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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 17
WEAR CHARACTERISTICS OF PURE ALUMINIUM, AL-ALLOY &
AL-ALUMINA METAL MTRIX NANO COMPOSITE IN DRY
CONDITION: PART-III
Vyjainto Kumar Ray1
, Payodhar Padhi2
, B. B. Jha3
, Tapas Kumar Sahoo4
1
Student of Ph.D., Mechanical Engineering Department, B.P.U.T., Bhubaneswar, Orissa, India
2
Principal, Mechanical Engineering Department, K.I.S.T., Bhubaneswar, Orissa, India
3
Chief Scientist, Metallurgical Engineering, Surface engineering department, I.M.M.T., Bhubaneswar, Orissa, India
4
Technical Assistant, Metallurgical Engineering, Surface engineering department, I.M.M.T., Bhubaneswar, Orissa,
India
Abstract
In this report, the aluminium metal matrix was reinforced with 1.5 wt. % of Al2O3 nano particles using non-contact cavitation
method to prepare the metal matrix nano composite. Microstructural examination conducted on the samples revealed a uniform
distribution of alumina particulates. Sliding wear behavior of the as-cast MMNC was studied in dry condition, under different test
conditions by varying the load and the sliding velocity, with an unlubricated Multiple Tribo Tester. It was found that resistance to
sliding wear improved considerably with the addition of alumina nano particles. Microscopic examinations of the worn out
surfaces of pure Al, Al-alloy (duralumin) and MMNC reveal that the MMNC has greater resistance to sliding wear compared to
pure aluminium and duralumin. Wear increases with increase in load and sliding velocity. Wear is more when load and speed are
increased in steps. Delamination and abrasion are the dominating types of wear observed.
Keywords: Sliding Wear, Al2O3, MMNC, Duralumin, Delamination and Abrasion.
--------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
With the development of new processing techniques and the
demand for lighter materials with high strength and
stiffness, high performance composite materials have been
developed which show enhanced properties compared to
traditional metals and alloys. Most of these high
performance materials are metallic matrixes reinforced with
fibre, particulate or whiskers. MMNCs are emerging as the
most versatile materials for advanced structural, automotive,
aviation, aerospace, defense applications because of their
excellent combination of properties. In recent years,
considerable interest has been paid in extending the use of
these composite materials in marine environment [1, 2].
These MMNCs have emerged as the important class of
advanced materials giving the prospect to tailor the material
properties according to their needs. These materials differ
from the conventional engineering materials because of their
homogeneity [3]. Aluminium based MMNCs possess
desirable properties like high specific stiffness, low density,
high specific strength controlled co efficient of thermal
expansion, increased fatigue resistance and superior
dimensional stability at elevated temperatures etc. [4, 5].
The mechanical and tribological properties of the MMNCs
can be improved by reinforcing various materials ranging
from very soft materials like Graphite, Talc etc. to high
hardened ceramic particulates like SiC, Al2O3, etc., [6, 7].
However, because of their high cost of production, their
application in industries is slowed down. Casting
Technology plays the key to overcome this problem,
although several technical challenges exist. Achieving a
uniform distribution of reinforcement within the matrix is a
big challenge, which directly influences the properties and
quality of the composite materials. The MMNCs possess
excellent mechanical and tribological properties and are,
therefore, considered as prospective engineering materials
for various tribological applications [8-15]. It is reported by
many researchers that sliding wear resistance and abrasion
resistance of MMCs and MMNCs, reinforced with ceramic
particulates like SiC, Al2O3, have improved [8-11]. When
nano particles of quantity as small as 2 wt. percent are
added, it enhances the hardness and yield strength by a
factor as high as 2 [16]. There are several methods for the
production of metal matrix nano composites which include
mechanical alloying, vertex process, and spray deposition
etc. But, the above processes are expensive. Solidification
processing is a relatively cheaper route. Nano particulates
tend to agglomerate during solidification processing as a
result of Van der Waals forces and therefore, proper
dispersion of the nano particulates in metal matrix is a
challenge. In the present work, a non-contact method, where
the ultrasonic probe is not in direct contact with the liquid
metal, was attempted to disperse nano sized Al2O3
particulates in aluminum matrix. In this method, the mold
was subjected to ultrasonic vibration [16-20].
But, no work has ever been reported on the dry sliding wear
behavior of MMNCs produced by non-contact cavitation
method [16, 21]. Therefore, in the present investigation, an
attempt has been made to study the dry sliding wear
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 18
behavior of Al+1.5% by wt. Al2O3 MMNC, prepared by
non-contact cavitation method, under different test
conditions by varying applying loads and sliding speeds
over a predefined time period.
2. EXPERIMENTAL PROCEDURE
2.1 Material
Alumina is a high hardened ceramic material. The chemical
composition of the composite (Al-Al2O3 1.5% by wt. nano
particle) is shown in Table 1. The motto to design MMNC is
to combine the metals & ceramic i.e. addition of high
strength, high modulus refractory particles to ductile metal
matrix to get tailor made properties.
