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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1059
Impact Analysis of Density Graded E-Glass Composite Laminate
Sedulingam Kandaswamy1, Deepthi K R2
1PG Scholar, 2Assistant Professor
1, 2 Dept. of Mechanical Engineering, New Horizon College of Engineering, Karnataka, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - E-Glass/Polyester composite laminates are
subjected to low velocity impact and their behavior is
analyzed. To investigate the impact strength, the laminate is
fabricated by hand-layup process. E-glass fiber mats of
different densities are used in the fabrication. Due to the cost
and complexity related to impact experiments itisnotoptimal
to base all impact related studies on laboratory tests alone.
Therefore, to reduce the experimentationcostfewsamplesare
fabricated and tested in laboratory using drop weight impact
tester, further numerical simulation of impact on composite
laminate is investigated using 3-D dynamic explicit finite
element code. ANSYS/AUTODYN whichis generalpurposenon-
linear dynamic modeling and simulation software. Trial
simulations are conducted and results are validated.
Key Words: Impact, E-Glass/Polyester, Density Grading,
Deformation, Energy Absorption.
1. INTRODUCTION
A composite is a material consisting of two or more
distinctive materials which acts as isotropic materials on a
macroscopic level but has anisotropic properties at
microscopic level. They are designed and fabricated to be
superior to those of the constituent materials acting
independently. Composite materials have significant design
advantages in the aerospace industry. The combined
properties such as light weight and high strength are the
most attractive feature for the aerospace and aircraft
designs. Composite materials are formed when two or more
chemically distinct materials are combined in such a way
that a distinct interface separates the components (as
opposed to alloys). Each of the constituent materials has its
own specific physical andchemical properties,thusresulting
in composite which has different properties from each
material alone. The composite for the impact protection is
generally fibrous or continuous fiber reinforced. This type
consists of one phase, which is usually much stronger i.e.
fiber, than the other phase i.e. matrix. This unique mixture
leads to anisotropic properties for the composite which
provide the specific characteristic of obtaininghighstrength
in one critical direction.
2. PROBLEM DESCRIPTION
The density graded E-glass composite laminate was
investigated on low velocity impact using experimental
setup and finite element analysis software. The finite
element software used in this study was AnsysAutodyn.The
complicated response of composite laminate along with the
high cost of fabrication limits the number of laminates
considered for experimentation. In order to overcome this
issue, finite element analysis can be used to find out the
responses for a number of density graded laminates, and to
obtain the various information on the parameters that
affects the impact phenomena.
2.1 Objectives of the Research
The main focus of this research is to study the response
of density graded E-glass composite laminate when
subjected to low velocity impact using both experimental
and finite element analysis.
The objectives of this research are:
 To determine the effects of low velocity impact on
density graded E-glass composite laminate.
 Linear and Symmetric density grading is tested to
find low velocity impact behavior on their
structures.
 To analyze the deformation, stress and the strain
energy distribution of the laminateswhenstruck by
an indenter at low velocity.
3. EXPERIMENTAL DETAILS
For conducting the low velocity impact test, the drop weight
impact test is used shown in figure 1. The testing is done
under low acceleration falling weight of 6.3kg from a height
of 1m having a velocity of 4.429m/s at the time of impact.
The indenter is cylinder of diameter 10mm and hasa conical
front with a cone angle of 900. This closely simulates a real
world impact conditions and the required data is obtained
from the Data Acquisition System present along with the
experimental setup.
Fig -1: Conical indenter on impact over specimen
In this study, specimens are preparedbyhandlayupprocess.
The various materials used in the experiment and their
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1060
properties are given in table I. E-glass fiber mats of densities
225g/m2, 300g/m2 and 600g/m2 are used. Six different
samples of 50mm X 50mm cross section area of varying
density arrangements were fabricated the arrangements of
the mats are shown in table II
Fig -2: Specimen before and after impact
Table -1: Material Property
Material Density
(Kg/m3)
Young’s
Modulus
(N/m2)
Poisson’s
Ratio
E-glass 2550 76e9 0.21
Polyester 1120 2.1e9 0.37
Structural
Steel
7850 2e11 0.3
Table -2: Arrangement of Fiber Mat
Specimen Stacking Sequence
1 225g/m2 [00
15]
2 300g/m2 [00
15]
3 600g/m2 [00
15]
4 [c00
2/b450
3/a450
2/a450
1]sym
5 [c00
2/b900
3/a900
2/a900
1]sym
6 [c00
2/b450
3/a450
2]2
Where a represents the fiber mat density of 225g/m2,
b represents density 300g/m2, and c represents density
600g/m2 in the above stacking sequence table 2.
