hitachi alloy cable
TRANSCRIPT
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HITACHI CABLE REVIEW No.25 (AUGUST 2006)18
50
55
60
65
0 0.1 0.2 0.3 0.4 0.5
Ratio of an addition element (mass%)
Electricalconductivity(%IACS)
Cr Mn
Mo
Ti
Li
Zr
Mg
Si
Cu
Ag
Fe
Zn, B
Ni
Sn, Cd
Sb
ABSTRACT: In recent years, lightweight aluminum alloy conductor with high elec-
trical conductivity characteristics is expected. Al-Fe-Zr alloy wire was developed in-
dustrially, although without having the tensile strength and elongation and spoiling
electrical conductivity characteristics.
The developed Aluminum alloy is expected to be applied in various fields such as the
automotive and electric wire for equipment.
Development of Aluminum Alloy Conductor with High ElectricalConductivity and Controlled Tensile Strength and Elongation
Toshiyuki Horikoshi*
Hiromitsu Kuroda*
Michiaki Shimizu**
Seigi Aoyama*
[1] INTRODUCTION
In recent years the automobile and electronics industries
have developed remarkably, and the demand for electric con-
ductive materials used for these applications is increasing com-
pared to the past. Conventionally, aluminum alloy has been ap-
plied mainly to the overhead conductor field taking advantage
of density of 1/3 and high conductivity of 2/3 in electrical con-
ductivity compared with copper. From the viewpoint of ef-
fective use of energy, the lightweight aluminum alloy conductor
is very effective, and possible advantages can also be expected
in the automotive and electronics industry. In order to use alu-
minum alloy electrical conductive material for industrial appli-
cations, we think that it is indispensable to develop an alloy that
responds also to recent social structural changes, such as envi-
ronmental issues and material requirements for recycling. The
present study introduces our recently developed aluminum al-
loy conductor with improved balance between tensile strength
and elongation properties that were demerits of the conventionalAluminum alloy while maintaining, at the same time, high con-
ductivity properties.
[2] DEVELOPMENT CONCEPT
2.1 The target properties of an aluminum alloy wire
In annealed pure Aluminum, the electrical conductivity is
about 64%IACS (International Annealed Copper Standard), ten-
sile strength reaches 100 MPa and elongation reaches about
20%.These properties conform to industrial use by annealing.
From an industrial point of view, for this type of aluminum wire,
electrical properties are not the only requirements, but also han-
dling and good balance of tensile strength and elongation are
important factors. In the present development, we set higher tar-
gets, with tensile strength higher than 30% and above 130MPa
compared with pare aluminum and elongation above 5% from
handling. We achieved these mechanical properties, reducing
the electrical conductivity decline as much as possible, and we
set the target for electrical conductivity above 58%IACS.
2.2 Examination of metal additions
Figure 1 shows changes in electrical conductivity after add-
ing various elements to pure aluminum.
Ni, Zn, Fe, Ag, Cu, Si, Mg, Zr, etc. can be considered pos-
sible additives in small quantities to reduce the decline in elec-
trical conductivity to a minimum.
Table 1 shows the influence on tensile strength after adding
various elements to pure aluminum. Although results show im-
provements on the strength of Cu and Fe, aluminum is used in
many cases with steel material, and the need for recycling
should be taken into consideration. Under these considerations
we excluded Cu as a possible additive, since it is known that
this has a negative influence if contained in steel even in very
small quantities. On the other hand, Fe is completely satisfac-
tory on this point. Moreover, Fe is reported as a material which
performs process softening of the aluminum and as a material
used to improve elongation. Moreover, since it is added in small
quantities, Fe can form a solid solution with aluminum, and im-
provement in tensile strength may be expected with the Properzi
process and the precipitation processing by heat treatment. Un-der these considerations we decided to utilize Fe as an additive.
Furthermore, thermal resistance improvement was also consid-
* Resarch & Develpment Group, Hitachi Cable, Ltd.
** Electronic & Automotive Products Group
Fig. 1 -Influence of the addition element exerted on electrical conduc-
tivity of aluminum2)
Selection of an addition element and quantity is considered so that elec-
trical conductivity may be set to about 60% IACS.
