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Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252
www.ijera.com 249 | P a g e
Cyclic Heating Effect on Hardness of Aluminum
Tahany W. Sadak*
*(Department of Production Engineering and Design, Faculty of Engineering, Beni-Suef University Beni-Suef,
Egypt)
ABSTRACT
Presented work discusses research results concerning the effect of the heat treatment process. Thermal fatigue
which expresses repeated heating and cooling processes affect the ductility or the brittleness of the material. In
this research 70 specimens of aluminum (2 mm thickness, 85 mm length, 32 mm width) are subjected to thermal
fatigue at different conditions. Heating temperatures; Th = 100, 300 and 500 ° C. Number of repeated cycles; N
=70. Results are evaluated then compared to each other and to that of specimens without subjected to thermal
fatigue.
Key words: Aluminum alloys, thermal analysis, heat treatment, hardness, thermal fatigue
I. INTRODUCTION
Well known advantages of aluminum alloys, like
low mass, good mechanical properties, corrosion
resistance, machinability, high percentage of
recycling, and low costs, are the driving force for
their development, i.e. usage in new applications as
early as in stage of development of a structures, as
well during development of new technological
solutions.
Thermal fatigue specifies the process of repeated
heating and cooling of machine parts. Some
investigators show the effect of cyclic heat treatment
on phase composition and structure of titanium alloys
[1, 2] others show the effect of repeated heating on
tempering or hardening of steels [3, 4, 5]. Performed
shortened heat treatment results in precipitation
hardening of the investigated 320.0 alloy, what
according to expectations produces increased
hardness of the material [6]. The improvement of
mechanical properties of the EN AB-42000 silumin
in the aspect of its hardness change due to the
performance of the T6 heat treatment is possible only
in case of the selection of suitable solutioning and
ageing treatment parameters [7]. Different machine
tools and elements are subjected to thermal fatigue in
different applications.
II. NOMENCLATURE
A Area of spherical surface indentation in Brinell
hardness test. [mm2
]
BHN Brinell hardness number. [Kg/mm2
]
d Impression diameter.[mm]
D Ball diameter. [mm]
N Number of thermal fatigue cycles
F Load of hardness test. [Kg]
tc Cooling time of thermal fatigue cycles. [min]
th Heating time of thermal fatigue cycles. [min]
TC Cooling temperature of thermal fatigue
process. [O
C]
Th Heating temperature of thermal fatigue
process. [O
C]
III. METHODS OF ANALYSES
To evaluate the effect of cyclic heating effect on
hardness of aluminum, the investigation was carried
out thus;
 Preparation of the specimens from aluminum.
 Hardness was measured for each specimen after
and before cyclic heating operations.
 From the different readings, curves were plotted
to know the trends of the property
IV. EQUIPMENT USED
 Laboratory Muffle Furnace
 Hand Polishing Aluminum Stand
 Hardness Testing machine
Preparation of the Hardness Specimens
The material used for this study is aluminum.
The sample Fig. 1 preparation was the usual grinding
and polishing procedure until a mirrored surface,
with no etching, was obtained.
Figure 1 Fatigue sample dimensions in millimeters.
Thickness: 2 mm mm.
Brinell Hardness Test
Brinell hardness is determined by forcing a hard
steel or carbide sphere of a specified diameter under a
REVIEW ARTICLE OPEN ACCESS
Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252
www.ijera.com 250 | P a g e
specified load into the surface of a material and
measuring the diameter of the indentation left after
the test Fig 2.
Figure 2 Brinell Hardness Test
The Brinell hardness number, or simply the
Brinell number, is obtained by dividing the load used,
in kilograms, by the actual surface area of the
indentation; A, in square millimeters. The result is a
pressure measurement, but the units are rarely stated.
The BHN is calculated according to the following
formula:
(1)
The ball diameter and applied load are constant
and are selected to suit the composition of the metal,
its hardness, and the thickness of the rest specimen,
Table 1. The diameter of the indentation is measured
with a special magnifying glass containing a scale
graduated in terms of a millimeter.