3.1 Experimental Results
Table -3: Deformation and Load at Impact
Specimen Total Deformation
(mm)
Peak Load
Measured (N)
1 9 5239
2 9 4953
3 8.2 5821
4 6.4 7354
5 5.1 10532
6 6.1 9841
The load versus deformation curve is obtained in real time
using the Data Acquisition System which is integrated
along with the Drop weight impact tester, thecurveisshown
in figure 3.
Fig -3: Load vs. Deformation of specimen 1
Fig -4: Load vs. Deformation of specimen 2
Fig -5: Load vs. Deformation of specimen 3
Fig -6: Load vs. Deformation of specimen 4
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1061
Fig -7: Load vs. Deformation of specimen 5
Fig -8: Load vs. Deformation of specimen 6
4. FEM DETAILS
In this study test laminate materials are density graded E-
glass fiber reinforced in polyester resin and the projectile
material is structural steel. The test plate is a square
laminate of 50mm X 50mm and 9mm thickness and the
impact indenter is conical. Modeling is done in Catia. The
boundary conditions used for low velocity impact on the
laminate has less effect on the final results, so reduction in
the test laminate size is not affecting the FEM results thus
user can reduce computational time. Finite elementanalysis
is done in Ansys 15 Explicit Dynamics workbench. The
indenter is considered as a rigid body and no deformation is
taken into account, and flexible body consideration is used
for the test laminate. To save computational time the
distance between the indenterandthelaminateisreducedin
the modeling. The specimen is meshed with minimum edge
length of 0.65mm shown in figure 4 and quad element is
chosen for the specimen since it is a flat laminate.
Fig -9: FE Model of the laminate and indenter after mesh
Fig -10: Boundary Condition applied to FE Model
4.1 FEM Results
Fig -11: Deformation of Specimen 1
Fig -12: Deformation of Specimen 2
Fig -13: Deformation of Specimen 3
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1062
Fig -14: Deformation of Specimen 4
Fig -15: Deformation of Specimen 5
Fig -16: Deformation of Specimen 6
4.2 Comparison of Experimental and FEA Results
Chart -1: Comparison of Experimental andFEADeformation
5. CONCLUSIONS
The present study focused on determining the low velocity
impact strength of density graded E-glass fiber reinforced
composite laminates. To find out the optimum density
grading for impact resistance composite laminates of 9mm
thickness were prepared by hand layup process. The
specimens are then subjected to drop weight impact test at
low velocity of 4m/s to 5m/s. It is found thatoptimal density
grading is found for 900 symmetrically graded laminate
which had the least deformation for the maximum load. The
same results are validated through FEM software Ansys in
explicit dynamics work bench. The factors that influencethe
impact performance include material property of the yarn,
indenter geometry,impactvelocityandboundaryconditions.
The individual effects cannot lead to a conclusive result. A
combination of computational modeling and simulation is
required to understand the deformation and low velocity
failure mechanism.
REFERENCES
1. Volnei Tita, Jonas De Carvalho and Dirk Vandepitte.
“Failure analysis of low velocity impact on thin
compoxite laminates: Experimental and Numerical
approaches”. Elsevier 2008, Composite Structure
83, pp. 413-428.
2. Costantino Menna, Domenico Asprone, Giancarlo
Caprino, Valentina Lopresto and Andrea Prota.
“Numerical simulation of impact tests on GFRP
composite laminates”. International Journal of
Impact Engineering 38,2011, pp. 677-685.