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HITACHI CABLE REVIEW No.25 (AUGUST 2006) 19
TensileStorength(MPa)
Elongation(%)
: Tensile Strength
: Elongation
0
50
100
150
200
250
300
0
5
10
15
20
25
30
54
56
58
60
62
64
66
RT 100 150 200 250 300 350ElectricalConductivity(%IACS
)
Annealing temperature ( ,1hr)
(a)
(b)
: Al: Al-0.3%Fe: Al-0.6%Fe
Tensile strength
Elongation
Fe concentration (mass%)
TensileStrength(MPa)
80
90
100
110
120
130
140
0 0.2 0.4 0.6 0.820
25
30
35
Elongation(%)
(Annealing temperature : 320 )
Elementy /C
(MPa/mass%)
f/C
(MPa/mass%)
Ag
Be
Cd
Ce
Cu
Fe
Ga
Ge
Hf
Mg
Mn
Si
V
Zn
19.6
46.6
98
7.35
19.6
10.8
5.0
14.7
19.6
66.6 or 58.8
90.2
56.8
125
12.7
15.7
37.2
24.5 or 15.7
18.6
19.6
45.1
9.8 or 2.9
ered and Zr was considered as an element to improve thermal re-
sistance. As a result, tensile strength and heat-resistance were im-
proved by adding Zr in amounts of 0.28mass% with aluminum. It
was decided to utilize Fe and Zr as additive to be included in this
study.
[3] EXAMINATION MATERIAL AND METHOD
At first, we produced aluminum alloy wire rods (of 9.5-mm
diameter) including 0.3 - 0.6mass% of Fe and 0.02 - 0.05mass%
of Zr, additions within the limits to allow Zr to form a solid
solution with aluminum(99.7% of purity) using the Properzi
process. Next, we carried out the cold-drawing process and per-
formed heat treatment, furthermore, through the cold-drawing
process we produced a wire of 0.25-mm diameter. This was con-
sidered as material for further experiment. Moreover, aluminum
(99.7% purity) produced with a similar process was used as
comparison material for the experiment. Next, we estimated
their softening characteristics.
[4] EXPERIMENT RESULT OF ALUMINUM-Fe-Zr SYS-TEM ALLOY WIRE, AND CONSIDERATIONS
4.1 Influence of the iron addition on the properties of an alu-
minum alloy wire
Figure 2 (a) shows the influence of heat treatment tempera-
ture on tensile strength and elongation of an Al-Fe alloy wire
(0.25-mm diameter). Figure 2 (b) shows the influence of heat
treatment temperature on electrical conductivity. It turns out that
the specimen added Fe compared with pure aluminum shows
high tensile strength in a wide range of annealing temperatures.
Moreover, at an annealing temperature of above 250C, the elec-
trical conductivity of any specimen is carried out at about2%IACS recovery compared with the no annealing specimen.
The reason is thought to be that processed strain was removed.
Table 1 Contribution of each element to solid solution hard-ening of aluminum3)
(sy / C, sf/ C : 0.2% proof stress and the amount of increasesof modification resistance by addition of unit mass % )It turns out that the effect of the improvement of 0.2% proofstress and modification resistance in Fe is high especiallyas an element.
Fig. 2 -Influence of heat treatment temperature on the tensile strength
and electrical conductivity of Al-Fe alloy wire (0.25-mm diameter)(a: Tensile strength, b: Electrical conductivity)
Fig. 3 -Influence of Fe concentration on tensile strength and elongation
after annealing.
When the concentration of Fe increases, tensile strength and elongation
also increase.
Figure 3 shows the tensile strength and elongation of pure alu-
minum and Al-Fe alloy wire annealed at 320C. As for an Al-Fe
alloy wire, this shows as expected that tensile strength and elon-
gation after re-crystallization are large compared with the pure
aluminum wire.
4.2 Influence of Zr addition on the properties of aluminum al-
loy wire
In section 4.1, Fe addition showed an improvement of ten-
sile strength and elongation compared with pure aluminum.
There is little influence on electrical conductivity at both
0.3mass% and 0.6mass% of Fe. For this reason, improvement
in tensile strength and the drawing process were thought as im-portant and the amount of Fe added was changed to 0.6mass%.