Table 1 Brinell test conditions
MaterialBHN
Thickness
of test
specimen
mm
Ratio
of
load
F to
ball
diam.
D
D
mm
F
Kg
Time load
application
Sec
aluminum
8 to
35
Over 5
From 6 to
3
Less than
3
F =
2.5
D2
10
5
2.5
250
62.5
15.625
60
The chemical composition of the investigated
specimen is shown in Table 2.
Table 2 The chemical composition percent.
Chemical composition%
Al Fe2 SI Cu
99.44 0.34 0.16 0.0041
Laboratory Muffle Furnace
The muffle furnace could be used for heating of
test specimen up1200o
C. Fig. 3 shows the
characteristic curves of the muffle furnace.
0
200
400
600
800
1000
1200
1400
0 40 80 100 140 180 220
Time; t [min]
Temperature;T[
o
c]
Figure 3 Characteristic curves of the muffle furnace
1 Heating – up curve, full load
2 Heating – up curve, partial load 50%.
3 Cooling Curve, with door closed.
4 Cooling Curve, with door open.
V. METALLOGRAPHIC TEST
The test specimens were firstly polished. A ball
of 2.5 mm diameter is chosen according to Table 1
for the test. The load is applied 15.625 Kg for 60 sec.
The hardness values before subjected to thermal
fatigue were measured on Brinell hardness tester
Table 3 shows the experimental results of hardness
test for the specimens of aluminum.
Table 3 Experimental results of hardness test of
aluminum without thermal fatigue.
Thermal
fatigue
Hardness Test
F=15.625 Kg D=2.5 mm t=60 sec
No
Thermal
fatigue
First specimen Second specimen
d1 BHN d2 BHN d1 BHN d2 BHN
0.64 47.8 0.64 47.8 0.65 46.3 0.67 43.5
Heating temperatures; Th = 100, 300 and 500 °C.
Number of repeated cycles; N =1, 3, 5, 20, 30, 50 and
70. The values of hardness are registered in Tables 4
to 6 respectively. The relationship between the
hardness values versus number of repeated cycles has
been plotted in Figs. 4 to 6.
Table 3 Experimental results of hardness test of
aluminum thermal fatigue heating temperature;
Th=100°C.
Thermal
fatigue
Hardness Test
F=31.25 Kg D=2.5 mm t=60 sec
Th
°C
N
Times
First specimen Second specimen
d1 BHN d2 BHN d1 BHN d2 BHN
100
1 0.64 47.8 0.64 47.8 0.65 46.3 0.65 46.3
3 0.65 46.3 0.65 46.3 0.65 46.3 0.65 46.3
7 0.65 46.3 0.65 46.3 0.66 44.8 0.67 43.5
14 0.60 54.3 0.60 54.3 0.63 49.3 0.64 47.8
20 0.65 46.3 0.65 46.3 0.65 46.3 0.65 46.3
30 0.65 46.3 0.65 46.3 0.65 46.3 0.65 46.3
50 0.63 49.3 0.63 49.3 0.63 46.3 0.63 49.3
70 0.64 47.8 0.64 47.8 0.64 47.8 0.64 47.8
1 2
3
4
Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252
www.ijera.com 251 | P a g e
0
10
20
30
40
50
60
0 10 20 30 40 50 60 70
Thermal Cycling; N
Hardness;BHN
Figure 4 Effect of thermal fatigue on hardness of
aluminum at temperature; Th =100o
C
Table 5 Experimental results of hardness test of
aluminum, thermal fatigue heating temperature;
Th=300°C.