Table 1 Composition of Al-Al2O3 (1.5 wt. %) MMNC.
Element Fe Mg Si Al Al2O3
Wt. % 1.3 0.43 0.26 96.51 1.5
Fig-1 HRTEM micrograph of Al2O3 nano powder
The Nano composites are prepared by a non-contact
ultrasonic solidification method by Padhi et al [16, 21].
2.2 Preparation of MMNC
The procedure for preparation of MMNC done by Padhi et
al [16, 21] is as follows. The experimental set up is shown in
Fig.1. It consists of an ultrasonic generator that generates
ultrasonic waves, an ultrasonic chamber and steel mould.
The mould was preheated to avoid thermal cracking. The
preheated mould was kept in the ultrasonic chamber and the
chamber was subjected to vibration at a frequency of 35
KHz. Liquid aluminum and alumina particulate (1.5 wt. %)
having average size 10 nm were simultaneously poured into
the vibrating mould from the mixing chamber.
Fig-2: Experimental set up
After the simultaneous pouring, the heating element was
immediately brought down above the liquid metal in order
to delay the solidification. The vibration was carried out for
a period of five minutes to ensure complete mixing. The
castings were obtained in both longitudinal and transverse
section.
Fig-3: HRTEM micrographs of Al-Al2O3 nano composite
showing uniform distribution of nano particles
2.3 Wear Tests
The experiments described here were carried out on a
Multiple Tribo Tester (TR-5), Ducom make. In this Multiple
Tribo Tester, the wheel rotates and the specimen, of size
6.35 x 6.35 x 9 mm, is pressed against the wheel .The
specimen is held by the fixture. Loads ranging from 0 to
1000 N and speeds up to 2000 rpm can be applied to press
the specimen against the periphery of the 20 mm thick, 60
mm diameter wheel. Since the specimen is held stationary
and the wheel rotates, the sliding contact occurs between the
wheel and the specimen and wear of both takes place as the
load is applied for the predefined test duration. Here, the
sliding wear tests were carried out under different load
conditions and at different speeds for a period of 30 minutes
or 1800 seconds. The test conditions are as follows.
1. Load of 100 N (constant), speed of 300 rpm
(constant) and test duration of 30 minutes (1800
Seconds).
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 19
2. Step load of 50 N with step load 10 N, 5 minutes
duration step, speed of 300 rpm (constant) and test
duration of 30 minutes (1800 Seconds).
3. Load of 130 N (constant), step speed of 100 rpm with
step of 100 rpm, time variation 10 minutes and test
duration of 30 minutes (1800 seconds).
4. Load of 130 N (constant), speed of 300 rpm
(constant) and test duration of 30 minutes (1800
seconds).
3. RESULTS AND DISCUSSION
The aluminum, duralumin and MMNC specimens were
subjected to the above said test conditions. Duralumin is an
aluminum-copper alloy. In addition to aluminium, the main
materials constituting duralumin are copper, manganese and
magnesium. It is used in aviation and automobile industry.
Fig-4: Wear verses time keeping speed constant at 300 rpm
at two different load conditions of 100 N (constant) and 100
N (step load) for pure aluminium, duralumin (Al-alloy) and
MMNCs.
Figure-4 shows the graph between wear in (µm) verses ime
in seconds for pure Aluminium, alloy and MMNC keeping
speed constant at 300 rpm at two different load conditions of
100 N (constant) and 100 N (step load) . The sliding wear
of commercially pure Aluminium, in both the conditions,
shows that the wear increases w.r.t. time. In case of
MMNCs, in both the cases, no significant variation of wear
occurs. Also the maximum wear in case of MMNC is 300
µm under 100 N step load whereas it is reduced to 200 µm
under 100 N constant load which occur after 1800 seconds
i.e. entire time duration. In case of pure aluminium, wear
increases drastically up to 1500 µm within 1000 seconds
approximately under 100 N constant load, but it is reduced
to 1350 µm within 900 seconds approximately under 100 N
step load. Initially pure aluminium is sticking to the wheel
under step load which indicates negative. In case of
duralumin, the maximum wear is 500 µm under 100 N
constant load and 600 µm under 100 N (step load). In all the
cases, wear is more under step load condition. Hence it is
concluded that the wear properties of composite is
significantly increased compared to pure aluminium and
alloy.
-500
0
500
1000
1500
2000
2500
0 500 1000 1500 2000
wear(µm)
time (sec.)
wearvs time
Al 130N 300rpm comp. 130N 300rpm
duralumin 130 N 300 rpm comp. 130N, 300 rpm(step)
Al 130N,300rpm(step) duralumin 130N 300rpm(step)
Fig-5: Wear verses time keeping load constant at 130 N at
two different speeds of 300 rpm (constant) and 300 rpm
(step) for pure Al, duralumin and MMNC.
Figure-5 shows the wear verses time keeping load constant
at 130 N at two different speeds of 300 rpm (constant) and
300 rpm (step) for pure aluminium, duralumin and MMNC.