Based on these, Zr was added within the limits of Zr forming a
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HITACHI CABLE REVIEW No.25 (AUGUST 2006)20
TensileStorength(MPa)
Elongation(%)
0
50
100
150
200
250
300
0
5
10
15
20
25
30
: Al: Al-0.6%Fe: Al-0.6%Fe-0.02%Zr: Al-0.6%Fe-0.05%Zr
: Tensile Strength
: Elongation
54
56
58
60
62
64
66
RT 100 150 200 250 300 350ElectricalConductivity(%
IACS)
Annealing temperature ( ,1hr )
(a)
(b)
Alloy composition
Tensile
Strength
(MPa)
Elongation
(%)
Electrical
Conductivity
(%IACS)
Developed
material
Al-0.6mass%Fe-
0.02mass%Zr
Annealed
material 146 8 60.4
Annealed
material 120 8 63.0
Comparison
material Pure AluminumConventional
material 104 22 63.8
0
5
10
15
20
25
30
100 120 140 160 180 200
Tensile strength (MPa)
Elongation(%)
: Al: Al-0.6%Fe
: Al-0.6%Fe-0.02%Zr
: Al-0.6%Fe-0.05%Zr
Target property
solid solution with Al-0.6mass%Fe, and we estimated the vari-
ous properties.
Figure 4 (a) shows the influence of the annealing tempera-
ture on the tensile strength and elongation of an Al-Fe-Zr alloy
wire (0.25-mm diameter). Figure 4 (b) shows the influence of
the annealing temperature on electrical conductivity. The addi-
tion of Zr showed that thermal resistance was improved. How-
ever, the consequence of adding Zr is the remarkable decline inelectrical conductivity compared with improvement in strength,
when 0.05mass%Zr is added, it turns out that electrical conduc-
tivity falls below 60%IACS. As mentioned above, in consider-
ation of the decline in electrical conductivity and drawing
processabi li ty, the amount of addition of Zr was set to
0.02mass%. From section 4.1 and 4.2, Al-0.6mass%Fe-
0.02mass%Zr was selected as the Al-Fe-Zr alloy sample.
[5] COMPREHENSIVE CHARACTERISTIC EVALUATIONOF AN Al-Fe-Zr SYSTEM ALLOY WIRE
If considering use as a wire for electric equipment, then it is
required to combine tensile strength and elongation triggered
by the advantage of handling. For this reason, it is required that
tensile strength and elongation be adjusted. As in section 4, it
turns out that improvement in tensile strength and elongation is
expected by softening examination at the time. Then, examina-
tion obtains the balance tensile strength and elongation by spe-
cial heat treatment. Figure 5 shows the tensile strength and elon-
gation of Al-Fe alloy and Al-Fe-Zr alloy wire under various con-ditions of heat treatment. It turns out that the tensile strength
and elongation of Al-Fe-Zr alloy wire are excellent compared
with Al-Fe alloy wire. For example, when the amount of added
Zr is 0, 0.02, and 0.05mass%, the elongation of 8, 12, and 15%
are respectively obtained at a fixed tensile strength of 140 MPa.
It is reported that crystal grain turn minutely by 0.2mass% of Zr
added, and it is thought that the improvement in tensile strength
and elongation is based on the crystal grain effect. From the
above, it turns out that Al-Fe-Zr alloy has high tensile strength
above 30% compared with pure aluminum and elongation byacquiring above 5% and furthermore their properties can be con-
trolled. Table 2 shows the properties of the specimen. The im-
provement in above 30% of tensile strength above 5% of elon-
gation, and above 58%IACS of electrical conductivity which
Al-0.6mass%Fe-0.02mass%Zr made the target to the pure alu-
minum wire of the conventional system was acquired. The ten-
sile strength and elongation of this specimen alloy can be ad-
justed to a necessary value.
Fig. 4 -Influence of heat treatment temperature on the tensile strength
and electrical conductivity of Al-Fe-Zr alloy wire (0.25-mm diameter)
(a: Tensile strength, b: Electrical conductivity)
Fig. 5 -Comparison of tensile strength of Al -Fe-Zr alloy wires (0.25mm-
diameter) with pure aluminum. Al-Fe-Zr alloy combines tensile strength
and elongation.