Thermal
fatigue
Hardness Test
F=15.625 Kg D=2.5 mm t=60
sec
Th
°C
N
Times
First specimen Second specimen
d1 BHN d2 BHN d1 BHN d2 BHN
100
1 0.63 49.3 0.63 49.3 0.64 47.8 0.64 47.8
5
0.62
0.65
50.9
46.3
0.62
0.65
50.9
46.3
0.62
0.65
50.9
46.3
0.62
0.65
50.9
46.3
10 0.63 49.3 0.63 49.3 0.65 46.3 0.65 46.3
15 0.70 39.8 0.70 39.8 0.70 39.8 0.70 39.8
20 0.70 39.8 0.70 39.8 0.70 39.8 0.70 39.8
30 0.71 38.6 0.71 38.6 0.71 38.6 0.71 38.6
50 0.69 41.0 0.71 38.6 0.72 37.6 0.72 37.6
70
0.72
70
37.6
39.8
0.72
70
37.6
39.8
0.72
0.72
37.6
37.6
0.72
0.72
37.6
37.6
0
10
20
30
40
50
60
0 10 20 30 40 50 60 70
Thermal Cycling; N
Hardness;BHN
Figure 5 Effect of thermal fatigue on hardness at
temperature; Th=300 o
C
Table 3 Experimental results of hardness test of
aluminum thermal fatigue heating temperature;
Th =500°C.
Thermal
fatigue
Hardness Test
F=15.625 Kg D=2.5 mm t=60
sec
Th
°C
N
Times
First specimen Second specimen
d1 BHN d2 BHN d1 BHN d2 BHN
100
1 0.94 21.7 0.94 21.7
5 0.94 21.7 0.94 21.7 0.95 21.2 0.96 20.8
10 0. 96 20.8 0. 96 20.8 0. 96 20.8 0. 96 20.8
20 0.80 30.2 0.83 28.1 0.95 21.2 0.95 21.2
30 0.85 26.7 0.90 23.7 0.95 21.2 0.96 20.8
50 0.82 28.7 0.82 28.7 0.90 23.7 0.94 21.7
70 0.97 20.3 0.97 20.3 0.97 20.3 0.97 20.3
0
10
20
30
40
50
60
0 10 20 30 40 50 60 70
Thermal Cycling; N
Hardness;BHN
Figure 6 Effect of thermal fatigue on hardness at
temperature; Th =500 oC
VI. RESULTS
Hardness of aluminum before thermal fatigue
amounted to HB 2.5/15.625/60, and was in the range
from 47.8 to 43.5. After thermal fatigue, obtained
hardness amounted to HB 2.5/15.625/60, at heating
temperature; Th=100 o
C, N=1, and was in the range
from 47.8 to 46.3, N=3 obtained hardness amounted
to 46.3 HB 2.5/15.625/60, N=7 it was in the range
from 43.5to 46.3, N=14 it was in the range from 47.8
to 54.3, N=20 obtained hardness amounted to 46.3
HB, N=30 obtained hardness amounted to 46.3 HB,
N=50 it was in the range from 46.3 to 49.3 and N=70
obtained hardness amounted to 47.8 HB Fig. 4 shows
the average values of BH hardness.
In cases of heating temperature 300 and 500 o
C
obtained average hardness amounted to HB
2.5/15.625/60 at different repeated cyclic heating
show in Figs. 5 and 6
Comparison of thermal fatigue effect of hardness
of aluminum at different values of heating
temperature; Th = 100, 300 and 500 show in Fig. 7.
Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252
www.ijera.com 252 | P a g e
0
10
20
30
40
50
60
0 10 20 30 40 50 60 70
Thermal Cycling; N
Hardness;BHN
Figure 7 Comparison of thermal fatigue on hardness
at different values of heating temperature; Th=100,
300 and 500 o
C
VII. Conclusion
The experimental results show that there is a
significant effect of cycling thermal treatment on
hardness.