It is observed that wear of MMNC, which is 750 µm under
300 rpm constant speed, increases gradually and linearly as
time increases up to 1800 seconds. But under 300 rpm step
speed, wear increases linearly up to 1500 µm approximately
till 1400 seconds are covered and then to 2300 µm suddenly
and gets worn out after 1550 seconds. In case of pure
aluminium, the wear increases to 1500 µm at 1000 seconds
during 300 rpm step speed condition and under 300 rpm
constant speed condition, the wear comes down to 1300 µm
approximately at 700 seconds. Similarly, in case of alloy,
the maximum wear is 2000 µm under constant speed
condition within 400 seconds and the maximum wear is
1600 µm under step speed condition within 1600 seconds.
Initially the alloy is sticking to the wheel under step load
which indicates negative. In all the cases, wear is more
under step speed condition. Again, it is concluded that the
wear properties of composite is significantly increased
compared to pure aluminium and alloy.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 20
Fig-6: Weight loss verses sliding distance keeping speed
constant at 300 rpm at two different load conditions of 100
N (constant) and 100 N (step load) for pure Al, duralumin
and MMNC.
Figure-6 shows weight loss verses sliding distance keeping
speed constant at 300 rpm under two different load
conditions 100 N constant and 100 N step. At constant load,
for MMNC, weight loss is initially high and gradually
decreases to nearly zero and maintains a steady state till
sliding distance 2000 meters. This happens due to the
embodied of nano particles in the aluminium matrix. Weight
loss for MMNCs at step load conditions is initially more and
gradually decreases to very small amount till 600 meters of
sliding distance then again decreases to almost zero and
continues to 1800 meters sliding distance. This is due to the
application of step load because during the transition period,
the wear rate decreases and subsequently it maintains steady
state. In case of pure aluminium, at constant load, weight
loss of material varies significantly as shown in the Figure 6.
Initially the material loss is very high (2800 µm), then
decreases to negative value due to sticking to the wheel,
then again increases and at 1000 meters of sliding distance,
complete worn out takes place. During the step load
condition, when sliding distance exceeds 50 meters, weight
loss increases to 1700 µm, then drastically decreases to
negative value due to sticking to the wheel, then again
increases and at 1000 meters of sliding distance, complete
worn out takes place. The weight loss for composites, in
both the cases, is initially high and then decreases to almost
zero as sliding distance increases up to 2000 meters. This
happens due to increase of hardness as alumina nano
particles embedded in the aluminium matrix. But still here is
a difference of weight loss between constant load and step
load. During step load, weight loss is more compared to
constant load. This is due to the frequent increase of load.
Weight loss increases at each step, which is very less. In
case of duralumin, under constant load 100 N, wt. loss
increases up to 900 µm, then falls to negative value for
sticking to the wheel, then rises and continues up to 2000
meters at almost constant rate. But under step load
condition, the alloy specimen sticks to the wheel initially
showing negative wt. loss. The wt. loss then rises up to 3000
µm, then falls to negligible value and continues up to 1850
meters of sliding distance. Weight loss is more when speed
is increased in steps.
Fig-7: Weight loss verses sliding distance keeping load
constant at 130 N at two different speeds of 300 rpm
(constant) and 300 rpm (step) for pure Al, duralumin and
MMNC.
Figure-7 shows weight loss verses sliding distance keeping
load constant at 130 N under constant and step speed
conditions. Weight loss for MMNC specimen at both speed
conditions is nearly zero though there is a little difference
which is not so significant where as in case of pure
aluminium, weight loss of material varies significantly as
shown. Initially the material is sticking to the wheel which
indicates negative. For duralumin, under 130 N constant
load and 300 rpm constant speed, wt. loss rises to 6500 µm
initially, then falls to around 500 µm and continues up to
300 meters of sliding distance. Under 300 rpm step speed
and 130 N constant load, alloy initially sticks to the wheel
showing negative wt. loss and then continues up to 1600
meters.
In all the cases, weight loss is more during step speeds. This
happens when speed changes step wise, at each step the wt.
loss increases and stabilizes after certain time. This
phenomena continues till the end. At constant speed,
initially weight loss is high and decreases to negligible
amount after few sliding distance and then maintains the
same.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 21
Fig-8: Force of friction verses time keeping speed constant
(300 rpm) at two different load conditions of 100 N constant
and 100 N step for pure Al, duralumin and MMNC.
Figure-8 shows the graph between force of friction verses
time keeping speed constant at two different load conditions.
For MMNC, the force of friction is almost constant in two
loading conditions, over the entire time period and is more
when load is applied in step. In case of pure aluminium,
force of friction is negative i.e. friction resistance is almost
zero under both the load conditions. For duralumin, the
force of friction is almost constant over the entire time
period under constant load condition where as it is negative
when load is increased in steps because it sticks to the
wheel. Friction resistance is more in case of MMNC.
Fig-9: Force of friction verses time keeping load constant
(130 N) at two different speed conditions of 300 rpm
(constant) and 300 rpm (step) for pure Al, duralumin and
MMNC.
