- Open Access
- Total Downloads : 363
- Authors : Ahmed Saifeldeen Mohamed, Hossam Kamal Ibrahim, Osama Kamal Mohamed, Abdelnaser Abdelhameed Zayed
- Paper ID : IJERTV5IS020228
- Volume & Issue : Volume 05, Issue 02 (February 2016)
- Published (First Online): 22-02-2016
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Experimental Determination of Mechanical Properties of Chopped Fiber Composite Materials
Ahmed Saifeldeen Mohamed
Ph. D. Student , Military Technical College Egyptian Armed Forces,
Cairo, Egypt Hossam Kamal Ibrahim
PH.D. Egyptian Armed Forces
Abstract- Mechanical properties of chopped composites are one of the most important parameter for determining the application of the use of these materials. An experimental identification for mechanical properties of different composite material was conducted. Tensile test at different temperatures, -40°c, 25°c (normal), 100 °c and 200 °c were done. Three different chopped composites which are Carbon fiber, Basalt and Fiber glass with a phenol resin as a matrix were selected to determine their mechanical properties. For comparison with the previous type of composite materials, a carbon fiber with epoxy resin as a matrix was selected. Carbon fiber with the epoxy was the highest mechanical properties among these materials, but when the temperature raised, its tensile property deteriorated whereas the carbon fiber with the phenol withstand the elevated temperatures. Three point bending and compression tests were done for these materials; Carbon fiber with Epoxy was the highest properties. Hardness test as another important factor was done for those composite materials. The four materials are in the rigid zone but also carbon fiber with epoxy was the hardest material among the selected materials.
Keywords: Composite, Chopped Fiber, Mechanical Properties, Tensile Test, Compression Test, Hardness.
-
INTRODUCTION
A composite is made up of different components and combining their essential or typical characteristics while preserving their separate identities. Composite materials became an important factor in modern technological society, especially for applications requiring great strength and light weight such as in the aerospace industry. Because these materials are hybrid heterogeneous materials, they can be difficult to characterize with any one single methodology [1]. Woven fabrics composites give an assortment of alluring properties, since they have high ability to adjust to complicated shapes. This is suitable for manufacturing parts with complicated shapes and more adaptability in processing operation compared to metals and even their chopped counterparts [2]. Knowing the mechanical behavior of these fabrics is important in many applications in particular for the simulation of textile composite forming. Shearing behavior of woven performs is the most considered mechanical property, since this mechanism of deformation is important for shaping on double curvature surfaces. [3-7].
Osama Kamal Mohamed
Ph. D. Military technical college
Abdelnaser Abdelhameed Zayed
Prof., Heliopolis University, Engineering Faculty Cairo, Egypt
Characterization of such materials has a great deal of consideration. The objectives are usually have two phases: to know the non-linear mechanical reaction of the materials during shear and to describe the cutoff of distortion. Many researches have been done on the mechanical properties of composite materials behavior. [813].
Improvement of new materials is turning out to be progressively difcult because of increased environmental concerns and because the number of useful materials made from simple components is limited. Composite materials can be narrowly dened to be ber-reinforced polymers, such as carbon ber-reinforced epoxy/phenol resin, fiber glass reinforced phenol and basalt. However, as composite technology has advanced, the denition of composite materials has become broader, to include materials such as molecular composites and Nano-composites which are also similar to immiscible blends. From a characterization perspective, these materials can be treated as heterogeneous materials.
In this work three different composite materials carbon fiber, basalt and fiber glass with phenol as a matrix were selected to determine its tensile strength and hardness. Carbon fiber was selected again with epoxy as a matrix to compare the results with the previous one.
-
EXPERIMENTAL WORK
For identifying material mechanical properties, four composite materials were studied experimentally. The steps conducted to achieve the tensile (at different temperatures), bending, compression and hardness of these materials, are illustrated in the following
-
Preparing the Tested Samples
Four composite materials were selected to obtain their characteristics which are Basalt with phenol as a resin, Fiber glass with phenol as a resin, Carbon fiber with phenol as a resin and Carbon fiber with epoxy as a resin [14].For the Carbone with Epoxy resin a mixture of fiber and resin was prepared and mixed together then cured under pressure only at normal temperature. For the three materials mixed with the Phenol, a mixture of chopped fiber Figure 1 and resin was prepared and mixed together and then cured under pressure and temperature to obtain composite materials in the sheets shape of dimensions 300 *300* 3 mm in the cured stage as shown in Figure 2.