Table 2 Example of room temperature properties of Al-Fe-
Zr alloy wire in an experiment (0.25mm-diameter)In annealed Al-0.6mass%Fe-0.02mass%Zr, tensile strengthincreases 22%, equivalent elongation and above 60%IACSelectrical conductivity as compared with annealed pure alu-minum.
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HITACHI CABLE REVIEW No.25 (AUGUST 2006) 21
Twist wire
20 mm
0.5 mm
Insulation
Twisted wires
Development materialCable
composition
Existence of
covering
Breakingstrength
(N)
Elongation
(%)
Electricalconductivity
(%IACS)
With nocoveringThose withcovering
42.2 16.4Al-0.6mass%Fe-0.02mass%Zr 7 / 0.25
59.7 20.360.7
[6] CABLE UTILIZING DEVELOPED ALUMINUM ALLOYWIRE
The cable (0.3SQ, 7/0.25) was produced as a cable used for the
car and the rebot for which lightering was needed. Figure 6
shows the cable utilizing the developed Al-0.6mass%Fe-
0.02mass%Zr as an experiment. Figure 7 shows a cross-section
photograph. In the trial production of this cable, the processes
of drawing and twisting covering of the wire and insulator etc.
are no problem. Table 3 shows the properties of the cable. We
expect the use of this aluminum alloy to expand in the future.
that responded to the new concept and, at the same time, can
control tensile strength and elongation. Moreover, the possibil-
ity of being supplied with similar conductivity as pure alumi-
num so that it can respond to customer's various needs and re-
spect environmental and recycling requirements. One of the fea-
tures of this alloy wire is its possibility to be manufactured us-
ing the Properzi process of continuity casting rolling method in
consideration of the homogeneity of the composition. With thisdeveloped aluminum alloy wire, while offering the function ac-
cording to demand of a Customer, the it is hoped that its use can
be extended to various fields.
[8] ACKNOWLEDGEMENT
We wish to express our deep gratitude to Ibaraki University
and to Professor Goroh Ito for their precious counsel and coop-
eration in the development of this aluminum alloy wire.
REFERENCES
(1) Y.Miyake: Keikinzoku, 36(1986), 51-60, 112-121.(2) E.E.Handbook: The Institute of Electrical Engineers of Ja-
pan, (1978), 619.
(3) The organization and character of aluminum: The Japan
Institute of Light Metals, (1991), 160.
(4) K.Shibata. et al: Fyeramu,7(2002),18-22.
(5) H.Takei. et al: Keikinzoku,30(1980),626-633.
(6) T.Fukui: Keikinzoku, 18(1968)320-331
(7) H.Suzuki. et al: Keikinzoku,33(1983),29-37.
(8) W.A.Dean: Aluminum,Ed.by J.E.Hatch,American Soc.Met.,Metals
Park,Ohio,(1984),240.
Toshiyuki Horikoshi
Resarch & Develpment GroupMaterials Technology Research & Development CenterCurrently engagad in research and development of elec-tric materials
Hiromitsu Kuroda
Resarch & Develpment GroupMaterials Technology Research & Development CenterCurrently engagad in research and development of elec-tric materials
Michiaki Shimizu
Electronic & Automotive Products GroupAutomotive Components Production Div.Electric Components Dept.
Seigi Aoyama
Resarch & Develpment GroupMaterials Technology Research & Development CenterPh.D. degree in Material Sciene
The Japan insutitute of MetalsCurrently engaged in research and development of elec-tric materials.
Fig. 6-Twist wire from the cable (0.3SQ, 7/0.25) produced using the
newly developed aluminum alloy.
The cable was insulated after twisting seven Al-Fe-Zr alloy wires
(0.25mm-diameter).
Fig. 7-A cross section of the trial production cable (0.3SQ, 7/0.25)
Table 3 Cable properties using Al-Fe-Zr alloy wire at roomtemperature
In the trial production of this cable, wire drawing and twist-ing wire and insulated covering, etc. have been conductedwithout any problems.
[7] CONCLUSION
In recent years the remarkable progress of the automotive
and electronics industry, the need for lightweight electric con-
duction material has increaseed and the development of alumi-num electric conduction material was considered with this in
mind. This development of an alloy wire focused on a material