Figure-9 shows the graph between force of friction verses
time (seconds) keeping load constant at 130 N under two
different speed conditions i.e. 300 rpm (constant) and 300
rpm (step). For MMNC, the friction force is maximum
initially and then remains almost constant under constant
speed condition of 300 rpm over the entire time period,
while under the step speed condition of 300 rpm, it is also
maximum at many points of the curve, but fluctuating
significantly as speed is applied stepwise over a time period
of 1700 seconds. In case of pure aluminium, force of friction
is negative in both the cases. As the material is sticking to
the wheel, the characteristic curves of aluminium in both the
cases show negative. For alloy, as the material is sticking to
the wheel, the characteristic curves in both the cases show
negative.
4. MICROSCOPIC EVALUATION
The microstructure of the worn out samples were evaluated
under FESEM. The FESEM images are shown in the figures
below.
Fig-10 Microstructure of pure Al at 100N and 300 rpm
Fig-11 Microstructure of alloy at 100N and 300 rpm
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 22
Fig-12 Microstructure of MMNC at 100N and 300 rpm
Fig-13 Microstructure of Al at 100 N (step) & 300 rpm
Fig-14 Microstructure of alloy at 100 N (step) & 300 rpm
Fig-15 Microstructure of MMNC at 100 N (step) &
300 rpm
Fig-16 Microstructure of pure Al at 130 N & 300 rpm (step)
Fig-17 Microstructure of Alloy at 130 N & 300 rpm (step)
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 23
Fig-18 Microstructure of MMNC at 130 N & 300 rpm (step)
Fig-19 Microstructure of pure Al at 130 N & 300 rpm
Fig-20 Microstructure of Alloy at 130 N & 300 rpm
Fig-21 Microstructure of MMNC at 130 N & 300 rpm
Figures 10, 11 and 12 present the FESEM micrograph of
worn out samples of pure aluminium, duralumin and
MMNC respectively under constant load of 100 N and
constant speed of 300 rpm. Figure 10 shows a wavy surface
which is formed because of the heat generation and
localized welding in pure aluminium. Since the surface is
sticky, the wear of aluminium becomes more. In figure 11,
deep cuts are observed due to non-uniform wear. In figure
12, a uniform worn out surface is observed throughout. This
occurs because of less wear and the peening effort of nano
particles embedded in the matrix.
In figure 13, only wavy surfaces are observed instead of
nodular ones. Grooves are also observed at some points.
This occurs because of the application of step load. When
higher load is applied, nodular surfaces are eliminated in
every step. When the higher load is applied at the last step,
at some points, grooves are observed due to localized
heating. Figure 14 presents the microstructure of the alloy
where, deep cuts and grooves are also observed due to step
load. The worn out surface is not uniform due to non-
uniform wear. Figure 15 presents the microstructure of
MMNC where, in addition to its smooth worn out surface,
some grooves are visible in few places due to the application
of step load. Grooves are formed instantly at some points at
the time of application of step load and it continues to be a
groove in the successive application of step load.
Figures 16, 17 and 18 present the FESEM pics of pure
aluminium, alloy and composite respectively at 130 N load
and speed of 300 rpm applied in step. At higher load, the
wear is more in all the cases. In case of pure aluminium, the
wear rate is so severe for which scratches as observed in fig.
16. In figure 17, deep scratches and ploughing action are
observed due to severe wear in case of alloy. In figure 18,
no scratch is observed as wear is very less compared to pure
Al and alloy.
Figures 19, 20 and 21 present the microstructure of worn out
surfaces of pure aluminium, alloy and MMNC respectively
under constant speed of 300 rpm and constant load of 130
N. Severe wear is observed in case of pure aluminium
compared to composite. Duralumin also experiences severe
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 24
wear compared to MMNC. In both the cases of aluminium
and alloy, ploughing action is observed. But in case of
MMNC, no ploughing action takes place thus keeping wear
uniform. This is because of the strengthening mechanism of
the nano particles embedded in the matrix. As the particles
are very small and are embedded in the matrix, no
projections are coming out of the surface which prevents
ploughing action.
5. CONCLUSION
As this paper reports the dry sliding wear behaviour of pure
aluminium, alloy and MMNC, the following conclusions
can be drawn.
(a) Wear decreases as the time duration increases.
(b) Wear decreases as the rolling distance increases.
(c) Wear increases with the increase in load.
(d) Wear increases with the increase in speed.
(e) Wear is more when load and speed are
applied/increased in steps.
(f) Force of friction increases with rise in load and speed
in case of MMNC.
(g) Resistance to wear and friction is more in case of
MMNC compared to aluminium and alloy.
The results shown by MMNC are encouraging in
comparison to pure aluminium and duralumin as far as wear,
material loss and friction force are concerned. This is
because of the strengthening mechanism due to uniform
dispersion of Al2O3 nano particles in the matrix. Addition of
nano alumina powder to aluminium increases the
mechanical and tribological properties of MMNC. It also
improves the hardness, yield strength, wear and abrasion
resistance of the composite [24]. Again this is light in
weight.