The JANNAF (Joint Army-Navy-NASA-Air Force Propulsion Committee) specimens [16-18] with dimensions as shown in Figure 4 were used instead of the strip specimens to avoid these problems. Sample specimens were cut according to the JANNAF standard as shown in Figure 5.
127
Fig. 1 Chopped Carbon fiber, Chopped Fiber glass and Chopped Basalt
To obtain the mechanical properties of these materials some tests might be done which are tensile test, three point bending, the compression test and the hardness test. According to the DIN 3039[15], the specimens were cut to make strips with dimensions 250x25x3.5mm. Tapping material was used at the both ends of the specimens as shown in Fig 3
Fig. 2 Carbon fiber, Basalt, Fiber glass and Carbon/epoxy sheets
.
9:10
.
9:10
3:5
74.4
25.4
25.4
50.8
R12.7
Fig. 4 Standard sample dimension with JANNAF
Fig. 5 JANNAF samples for Basalt, Carbon fiber, Fiber Glass and Carbon
/ Epoxy
Fig. 3 Carbon fiber, Basalt and Fiber glass specimens
The tensile test has been done to the strip specimens shown in the figure 3 for three materials which are carbon fiber, basalt and fiber glass. Two problems occurred which are the slipping of the specimens from the tapping material and sliding was occurred between the tapping material and the jaws.
-
Test machine
The ZWICK Z050 universal test machine has been used for carrying out all the mechanical tests. This machine has remote control software which could acquire record, analyze, store and print test data with minimum manual effort. The maximum permissible test load is 10KN, and the range of crosshead speed varies from 0.0005 to 1000 mm/min with accuracy 0.004 % of the set speed. The machine is provided with temperature chamber having a range varies from -70 to +250 ºc.
-
Test plane
The specimens were prepared to satisfy the mechanical tests requirements as shown in table 1 for the tensile tests, it was done at deferent temperatures which were (-40°c, 25°c,
100°c and 200°c). At the normal temperature 3 specimens were prepared for each material, at -40 °c 2 specimens were prepared for each material and one specimen for both 100 °c and 200°c. In total, 28 specimens were prepared for the tensile test.
For the compression and three points bending tests three specimens for each material were prepared with a total number of twelve specimens for each test an the both tests were done at normal temperature as shown in table 1.
Table 1 Test specimens plane
Table 2 Bending test results of the Basalt
Spec. No.
Max. Stress Mpa
Max. strain %
Break Stress Mpa
Strain at break%
Q =
1
20.8
0.79
19.5
0.91
2
21.62
0.85
20.5
1.02
3
20.2
0.82
19.5
0.97
The mean
20.87
0.82
20
0.9667
=
13.125
Spec. No.
Max. Stress Mpa
Max. strain %
Break Stress Mpa
Strain at break%
Q =
1
20.8
0.79
19.5
0.91
2
21.62
0.85
20.5
1.02
3
20.2
0.82
19.5
0.97
The mean
20.87
0.82
20
0.9667
=
13.125
Test
No. of Materials
total
-40 °c
25 °c
100 °c
200 °c
Tensile
2
3
1
1
4
28
Compression
3
4
12
3 point bending
3
4
12
Test
No. of Materials
total
-40 °c
25 °c
100 °c
200 °c
Tensile
2
3
1
1
4
28
Compression
3
4
12
3 point bending
3
4
12
3.1.3 The compression test
For the compression test the results were as shown in table 3
Table 3 Compression test results of the Basalt
Spec. No.
Max. Stress
Max. strain
Break Stress
Strain at break
=
1
343.23
4.4
326.56
4.6
2
318.7
4.9
300
5.7
3
346.2
3.1
345.19
3.2
The mean
336.04
4.13
323.94
4.5
= 211.35
Spec. No.
