-76 atom% and a complex monoclinic, bodycentred cubic
structure. Furthermore, this phase is characterized by a columnar
crystal shape. In contrast, the aluminium concentration in the
intermetallic phase [Fe.sub.2][Al.sub.5] lies between 69-73 atom%. For
comparison, the aluminium concentration in the joining zone of the
sample, which was joined at 500[degrees]C, was ca 59 atom%.
[FIGURE 9 OMITTED]
[FIGURE 10 OMITTED]
[FIGURE 11 OMITTED]
Figure 11 shows a broken joint after a stability test. An oxide
layer, based on aluminium oxide, could be detected on the surfaces. The
residual oxygen concentration in the pre-vacuum of 10-1 mbar caused the
creation of the oxide layer, which was not broken due to the low joining
temperatures [5]. These oxide layers additionally function as diffusion
barriers and extend the joining time.
4. CONCLUSIONS
The examinations proved that through diffusion joining
interlayer-free and crack-free dissimilar material joints can be
manufactured between CrNi steel (X5CrNi18-10) and AlMg alloy
([AlMg.sub.3]) at joining temperatures lower than 600[degrees]C. Ground
and polished surfaces are a precondition for an optimal joining process.
Different hardness and expansion behaviour (different expansion
coefficients) of the joining parts enabled the manufacture of
homogeneous and mechanically stable joints. Hardness and expansion
behaviour are closely linked with each other and they are essential for
achieving a low-tension joint. The creation and the characteristics of
the joining zone depend on the Mg and Al content as well as on the alloy
elements of the CrNi steel. The joining parameters (temperature, time
and joining force) show functional interdependence, which results in the
creation of different diffusion areas. The process parameters have a
direct influence on the creation of intermetallic phases in the joining
zone. Currently no conclusions can be made on the creation of
intermetallic phases in a system with a variety of elements like in the
examined case. That is why the examinations on the creation of
intermetallic phases were restricted mainly on the system Fe-Al. The
creation of intermetallic phases in the Fe-Al system is based on the
almost absolute insolubility of iron and aluminium in the solid state. A
short heat impact stimulates mainly the formation of intermetallic
phases [Fe.sub.2][Al.sub.5] and Fe[Al.sub.3].
Examinations on intermetallic Al-Fe phases as well as the inclusion
of further alloy elements and the prevention of an oxide layer on the
Al[Mg.sub.3] will be subject of future research.
ACKNOWLEDGEMENTS
The described results are extracts from an ongoing research project
within the frame of the BMWi programme INNO-WATT--FuE-Projekt Reg.
VF080016 "Diffusion joining of ceramics" and FuE-Projekt Reg.
IWO91046 "Verfahrensentwicklung zum Diffusionsschweissen von
Werkstoffen mit unterschiedlichen Eigenschaftsprofilen", Germany.
doi: 10.3176/eng.2010.4.03
REFERENCES
[1.] Pohle, C. Schweissen von Werkstoffkombinationen. DVS-Verlag,
Dusseldorf, 1999.
[2.] Broda, T., Herrmann, J. and Uhlemann, M. Fugetechnologien fur
Mischverbindungen durch Lotapplikation mittels Ultraschallschweissen.
DVS-Berichte, Band 2009 "Die Verbindungs-spezialisten
Tagungsband". Verlag DVS Media GmbH, 206-212.
[3.] Wilden, J. and Bergmann, J.-P. Herstellung von Titan-Aluminium
and Titan-Stahl-Verbindungen durch Diffusionsschweissen. Mitteilung aus
der Technischen Universitat Ilmenau, Fachgebiet Fertigungstechnik,
Schweien and Schneiden, 2004, 56, 199-207.
[4.] Dahms, S., Gemse, F., Basler, U., Martin, H.-P. and Triebert,
A. Diffusion joining of silicon nitride ceramics. Estonian J. Eng.,
2009, 15, 301-308.
[5.] Dahms, S., Gemse, F. and Basle-, U. Diffusionsschweissen--ein
innovatives Fugeverfahren fur Werkstoffverbunde mit unterschiedlichen
Eigenschaftsprofilen. DVS-Berichte, Band 2009 "Die
Verbindungsspezialisten Tagungsband". Verlag DVS Media GmbH, 54-59.
[6.] Pietrzak, K., Kalinski, D. and Chmielewski, M. Interlayer of
A1203-Cr functionally graded material for reduction of thermal stresses
in alumina-heat resisting steel joints. J. Europ. Ceram. Soc., 2007, 27,
1281-1286.
[7.] Travessa, D., Ferrante, M. and den Ouden, G. Diffusion bonding
of aluminium oxide to stainless steel using stress relief interlayers.
In Materials Science and Engineering. Elsevier Science B.V., 2002,
A337,287-296.
[8.] Zeng, L., Case, E. D. and Crimp, M. A. The interfacial
microstructure of joined single crystal and polycrystalline alumina. In
Materials Science and Engineering. Elsevier Science B.V., 2003,
A360,228-236.
[9.] Geguzin, J. E. Grundzuge der Diffusion in Kristallen. VEB
Deutscher Verlag fur Grundstoff-industrie, Leipzig, 1977.
Steffen Dahms (a), Priit Kulu (b), Renno Veinthal (b), and Ursula
Basler (a)
(a) Gunter-Kohler-Institut fur Fugetechnik and Werkstoffprufung
GmbH, Otto-Schott Str. 13, 07745 Jena, Germany; {sdahms,
ubasler}@ifw-jena.de
(b) Tallinn University of Technology, Department of Materials
Engineering, Ehitajate tee 5, 19086 Tallinn, Estonia; {priit.kulu,
renno.veinthal}@ttu.ee
Received 26 April 2010, in revised form 17 September 2010
Table 1. Thermophysical properties
Parameter CrNi steel AlMg alloy
X5CrNi18-10 AlMg3
Density, g/[cm.sup.3] 7.93 2.7
Space lattice fcc fcc
Melting point, [degrees]C 1400-1455 620
Thermal expansion at 18 x [10.sup.-6] 23.5 x [10.sup.-6]
20-100[degrees]C, [K.sup.-1]
Heat conductivity at RT, 16.3 at RT 125
[Wm.sup.-1] [K.sup.-1]
Vickers hardness, HV 175 75
Modulus of Elasticity, GPa 190-210 71
Tensile strength, MPa 460-1100 300-450
Table 2. Experimental joining parameters of the dissimilar
material joint CrNi steel with AlMg alloy
No. of the Joining temperature Joining time t, Joining force F,
experiment T, [degrees]C h N
1 450 2 2000
2 500 2 2000
3 550 2 2000
4 450 12 1000
5 500 12 1000
6 550 12 1000
Table 3. Surface characterization of the dissimilar
material joint of CrNi steel with AlMg alloy
Surface CrNi steel
parameters
Manufacturing quality Final state
[R.sub.a], [micro]m 0.834 0.109
Surface AlMg alloy
parameters
Manufacturing quality Final state
[R.sub.a], [micro]m 0.298 0.225