FUTURE SCOPE
More tests are required to be conducted to study all the
parameters varying the load, speed, time as well as weight
percentage of reinforcements. MMNCs can be prepared by
varying the weight percentage of alumina and by reinforcing
alumina in the matrix of duralumin. Even hybrid MMNCs
can be prepared using non-contact ultrasonic cavitation
method and tribological properties can be studied.
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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 25
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[26]. Ray Vyjainto Kumar, Padhi Payodhar, Jha B.B &
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Aluminium, Al-Alloy & Al-Alumina metal mtrix nano
composite in dry condition: part-II, IJRET, May 2015, Vol-
04, Iss-5, pp. 246-252.

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Wear characteristics of pure aluminium, al alloy & al-alumina metal mtrix nano composite in dry condition part-iii

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 17 WEAR CHARACTERISTICS OF PURE ALUMINIUM, AL-ALLOY & AL-ALUMINA METAL MTRIX NANO COMPOSITE IN DRY CONDITION: PART-III Vyjainto Kumar Ray1 , Payodhar Padhi2 , B. B. Jha3 , Tapas Kumar Sahoo4 1 Student of Ph.D., Mechanical Engineering Department, B.P.U.T., Bhubaneswar, Orissa, India 2 Principal, Mechanical Engineering Department, K.I.S.T., Bhubaneswar, Orissa, India 3 Chief Scientist, Metallurgical Engineering, Surface engineering department, I.M.M.T., Bhubaneswar, Orissa, India 4 Technical Assistant, Metallurgical Engineering, Surface engineering department, I.M.M.T., Bhubaneswar, Orissa, India Abstract In this report, the aluminium metal matrix was reinforced with 1.5 wt. % of Al2O3 nano particles using non-contact cavitation method to prepare the metal matrix nano composite. Microstructural examination conducted on the samples revealed a uniform distribution of alumina particulates. Sliding wear behavior of the as-cast MMNC was studied in dry condition, under different test conditions by varying the load and the sliding velocity, with an unlubricated Multiple Tribo Tester. It was found that resistance to sliding wear improved considerably with the addition of alumina nano particles. Microscopic examinations of the worn out surfaces of pure Al, Al-alloy (duralumin) and MMNC reveal that the MMNC has greater resistance to sliding wear compared to pure aluminium and duralumin. Wear increases with increase in load and sliding velocity. Wear is more when load and speed are increased in steps. Delamination and abrasion are the dominating types of wear observed. Keywords: Sliding Wear, Al2O3, MMNC, Duralumin, Delamination and Abrasion. --------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION With the development of new processing techniques and the demand for lighter materials with high strength and stiffness, high performance composite materials have been developed which show enhanced properties compared to traditional metals and alloys. Most of these high performance materials are metallic matrixes reinforced with fibre, particulate or whiskers. MMNCs are emerging as the most versatile materials for advanced structural, automotive, aviation, aerospace, defense applications because of their excellent combination of properties. In recent years, considerable interest has been paid in extending the use of these composite materials in marine environment [1, 2]. These MMNCs have emerged as the important class of advanced materials giving the prospect to tailor the material properties according to their needs. These materials differ from the conventional engineering materials because of their homogeneity [3]. Aluminium based MMNCs possess desirable properties like high specific stiffness, low density, high specific strength controlled co efficient of thermal expansion, increased fatigue resistance and superior dimensional stability at elevated temperatures etc. [4, 5]. The mechanical and tribological properties of the MMNCs can be improved by reinforcing various materials ranging from very soft materials like Graphite, Talc etc. to high hardened ceramic particulates like SiC, Al2O3, etc., [6, 7]. However, because of their high cost of production, their application in industries is slowed down. Casting Technology plays the key to overcome this problem, although several technical challenges exist. Achieving a uniform distribution of reinforcement within the matrix is a big challenge, which directly influences the properties and quality of the composite materials. The MMNCs possess excellent mechanical and tribological properties and are, therefore, considered as prospective engineering materials for various tribological applications [8-15]. It is reported by many researchers that sliding wear resistance and abrasion resistance of MMCs and MMNCs, reinforced with ceramic particulates like SiC, Al2O3, have improved [8-11]. When nano particles of quantity as small as 2 wt. percent are added, it enhances the hardness and yield strength by a factor as high as 2 [16]. There are several methods for the production of metal matrix nano composites which include mechanical alloying, vertex process, and spray deposition etc. But, the above processes are expensive. Solidification processing is a relatively cheaper route. Nano particulates tend to agglomerate during solidification processing as a result of Van der Waals forces and therefore, proper dispersion of the nano particulates in metal matrix is a challenge. In the present work, a non-contact method, where the ultrasonic probe is not in direct contact with the liquid metal, was attempted to disperse nano sized Al2O3 particulates in aluminum matrix. In this method, the mold was subjected to ultrasonic vibration [16-20]. But, no work has ever been reported on the dry sliding wear behavior of MMNCs produced by non-contact cavitation method [16, 21]. Therefore, in the present investigation, an attempt has been made to study the dry sliding wear