Max. Stress
Max. strain
Break Stress
Strain at break
=
1
343.23
4.4
326.56
4.6
2
318.7
4.9
300
5.7
3
346.2
3.1
345.19
3.2
The mean
336.04
4.13
323.94
4.5
= 211.35
-
-
MEASURED DATA
-
For the Basalt
-
The tensile test
Max. Stress
MPa.
Max. Stress
MPa.
The values of the maximum stresses at different temperatures were as shown in figure 6:
Basalt
30
20
10
0
-50 0 50 100 150 200 250
Temp. °c
Basalt
30
20
10
0
-50 0 50 100 150 200 250
Temp. °c
FIG. 6 Tensile strength of Basalt
At normal temperature, the maximum stress for the Basalt reaches 19.8 Mpa and at -40°c it reaches 15.6 Mpa with a decreasing percentage of 20%. When the temperature rises to 100 °c, the stress decreases to 4.66 Mpa with a decreasing percentage of 76% and at 200°c the stress decreases again to 3.2 Mpa with a decreasing percentage of 83.8%.
-
Three point bending test
-
For the three points bending the results for the three specimens were as shown in table 2:
The maximum stress for the three samples varies from
20.2 Mpa to 21.6 Mpa where the strain varies from 0.79% to 0.85%.
Here the maximum stress for the compression test for the Basalt varies from 318.7 Mpa to 346.2 Mpa where the strain varies from 3% to 4.9%.
3.1.4 The Hardness test:
The value of hardness of the Basalt is 82 Shore D which means that it is in the hard zone.
-
For the Fiber glass
-
The tensile test
Max. Stress
MPa.
Max. Stress
MPa.
The values of the maximum stresses at different temperatures were as shown in figure 7:
Fiber Glass
Fiber Glass
25
20
15
10
5
0
25
20
15
10
5
0
-50
50
150
250
-50
50
150
250
Temp. °c
Temp. °c
FIG. 7 Tensile strength of Fiber Glass
At normal temperature, the maximum stress for the Fiber glass reaches 22.26 Mpa and at -40 °c it was 20.2 Mpa with a decreasing percentage of 9.25%. When raising the temperature to 100 °c the stress decreases to 11.66 Mpa with a decreasing percentage of 47.5% and at 200 °c the stress decreases again to 3.56 Mpa with a decreasing percentage of 83.9 %.
-
Three point bending test
For the three points bending the results were as shown in table 4
-
-
For the Carbon with phenol:
-
The tensile test
-
The values of the maximum stresses at different temperatures were as shown in figure 8:
Carbon fiber
Carbon fiber
30
20
10
0
30
20
10
0
Max. Stress
MPa.
Max. Stress
MPa.
Table 4 Bending test results of the Fiber glass
-50
50
150
250
-50
50
150
250
Temp. °c
Temp. °c
Spec. No.
Max. Stress Mpa
Max. strain
Break Stress Mpa
Strain at break
=
1
43.4
0.42
30.8
0.43
2
45
0.59
32.1
0.65
3
47.9
0.71
34.4
0.77
The mean
45.433
0.57
32.4
0.62
= 211.35
Spec. No.
Max. Stress Mpa
Max. strain
Break Stress Mpa
Strain at break
=
1
43.4
0.42
30.8
0.43
2
45
0.59
32.1
0.65
3
47.9
0.71
34.4
0.77
The mean
45.433
0.57
32.4
0.62
= 211.35
For the bending test of the Fiber glass, the results of the maximum stress varies from 43.4 Mpa to 47.9 Mpa where the strain varies from 0.42% to 0.71%
-
The compression test
For the compression test the results were as shown in table 5:
Stress Mpa
Stress Mpa
break
break
Table 5 Compression test results of the Basalt
Spec.
No.
Max.
Max. strain
Break Stress
Mpa
Strain at
Q =
1
309.89
1.5
308.9
1.5
2
298.22
1.4
297.23
1.4
3
322.6
1.6
321.65
1.6
The mean
310.18
1.5
309.2
1.5
= 179.29
For the compression test of Fiber Glass, the maximum stress varies from 298.22 Mpa to 322.6 Mpa where the strain varies from 1.4% to 1.6%.
-
The Hardness test
The value of hardness of the Fiber glass is 78 Shore D which means that it is in the hard zone.