Repeated heating of aluminum specimens at 100
o
C show slightly decrease in hardness values, which
have no effect by the increase of heating cycles. By
cyclic heating at 300 o
C the hardness decreases to
37.6 BHN after 20 cycles, then it constant by further
heating cycles, while by heating to 500 o
C, the
hardness decreases to a value of about 20.3 BHN
after 10 cycles then remains at this value by further
heating cycles
Acknowledgements
The experimental investigations are conducted in
the Strength of Materials Research Lab., Faculty of
Engineering, Minia University.
The author wish to express their gratitude and
deep appreciation to Prof. Dr.-Ing. M. RIZK and to
the staff of the laboratory for their assistance and
help.
REFERENCES
[1] Gridnev, V. N., et al., Effect of cyclic heat
treatment on the phase composition and
structure of VT 22 alloy, Izvestiya Akademii
Nauk SSSr. Metally, No 3, 1984.
[2] Kopp, R., Scheffer, L., Einfluss dus
mehrmalingen Erwarmens beim partiellen
schmieden Von Werkstocken aus, Ti A16
V4, Metall. 37. Jahrgang. Heft 4. April
1983.
[3] Zabil' Skiy, V. V. and Sarrak, V. I.,
Recovery of the properties and
strengthening in steels tempered under load,
Phys. Met. Metall. Vol. 55, No.2, 1983
[4] Bakhmatov, A. L., Effect of partial cooling
and repeated heating in hardening on the
structure and properties of nitride parts made
of steel 25khGM, Metallovedenie I
termicheskaya obrabotka metallov, No. 8,
August 1986
[5] Moiseyev, B. A., et at., Effect of thermo
cycling on the structure and mechanical
properties of 35khN2MF steel, Soviet
Materials Science Reviews, 2, 1988.
[6] J. Pezda Effect of Shortened Heat Treatment
on the Hardness and Microstructure of 320.0
Aluminium Alloy, Archives of Foundry
Engineering, Published quarterly as the
organ of the Foundry Commission of the
Polish Academy of Sciences Corresponding
author. Volume14, 2/2014, 27 – 30
[7] J. Pezda The Effect of The T6 Hea
Treatment on Hardness and Microstructure
of the En Ac-Alsi12cunimg Alloy,
researchgate.net, METALURGIJA, 53
(2014) 1, 63-66
300
o
C
100
o
C
500
o
C

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Cyclic Heating Effect on Hardness of Aluminum

  • 1. Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252 www.ijera.com 249 | P a g e Cyclic Heating Effect on Hardness of Aluminum Tahany W. Sadak* *(Department of Production Engineering and Design, Faculty of Engineering, Beni-Suef University Beni-Suef, Egypt) ABSTRACT Presented work discusses research results concerning the effect of the heat treatment process. Thermal fatigue which expresses repeated heating and cooling processes affect the ductility or the brittleness of the material. In this research 70 specimens of aluminum (2 mm thickness, 85 mm length, 32 mm width) are subjected to thermal fatigue at different conditions. Heating temperatures; Th = 100, 300 and 500 ° C. Number of repeated cycles; N =70. Results are evaluated then compared to each other and to that of specimens without subjected to thermal fatigue. Key words: Aluminum alloys, thermal analysis, heat treatment, hardness, thermal fatigue I. INTRODUCTION Well known advantages of aluminum alloys, like low mass, good mechanical properties, corrosion resistance, machinability, high percentage of recycling, and low costs, are the driving force for their development, i.e. usage in new applications as early as in stage of development of a structures, as well during development of new technological solutions. Thermal fatigue specifies the process of repeated heating and cooling of machine parts. Some investigators show the effect of cyclic heat treatment on phase composition and structure of titanium alloys [1, 2] others show the effect of repeated heating on tempering or hardening of steels [3, 4, 5]. Performed shortened heat treatment results in precipitation hardening of the