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 18 behavior of Al+1.5% by wt. Al2O3 MMNC, prepared by non-contact cavitation method, under different test conditions by varying applying loads and sliding speeds over a predefined time period. 2. EXPERIMENTAL PROCEDURE 2.1 Material Alumina is a high hardened ceramic material. The chemical composition of the composite (Al-Al2O3 1.5% by wt. nano particle) is shown in Table 1. The motto to design MMNC is to combine the metals & ceramic i.e. addition of high strength, high modulus refractory particles to ductile metal matrix to get tailor made properties. Table 1 Composition of Al-Al2O3 (1.5 wt. %) MMNC. Element Fe Mg Si Al Al2O3 Wt. % 1.3 0.43 0.26 96.51 1.5 Fig-1 HRTEM micrograph of Al2O3 nano powder The Nano composites are prepared by a non-contact ultrasonic solidification method by Padhi et al [16, 21]. 2.2 Preparation of MMNC The procedure for preparation of MMNC done by Padhi et al [16, 21] is as follows. The experimental set up is shown in Fig.1. It consists of an ultrasonic generator that generates ultrasonic waves, an ultrasonic chamber and steel mould. The mould was preheated to avoid thermal cracking. The preheated mould was kept in the ultrasonic chamber and the chamber was subjected to vibration at a frequency of 35 KHz. Liquid aluminum and alumina particulate (1.5 wt. %) having average size 10 nm were simultaneously poured into the vibrating mould from the mixing chamber. Fig-2: Experimental set up After the simultaneous pouring, the heating element was immediately brought down above the liquid metal in order to delay the solidification. The vibration was carried out for a period of five minutes to ensure complete mixing. The castings were obtained in both longitudinal and transverse section. Fig-3: HRTEM micrographs of Al-Al2O3 nano composite showing uniform distribution of nano particles 2.3 Wear Tests The experiments described here were carried out on a Multiple Tribo Tester (TR-5), Ducom make. In this Multiple Tribo Tester, the wheel rotates and the specimen, of size 6.35 x 6.35 x 9 mm, is pressed against the wheel .The specimen is held by the fixture. Loads ranging from 0 to 1000 N and speeds up to 2000 rpm can be applied to press the specimen against the periphery of the 20 mm thick, 60 mm diameter wheel. Since the specimen is held stationary and the wheel rotates, the sliding contact occurs between the wheel and the specimen and wear of both takes place as the load is applied for the predefined test duration. Here, the sliding wear tests were carried out under different load conditions and at different speeds for a period of 30 minutes or 1800 seconds. The test conditions are as follows. 1. Load of 100 N (constant), speed of 300 rpm (constant) and test duration of 30 minutes (1800 Seconds).
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 19 2. Step load of 50 N with step load 10 N, 5 minutes duration step, speed of 300 rpm (constant) and test duration of 30 minutes (1800 Seconds). 3. Load of 130 N (constant), step speed of 100 rpm with step of 100 rpm, time variation 10 minutes and test duration of 30 minutes (1800 seconds). 4. Load of 130 N (constant), speed of 300 rpm (constant) and test duration of 30 minutes (1800 seconds). 3. RESULTS AND DISCUSSION The aluminum, duralumin and MMNC specimens were subjected to the above said test conditions. Duralumin is an aluminum-copper alloy. In addition to aluminium, the main materials constituting duralumin are copper, manganese and magnesium. It is used in aviation and automobile industry. Fig-4: Wear verses time keeping speed constant at 300 rpm at two different load conditions of 100 N (constant) and 100 N (step load) for pure aluminium, duralumin (Al-alloy) and MMNCs. Figure-4 shows the graph between wear in (µm) verses ime in seconds for pure Aluminium, alloy and MMNC keeping speed constant at 300 rpm at two different load conditions of 100 N (constant) and 100 N (step load) . The sliding wear of commercially pure Aluminium, in both the conditions, shows that the wear increases w.r.t. time. In case of MMNCs, in both the cases, no significant variation of wear occurs. Also the maximum wear in case of MMNC is 300 µm under 100 N step load whereas it is reduced to 200 µm under 100 N constant load which occur after 1800 seconds i.e. entire time duration. In case of pure aluminium, wear increases drastically up to 1500 µm within 1000 seconds approximately under 100 N constant load, but it is reduced to 1350 µm within 900 seconds approximately under 100 N step load. Initially pure aluminium is sticking to the wheel under step load which indicates negative. In case of duralumin, the maximum wear is 500 µm under 100 N constant load and 600 µm under 100 N (step load). In all the cases, wear is more under step load condition. Hence it is concluded that the wear properties of composite is significantly increased compared to pure aluminium and alloy. -500 0 500 1000 1500 2000 2500 0 500 1000 1500 2000 wear(µm) time (sec.) wearvs time Al 130N 300rpm comp. 130N 300rpm duralumin 130 N 300 rpm comp. 130N, 300 rpm(step) Al 130N,300rpm(step) duralumin 130N 300rpm(step) Fig-5: Wear verses time keeping load constant at 130 N at two different speeds of 300 rpm (constant) and 300 rpm (step) for pure Al, duralumin and MMNC. Figure-5 shows the wear verses time keeping load constant at 130 N at two different speeds of 300 rpm (constant) and 300 rpm (step) for pure aluminium, duralumin and MMNC. It is observed that wear of MMNC, which is 750 µm under 300 rpm constant speed, increases gradually and linearly as time increases up to 1800 seconds. But under 300 rpm step speed, wear increases linearly up to 1500 µm approximately till 1400 seconds are covered and then to 2300 µm suddenly and gets worn out after 1550 seconds. In case of pure aluminium, the wear increases to 1500 µm at 1000 seconds during 300 rpm step speed condition and under 300 rpm constant speed condition, the wear comes down to 1300 µm approximately at 700 seconds. Similarly, in case of alloy, the maximum wear is 2000 µm under constant speed condition within 400 seconds and the maximum wear is 1600 µm under step speed condition within 1600 seconds. Initially the alloy is sticking to the wheel under step load which indicates negative. In all the cases, wear is more under step speed condition. Again, it is concluded that the wear properties of composite is significantly increased compared to pure aluminium and alloy.