FIG. 8 Tensile strength of Carbon/phenol
At normal temperature, the maximum stress for the Carbon/phenol reaches 28 Mpa and at -40 °c it was 24.7 Mpa with a decreasing percentage of 11.5 %. When temperature rises to 100 °c the stress decreases to 11.27 Mpa with a decreasing percentage of 60 % and at 200 °c the stress decreases again to 6.14 Mpa with a decreasing percentage of 78%.
3.3.2 Three point bending test
For the three points bending the results were as shown in table 6:
=
=
Table 6 Bending test results of the Carbon/phenol
Spec. No.
Max. Stress
Max. strain
Break Stress
Strain at break
1
35.2
0.8
24.6
1.2
2
37.5
0.5
26.3
0.87
3
35.4
0.45
22.8
0.53
The mean
36
0.58
24.5
0.86
= 24.65
For the bending test of the carbon with phenol the Maximum stress varies from 35.2 Mpa to 37.5 Mpa where the strain varies from 0.45% to 0.8%.
.3.3 The compression test
For the compression test the results were as shown in table 7:
Table 7 Compression test results of the Carbon/phenol
Spec. No.
Max. Stress
Max. strain
Break tress
Strain at break
=
1
743.3
2.8
743.3
2.8
2
728.6
2.5
727.7
2.6
3
753.2
3.1
752.2
3.3
The mean
741.7
2.8
741
3
= 508
For the compression test of Carbon/phenol, the maximum stress varies from 728.6 Mpa to 753.2 Mpa where the strain varies from 2.5% to 3.1%.
3.3.4 The Hardness test
The value of hardness of the Carbon/phenol is 80 Shore D which means that it is in the hard zone.
-
For the Carbon with Epoxy:
-
The tensile test
Max. Stress
MPa.
Max. Stress
MPa.
The values of the maximum stresses at different temperatures were as shown in figure 9:
Carbon / Epoxy
100
80
60
40
20
0
-50 50 150
250
Carbon / Epoxy
100
80
60
40
20
0
-50 50 150
250
Temp. °c
Temp. °c
FIG. 9 Tensile strength of Carbon/Epoxy
At normal temperature, the maximum stress for the Carbon/Epoxy reaches 64.82 and at -40°c it was 77.5
with an increasing percentage of 19.5%. When the temperature rises to 100°c the stress decreases to 5.6 with a decreasing percentage of 91.4 % and at 200 °c the stress decreases again to 2.38 with a decreasing percentage of 96.3%.
-
Three point bending test
For the three points bending the results were as shown in table 8:
Table 8 Bending test results of the Carbon/Epoxy
Spec. No.
Max. Stress
Max. strain
Break Stress
Strain at break
=
1
55.5
0.99
39.6
1.1
2
51
0.92
34.3
0.97
3
56.5
1
38.7
1.1
The mean
54.3
0.92
37.5
1.1
= 42.75
For the bending test of the carbon with epoxy the Maximum stress varies from 51 to 56.5 where the strain varies from 0.92% to 1%.
-
The compression test
For the compression test the results were as shown in table 9:
Table 9 Compression test results of the Carbon/Epoxy
Spec. No.
Max. Stress
Max. strain
Break Stress
Strain at break
=
1
831.6
5.6
830..6
5.6
2
866
3.6
854.5
4.4
3
848.3
4
.6
838.2
4.6
The mean
848.6
4.6
841.1
4.86
= 668.2
For the compression test of carbon/ epoxy the maximum stress varies from 831.6 Mpa to 866 Mpa where the strain varies from 3.6% to 5.6%.
-
The Hardness test
The value of hardness of the Carbon/Epoxy was 90 Shore D which means that it is in the hard zone.
-
-
Comparison of Measured Data in the Tensile Strength
-
Comparison of materials with the same resin
As mentioned before, three materials with the same resin were selected so when making a comparison between these materials figure 10, the comparison here is between the fibers itself.
It is noticed that the max stress of the three materials takes the same behavior at the different temperature. It has a low value at freezing temperature compared by its value at room temperature. When the temperature rises, the stress decreases to lower values.
From the previous char it is noticed that the Carbone fiber was the highest stress values among the selected materials at different temperatures and the Basalt was the lowest stress at the same temperatures.