investigated 320.0 alloy, what according to expectations produces increased hardness of the material [6]. The improvement of mechanical properties of the EN AB-42000 silumin in the aspect of its hardness change due to the performance of the T6 heat treatment is possible only in case of the selection of suitable solutioning and ageing treatment parameters [7]. Different machine tools and elements are subjected to thermal fatigue in different applications. II. NOMENCLATURE A Area of spherical surface indentation in Brinell hardness test. [mm2 ] BHN Brinell hardness number. [Kg/mm2 ] d Impression diameter.[mm] D Ball diameter. [mm] N Number of thermal fatigue cycles F Load of hardness test. [Kg] tc Cooling time of thermal fatigue cycles. [min] th Heating time of thermal fatigue cycles. [min] TC Cooling temperature of thermal fatigue process. [O C] Th Heating temperature of thermal fatigue process. [O C] III. METHODS OF ANALYSES To evaluate the effect of cyclic heating effect on hardness of aluminum, the investigation was carried out thus;  Preparation of the specimens from aluminum.  Hardness was measured for each specimen after and before cyclic heating operations.  From the different readings, curves were plotted to know the trends of the property IV. EQUIPMENT USED  Laboratory Muffle Furnace  Hand Polishing Aluminum Stand  Hardness Testing machine Preparation of the Hardness Specimens The material used for this study is aluminum. The sample Fig. 1 preparation was the usual grinding and polishing procedure until a mirrored surface, with no etching, was obtained. Figure 1 Fatigue sample dimensions in millimeters. Thickness: 2 mm mm. Brinell Hardness Test Brinell hardness is determined by forcing a hard steel or carbide sphere of a specified diameter under a REVIEW ARTICLE OPEN ACCESS
  • 2. Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252 www.ijera.com 250 | P a g e specified load into the surface of a material and measuring the diameter of the indentation left after the test Fig 2. Figure 2 Brinell Hardness Test The Brinell hardness number, or simply the Brinell number, is obtained by dividing the load used, in kilograms, by the actual surface area of the indentation; A, in square millimeters. The result is a pressure measurement, but the units are rarely stated. The BHN is calculated according to the following formula: (1) The ball diameter and applied load are constant and are selected to suit the composition of the metal, its hardness, and the thickness of the rest specimen, Table 1. The diameter of the indentation is measured with a special magnifying glass containing a scale graduated in terms of a millimeter. Table 1 Brinell test conditions MaterialBHN Thickness of test specimen mm Ratio of load F to ball diam. D D mm F Kg Time load application Sec aluminum 8 to 35 Over 5 From 6 to 3 Less than 3 F = 2.5 D2 10 5 2.5 250 62.5 15.625 60 The chemical composition of the investigated specimen is shown in Table 2. Table 2 The chemical composition percent. Chemical composition% Al Fe2 SI Cu 99.44 0.34 0.16 0.0041 Laboratory Muffle Furnace The muffle furnace could be used for heating of test specimen up1200o C. Fig. 3 shows the characteristic curves of the muffle furnace. 0 200 400 600 800 1000 1200 1400 0 40 80 100 140 180 220 Time; t [min] Temperature;T[ o c] Figure 3 Characteristic curves of the muffle furnace 1 Heating – up curve, full load 2 Heating – up curve, partial load 50%. 3 Cooling Curve, with door closed. 