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 20 Fig-6: Weight loss verses sliding distance keeping speed constant at 300 rpm at two different load conditions of 100 N (constant) and 100 N (step load) for pure Al, duralumin and MMNC. Figure-6 shows weight loss verses sliding distance keeping speed constant at 300 rpm under two different load conditions 100 N constant and 100 N step. At constant load, for MMNC, weight loss is initially high and gradually decreases to nearly zero and maintains a steady state till sliding distance 2000 meters. This happens due to the embodied of nano particles in the aluminium matrix. Weight loss for MMNCs at step load conditions is initially more and gradually decreases to very small amount till 600 meters of sliding distance then again decreases to almost zero and continues to 1800 meters sliding distance. This is due to the application of step load because during the transition period, the wear rate decreases and subsequently it maintains steady state. In case of pure aluminium, at constant load, weight loss of material varies significantly as shown in the Figure 6. Initially the material loss is very high (2800 µm), then decreases to negative value due to sticking to the wheel, then again increases and at 1000 meters of sliding distance, complete worn out takes place. During the step load condition, when sliding distance exceeds 50 meters, weight loss increases to 1700 µm, then drastically decreases to negative value due to sticking to the wheel, then again increases and at 1000 meters of sliding distance, complete worn out takes place. The weight loss for composites, in both the cases, is initially high and then decreases to almost zero as sliding distance increases up to 2000 meters. This happens due to increase of hardness as alumina nano particles embedded in the aluminium matrix. But still here is a difference of weight loss between constant load and step load. During step load, weight loss is more compared to constant load. This is due to the frequent increase of load. Weight loss increases at each step, which is very less. In case of duralumin, under constant load 100 N, wt. loss increases up to 900 µm, then falls to negative value for sticking to the wheel, then rises and continues up to 2000 meters at almost constant rate. But under step load condition, the alloy specimen sticks to the wheel initially showing negative wt. loss. The wt. loss then rises up to 3000 µm, then falls to negligible value and continues up to 1850 meters of sliding distance. Weight loss is more when speed is increased in steps. Fig-7: Weight loss verses sliding distance keeping load constant at 130 N at two different speeds of 300 rpm (constant) and 300 rpm (step) for pure Al, duralumin and MMNC. Figure-7 shows weight loss verses sliding distance keeping load constant at 130 N under constant and step speed conditions. Weight loss for MMNC specimen at both speed conditions is nearly zero though there is a little difference which is not so significant where as in case of pure aluminium, weight loss of material varies significantly as shown. Initially the material is sticking to the wheel which indicates negative. For duralumin, under 130 N constant load and 300 rpm constant speed, wt. loss rises to 6500 µm initially, then falls to around 500 µm and continues up to 300 meters of sliding distance. Under 300 rpm step speed and 130 N constant load, alloy initially sticks to the wheel showing negative wt. loss and then continues up to 1600 meters. In all the cases, weight loss is more during step speeds. This happens when speed changes step wise, at each step the wt. loss increases and stabilizes after certain time. This phenomena continues till the end. At constant speed, initially weight loss is high and decreases to negligible amount after few sliding distance and then maintains the same.