30
20
10
30
20
10
Max. Stress Mpa
Max. Stress Mpa
If we assume a ratio factor between the ultimate tensile strength and the density of the materials we will have the following results: 12.48 for the basalt, 12.87 for the fiber glass, 19.16 for the carbon/phenol and 59.05 for the carbon/epoxy.
Comparison of Max. Stress
for material with the same resin
Comparison of Max. Stress
for material with the same resin
Carbone
Fiber
Fiber glass
Carbone
Fiber
Fiber glass
0
-50 0 50 100150200250 Basalt
Temperature °c
0
-50 0 50 100150200250 Basalt
Temperature °c
FIG. 10 Comparison of stress for materials with the same resin
-
Comparison of materials with the same Fiber
-
100
80
60
40
20
0
-50
100
80
60
40
20
0
-50
Carbone
phenole
Carbone
phenole
Max. Stress Mpa
Max. Stress Mpa
Here is a comparison between the same fibers with using two different resins as shown in figure 11:
Comparison of Max. Stress
for materials with the same fiber
Comparison of Max. Stress
for materials with the same fiber
Carbone
Epoxy
Carbone
Epoxy
0 50 100 150 200 250
Temperature °c
0 50 100 150 200 250
Temperature °c
FIG. 11 Comparison of stress for materials with different resin
Here it is noticed that the Carbone / Epoxy stress is more higher than Carbone/ Phenol but at elevated temperatures, the stress of the Carbone / Epoxy deteriorate with percentage of 96.8% and reaches 2.38 Mpa while the stress of the Carbone/Phenol decreased with a percentage of 77.84% and reaches 6.14 Mpa.
-
Comparison of Measured Data in the Bending Test
The Carbon with Epoxy has the highest value in bending test which reaches 54.3 where the Basalt has the lowest value of the bending by the value of 21.
When assuming a ratio factor between the flexure and the density of the materials we get the following data: 13.125 for basalt, 26.26 for the fiber glass, 24.65 for the carbon/phenol and 42.75 for the carbon/epoxy. It is obvious the carbon/epoxy has the highest ratio among the selected materials.
-
Comparison of Measured Data in the compression test The Carbon /Epoxy has also the highest value of the compression test by the value of 848.6 where the Fiberglass has the lowest value of 310.2 .
When assuming a ratio factor between the compression and the density of the materials we get the following data:
211.35 for basalt, 179.29 for the fiber glass, 508 for the carbon/phenol and 668.2 for the carbon/epoxy. it is obvious the carbon/epoxy has the highest ratio among the selected materials.
3.8 Hardness test results
Hardnesss
Shore D
Hardnesss
Shore D
The values of the Hardness of the composite material are as shown in figure 12:
Hardness
95
90
85
80
75
70
Composite type
Hardness
95
90
85
80
75
70
Composite type
FIG. 12 Measured Data of Hardness test
-
-
CONCLUTION
The results show that for carbon/phenol, it reaches its maximum strength at the normal temperature which was 28 Mpa and it can withstand the high temperature (200 ºc) and its strength reaches 0.22% of its strength at normal temperature. For the carbon / epoxy it also reaches its maximum strength at the normal temperature which was
64.8 MPa but at high temperature its strength decrease to 0.03% from its strength at normal temperature. For the fiber glass it also reaches its maximum strength at the normal temperature which was 22.26 Mpa and at high temperature its strength reaches 0.18% of its strength at normal temperature. For basalt it reaches its maximum strength at the normal temperature which was 19.8 Mpa and at high temperature its strength reaches 0.23% of its strength at normal temperature.
For Hardness, the four materials are almost in the same range but also the carbon fiber with epoxy is the most rigid one.
The results show that at normal temperature, the carbon with epoxy is the highest tensile properties and the highest hardness among the selected materials. But when the temperature rose, the carbon fiber with phenol is the highest one.
The mechanical properties for the selected composite materials are now known. The JANNAF standard is more efficient for getting accurate results for the chopped composite materials.
The Carbone fiber with the epoxy resin is the highest mechanical properties among the selected composite materials at room temperature.
At higher temperatures, Carbon fiber with phenol resin can withstand this temperature better than carbon fiber with epoxy resin.