4 Cooling Curve, with door open. V. METALLOGRAPHIC TEST The test specimens were firstly polished. A ball of 2.5 mm diameter is chosen according to Table 1 for the test. The load is applied 15.625 Kg for 60 sec. The hardness values before subjected to thermal fatigue were measured on Brinell hardness tester Table 3 shows the experimental results of hardness test for the specimens of aluminum. Table 3 Experimental results of hardness test of aluminum without thermal fatigue. Thermal fatigue Hardness Test F=15.625 Kg D=2.5 mm t=60 sec No Thermal fatigue First specimen Second specimen d1 BHN d2 BHN d1 BHN d2 BHN 0.64 47.8 0.64 47.8 0.65 46.3 0.67 43.5 Heating temperatures; Th = 100, 300 and 500 °C. Number of repeated cycles; N =1, 3, 5, 20, 30, 50 and 70. The values of hardness are registered in Tables 4 to 6 respectively. The relationship between the hardness values versus number of repeated cycles has been plotted in Figs. 4 to 6. Table 3 Experimental results of hardness test of aluminum thermal fatigue heating temperature; Th=100°C. Thermal fatigue Hardness Test F=31.25 Kg D=2.5 mm t=60 sec Th °C N Times First specimen Second specimen d1 BHN d2 BHN d1 BHN d2 BHN 100 1 0.64 47.8 0.64 47.8 0.65 46.3 0.65 46.3 3 0.65 46.3 0.65 46.3 0.65 46.3 0.65 46.3 7 0.65 46.3 0.65 46.3 0.66 44.8 0.67 43.5 14 0.60 54.3 0.60 54.3 0.63 49.3 0.64 47.8 20 0.65 46.3 0.65 46.3 0.65 46.3 0.65 46.3 30 0.65 46.3 0.65 46.3 0.65 46.3 0.65 46.3 50 0.63 49.3 0.63 49.3 0.63 46.3 0.63 49.3 70 0.64 47.8 0.64 47.8 0.64 47.8 0.64 47.8 1 2 3 4
  • 3. Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252 www.ijera.com 251 | P a g e 0 10 20 30 40 50 60 0 10 20 30 40 50 60 70 Thermal Cycling; N Hardness;BHN Figure 4 Effect of thermal fatigue on hardness of aluminum at temperature; Th =100o C Table 5 Experimental results of hardness test of aluminum, thermal fatigue heating temperature; Th=300°C. Thermal fatigue Hardness Test F=15.625 Kg D=2.5 mm t=60 sec Th °C N Times First specimen Second specimen d1 BHN d2 BHN d1 BHN d2 BHN 100 1 0.63 49.3 0.63 49.3 0.64 47.8 0.64 47.8 5 0.62 0.65 50.9 46.3 0.62 0.65 50.9 46.3 0.62 0.65 50.9 46.3 0.62 0.65 50.9 46.3 10 0.63 49.3 0.63 49.3 0.65 46.3 0.65 46.3 15 0.70 39.8 0.70 39.8 0.70 39.8 0.70 39.8 20 0.70 39.8 0.70 39.8 0.70 39.8 0.70 39.8 30 0.71 38.6 0.71 38.6 0.71 38.6 0.71 38.6 50 0.69 41.0 0.71 38.6 0.72 37.6 0.72 37.6 70 0.72 70 37.6 39.8 0.72 70 37.6 39.8 0.72 0.72 37.6 37.6 0.72 0.72 37.6 37.6 0 10 20 30 40 50 60 0 10 20 30 40 50 60 70 Thermal Cycling; N Hardness;BHN Figure 5 Effect of thermal fatigue on hardness at temperature; Th=300 o C Table 3 Experimental results of hardness test of aluminum thermal fatigue heating temperature; Th =500°C. Thermal fatigue Hardness Test F=15.625 Kg D=2.5 mm t=60 sec Th °C N Times First specimen Second specimen d1 BHN d2 BHN d1 BHN d2 BHN 100 1 0.94 21.7 0.94 21.7 5 0.94 21.7 0.94 21.7 0.95 21.2 0.96 20.8 10 0. 96 20.8 0. 96 20.8 0. 96 20.8 0. 96 20.8 20 0.80 30.2 0.83 28.1 0.95 21.2 0.95 21.2 30 0.85 26.7 0.90 23.7 0.95 21.2 0.96 20.8 50 0.82 28.7 0.82 28.7 0.90 23.7 0.94 21.7 70 0.97 20.3 0.97 20.3 0.97 20.3 0.97 20.3 0 10 20 30 40 50 60 0 10 20 30 40 50 60 70 Thermal Cycling; N Hardness;BHN Figure 6 Effect of thermal fatigue on hardness at temperature; Th =500 oC VI. RESULTS Hardness of aluminum before thermal fatigue amounted to HB 2.5/15.625/60, and was in the range from 47.8 to 43.5. After thermal fatigue, obtained hardness amounted to HB 2.5/15.625/60, at heating temperature; Th=100 o C, N=1, and was in the range from 47.8 to 46.3, N=3 obtained hardness amounted to 46.3 HB 2.5/15.625/60, N=7 it was in the range from 43.5to 46.3, N=14 it was in the range from 47.8 to 54.3, N=20 obtained hardness amounted to 46.3 HB, N=30 obtained hardness amounted to 46.3 HB, N=50 it was in the range from 46.3 to 49.3 and N=70 obtained hardness amounted to 47.8 HB Fig. 4 shows the average values of BH hardness. In cases of heating temperature 300 and 500 o C obtained average hardness amounted to HB 2.5/15.625/60 at different repeated cyclic heating show in Figs. 5 and 6 Comparison of thermal fatigue effect of hardness of aluminum at different values of heating temperature; Th = 100, 300 and 500 show in Fig. 7.