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 21 Fig-8: Force of friction verses time keeping speed constant (300 rpm) at two different load conditions of 100 N constant and 100 N step for pure Al, duralumin and MMNC. Figure-8 shows the graph between force of friction verses time keeping speed constant at two different load conditions. For MMNC, the force of friction is almost constant in two loading conditions, over the entire time period and is more when load is applied in step. In case of pure aluminium, force of friction is negative i.e. friction resistance is almost zero under both the load conditions. For duralumin, the force of friction is almost constant over the entire time period under constant load condition where as it is negative when load is increased in steps because it sticks to the wheel. Friction resistance is more in case of MMNC. Fig-9: Force of friction verses time keeping load constant (130 N) at two different speed conditions of 300 rpm (constant) and 300 rpm (step) for pure Al, duralumin and MMNC. Figure-9 shows the graph between force of friction verses time (seconds) keeping load constant at 130 N under two different speed conditions i.e. 300 rpm (constant) and 300 rpm (step). For MMNC, the friction force is maximum initially and then remains almost constant under constant speed condition of 300 rpm over the entire time period, while under the step speed condition of 300 rpm, it is also maximum at many points of the curve, but fluctuating significantly as speed is applied stepwise over a time period of 1700 seconds. In case of pure aluminium, force of friction is negative in both the cases. As the material is sticking to the wheel, the characteristic curves of aluminium in both the cases show negative. For alloy, as the material is sticking to the wheel, the characteristic curves in both the cases show negative. 4. MICROSCOPIC EVALUATION The microstructure of the worn out samples were evaluated under FESEM. The FESEM images are shown in the figures below. Fig-10 Microstructure of pure Al at 100N and 300 rpm Fig-11 Microstructure of alloy at 100N and 300 rpm
  • 6. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 22 Fig-12 Microstructure of MMNC at 100N and 300 rpm Fig-13 Microstructure of Al at 100 N (step) & 300 rpm Fig-14 Microstructure of alloy at 100 N (step) & 300 rpm Fig-15 Microstructure of MMNC at 100 N (step) & 300 rpm Fig-16 Microstructure of pure Al at 130 N & 300 rpm (step) Fig-17 Microstructure of Alloy at 130 N & 300 rpm (step)
  • 7. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 23 Fig-18 Microstructure of MMNC at 130 N & 300 rpm (step) Fig-19 Microstructure of pure Al at 130 N & 300 rpm Fig-20 Microstructure of Alloy at 130 N & 300 rpm Fig-21 Microstructure of MMNC at 130 N & 300 rpm Figures 10, 11 and 12 present the FESEM micrograph of worn out samples of pure aluminium, duralumin and MMNC respectively under constant load of 100 N and constant speed of 300 rpm. Figure 10 shows a wavy surface which is formed because of the heat generation and localized welding in pure aluminium. Since the surface is sticky, the wear of aluminium becomes more. In figure 11, deep cuts are observed due to non-uniform wear. In figure 12, a uniform worn out surface is observed throughout. This occurs because of less wear and the peening effort of nano particles embedded in the matrix. In figure 13, only wavy surfaces are observed instead of nodular ones. Grooves are also observed at some points. This occurs because of the application of step load. When higher load is applied, nodular surfaces are eliminated in every step. When the higher load is applied at the last step, at some points, grooves are observed due to localized heating. Figure 14 presents the microstructure of the alloy where, deep cuts and grooves are also observed due to step load. The worn out surface is not uniform due to non- uniform wear. Figure 15 presents the microstructure of MMNC where, in addition to its smooth worn out surface, some grooves are visible in few places due to the application of step load. Grooves are formed instantly at some points at the time of application of step load and it continues to be a groove in the successive application of step load. Figures 16, 17 and 18 present the FESEM pics of pure aluminium, alloy and composite respectively at 130 N load and speed of 300 rpm applied in step. At higher load, the wear is more in all the cases. In case of pure aluminium, the wear rate is so severe for which scratches as observed in fig. 16. In figure 17, deep scratches and ploughing action are observed due to severe wear in case of alloy. In figure 18, no scratch is observed as wear is very less compared to pure Al and alloy. Figures 19, 20 and 21 present the microstructure of worn out surfaces of pure aluminium, alloy and MMNC respectively under constant speed of 300 rpm and constant load of 130 N. Severe wear is observed in case of pure aluminium compared to composite. Duralumin also experiences severe
  • 8. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 07 | July-2015, Available @ http://www.ijret.org 24 wear compared to MMNC. In both the cases of aluminium and alloy, ploughing action is observed. But in case of MMNC, no ploughing action takes place thus keeping wear uniform. This is because of the strengthening mechanism of the nano particles embedded in the matrix. As the particles are very small and are embedded in the matrix, no projections are coming out of the surface which prevents ploughing action. 5. CONCLUSION As this paper reports the dry sliding wear behaviour of pure aluminium, alloy and MMNC, the following conclusions can be drawn. (a) Wear decreases as the time duration increases. (b) Wear decreases as the rolling distance increases. (c) Wear increases with the increase in load. (d) Wear increases with the increase in speed. (e) Wear is more when load and speed are applied/increased in steps. (f) Force of friction increases with rise in load and speed in case of MMNC. (g) Resistance to wear and friction is more in case of MMNC compared to aluminium and alloy. The results shown by MMNC are encouraging in comparison to pure aluminium and duralumin as far as wear, material loss and friction force are concerned. This is because of the strengthening mechanism due to uniform dispersion of Al2O3 nano particles in the matrix. Addition of nano alumina powder to aluminium increases the mechanical and tribological properties of MMNC. It also improves the hardness, yield strength, wear and abrasion resistance of the composite [24]. Again this is light in weight. FUTURE SCOPE More tests are required to be conducted to study all the parameters varying the load, speed, time as well as weight percentage of reinforcements. 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