For the hardness, the four selected composite materials are in the hard zone which is greater than 50 but the carbon fiber with epoxy is the hardest one.
REFRENCES
-
Hatsuo Ishida, C. Richard Brundle, Charles A. Evans, Jr. Characterization of Composite Materials ISBN: 978-1-60650-191- 7 momentum press.
-
Khan MA, Mabrouki T, Vidal-Salle´ E, et al. Numerical and experimental analyses of woven composite reinforcement forming using a hypoelastic behaviour. Application to the double dome benchmark. J Mater Process Technol 2009; 210: 378388.
-
Hamila N and Boisse P. A mesomacro three node finite element for draping of textile composite preforms. Appl Comp Mater 2007; 14: 235250.
-
Pora J. Composite materials in the airbus A380 from history to future. In: 13th international conference on composite materials (ICCM-13), Beijing, China, July 2001.
-
Sinke J. Manufacturing of glare parts and structures. Application of Composites Materials. 2003; 10: 293305.
-
TP Sathishkumar, P Navaneethakrishnan1, S Shankar and J Kumar Mechanical properties of randomly oriented snake grass fiber with banana and coir fiber-reinforced hybrid composites Journal of Composite Materials 47(18) 21812191
-
Jeno Sándor SZABÓ, Zoltán KOCSIS and Tibor CZIGÃNY Mechanical Properties of Basalt Fiber Reinforced PP/PA Blends Periodic Polytechnic. MECH. ENG. VOL. 48, NO. 2, PP. 119132 (2004)
-
Badel P, Vidal-Salle´ E and Boisse P. Computational determination of the mechanical behavior of textile composite reinforcement. Validation with x-ray tomography. Int J Mater Form 2008; 1: 823 826.
-
Gasser A, Boisse P and Hanklar S. Mechanical behavior of dry fabric reinforcements. 3D simulations versus biaxial tests. Comput Mater Sci 2000; 17: 720.
-
Ishikawa T and Wei Chou T. Nonlinear behavior of woven fabric composites. J Comp Mater 1983; 17: 399413.
-
Glaessgen EH, Pastore CM, Griffin OH, et al. Geometrical and finite element modelling of textile composites. Compos B: Eng 1996; 27: 4350.
-
Bigaud D and Hamelin P. Mechanical properties prediction of textile-reinforced composite materials using a multiscale energetic approach. Compos Struct 1997; 38: 361371.
-
Daghboudj Samir and Satha Hamid Determination of the in-plane shear rigidity modulus of a carbon non-crimp fabric from bias- extension data test, Journal of Composite Materials 2014, Vol. 48(22) 27292736
-
P.Amuthakkannan,V.Manikandan,e al Effect Of Fiber Length and Fiber Content on Mechanical Properties of Short Basalt Fiber Reinforced Polymer Matrix Composite Material Physics and Mechanics 16 (2013) 107-117,Jan. 2013
-
Neviee R., An Extension of the Time-Temperature Superposition Principal to nonlinear Viscoelastic Solids, Int. J. of Solid and Str., Vol. 43, 2006, pp. 5295-5306.
-
Raghavendra Gujjala, Shakuntala Ojha1, SK Acharya and SK Pal Mechanical properties of woven juteglass hybrid-reinforced epoxy composite Journal of Composite Materials 2014, Vol. 48(28) 3445 3455
-
L.T. Harper, T.A. Turner, N.A. Warrior, J.S. Dahl and C.D. Rudd Characterization of random carbon fiber composite from a direct fiber performing process: Analysis of microstructural parameters composite: part A 37 (2006) 2136-2147
-
D.Alain, Solid Rocket Propulsion Technology, Pergamon Press,ISBN 0-08-040999-7,1993.
-
Solid propellant grain structural integrity analysis. NASA, Lewis Research Center (Design Criteria Office), Cleveland, Ohio – 44135, USA. Report No. NASA SP-8073. June, 1973.
-
Structural assessment of solid propellant grains. Advisory Group for Aerospace Research and Development. (AGARD), 7 Rue Ancelle, 92200 Neuilly-Sur-Seine, France. Report No. AGARD-AR-350, December 1997.