  • 4. Tahany W. Sadak et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 5, Issue 8, (Part - 5) August 2015, pp.249-252 www.ijera.com 252 | P a g e 0 10 20 30 40 50 60 0 10 20 30 40 50 60 70 Thermal Cycling; N Hardness;BHN Figure 7 Comparison of thermal fatigue on hardness at different values of heating temperature; Th=100, 300 and 500 o C VII. Conclusion The experimental results show that there is a significant effect of cycling thermal treatment on hardness. Repeated heating of aluminum specimens at 100 o C show slightly decrease in hardness values, which have no effect by the increase of heating cycles. By cyclic heating at 300 o C the hardness decreases to 37.6 BHN after 20 cycles, then it constant by further heating cycles, while by heating to 500 o C, the hardness decreases to a value of about 20.3 BHN after 10 cycles then remains at this value by further heating cycles Acknowledgements The experimental investigations are conducted in the Strength of Materials Research Lab., Faculty of Engineering, Minia University. The author wish to express their gratitude and deep appreciation to Prof. Dr.-Ing. M. RIZK and to the staff of the laboratory for their assistance and help. REFERENCES [1] Gridnev, V. N., et al., Effect of cyclic heat treatment on the phase composition and structure of VT 22 alloy, Izvestiya Akademii Nauk SSSr. Metally, No 3, 1984. [2] Kopp, R., Scheffer, L., Einfluss dus mehrmalingen Erwarmens beim partiellen schmieden Von Werkstocken aus, Ti A16 V4, Metall. 37. Jahrgang. Heft 4. April 1983. [3] Zabil' Skiy, V. V. and Sarrak, V. I., Recovery of the properties and strengthening in steels tempered under load, Phys. Met. Metall. Vol. 55, No.2, 1983 [4] Bakhmatov, A. L., Effect of partial cooling and repeated heating in hardening on the structure and properties of nitride parts made of steel 25khGM, Metallovedenie I termicheskaya obrabotka metallov, No. 8, August 1986 [5] Moiseyev, B. A., et at., Effect of thermo cycling on the structure and mechanical properties of 35khN2MF steel, Soviet Materials Science Reviews, 2, 1988. [6] J. Pezda Effect of Shortened Heat Treatment on the Hardness and Microstructure of 320.0 Aluminium Alloy, Archives of Foundry Engineering, Published quarterly as the organ of the Foundry Commission of the Polish Academy of Sciences Corresponding author. Volume14, 2/2014, 27 – 30 [7] J. Pezda The Effect of The T6 Hea Treatment on Hardness and Microstructure of the En Ac-Alsi12cunimg Alloy, researchgate.net, METALURGIJA, 53 (2014) 1, 63-66 300 o C 100 o C 500 o C