3. Balasubramani.V, Rajendra Boopathy and
Vasudevan.R. “ Numerical analysis of low velocity
impact on laminated composite plates”. Elsevier
2013, Procedia Engineering 64, pp. 1089-1098.
4. N.Razali, M.T.H.Sultan, F.Mustapha, N. Yidris and
M.R. Ishak. “Impact damage on composite
structures”. The International Journal of
Engineering and Science, 2014, Vol.3, Issue 7, pp.8-
20.
5. S.N.A.Safri, M.T.H.Sultan, N.Yidris and F.Mustapha.
“Low velocity and high velocity impact test on
composite materials”. The International Journal of
Engineering and Science, 2014, Vol.3, Issue 9, pp.
50-60.
6. Sunith Babu L and H.K. Shivanad. “ Impact analysis
of laminated composite on glass fiber and carbon
fiber”. International Journal of Engineering and
Technology and Advanced Engineerinng, Vol.4,
Issue 6, June 2014, pp. 824-829.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1063
7. Rakesh Reghunath, Mahadevan Lakshman and
K.M.Mini. “Low velocity impact analysis on glass
fiber reinforced composites with varied volume
fractions”. IOP conference series, Materials Science
and Engineering 73, 2015.
8. Baliga and Sarvesh. “LowVelocityimpactanalysisof
composite repair patches of different shapes”.
2015.Dissertions and theses paper 197.
9. Yehia Abdel Nasser, Ahmed M.H Elhewy and Al
Mallah. “Impact analysis of composite laminate
using finite element method”. Taylor and Francis,
Ships and Offshore Structures 2016.

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Impact Analysis and Simulation of Density Graded E-Glass Composite

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1059 Impact Analysis of Density Graded E-Glass Composite Laminate Sedulingam Kandaswamy1, Deepthi K R2 1PG Scholar, 2Assistant Professor 1, 2 Dept. of Mechanical Engineering, New Horizon College of Engineering, Karnataka, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - E-Glass/Polyester composite laminates are subjected to low velocity impact and their behavior is analyzed. To investigate the impact strength, the laminate is fabricated by hand-layup process. E-glass fiber mats of different densities are used in the fabrication. Due to the cost and complexity related to impact experiments itisnotoptimal to base all impact related studies on laboratory tests alone. Therefore, to reduce the experimentationcostfewsamplesare fabricated and tested in laboratory using drop weight impact tester, further numerical simulation of impact on composite laminate is investigated using 3-D dynamic explicit finite element code. ANSYS/AUTODYN whichis generalpurposenon- linear dynamic modeling and simulation software. Trial simulations are conducted and results are validated. Key Words: Impact, E-Glass/Polyester, Density Grading, Deformation, Energy Absorption. 1. INTRODUCTION A composite is a material consisting of two or more distinctive materials which acts as isotropic materials on a macroscopic level but has anisotropic properties at microscopic level. They are designed and fabricated to be superior to those of the constituent materials acting independently. Composite materials have significant design advantages in the aerospace industry. The combined properties such as light weight and high strength are the most attractive feature for the aerospace and aircraft designs. Composite materials are formed when two or more chemically distinct materials are combined in such a way that a distinct interface separates the components (as opposed to alloys). Each of the constituent materials has its own specific physical andchemical properties,thusresulting in composite which has different properties from each material alone. The composite for the impact protection is generally fibrous or continuous fiber reinforced. This type consists of one phase, which is usually much stronger i.e. fiber, than the other phase i.e. matrix. This unique mixture leads to anisotropic properties for the composite which provide the specific characteristic of obtaininghighstrength in one critical direction. 2. PROBLEM DESCRIPTION The density graded E-glass composite laminate was investigated on low velocity impact using experimental setup and finite element analysis software. The finite element software used in this study was AnsysAutodyn.The complicated response of composite laminate along with the high cost of fabrication limits the number of laminates considered for experimentation. In order to overcome this issue, finite element analysis can be used to find out the responses for a number of density graded laminates, and to obtain the various information on the parameters that affects the impact phenomena. 2.1 Objectives of the Research The main focus of this research is to study the response of density graded E-glass composite laminate when subjected to low velocity impact using both experimental and finite element analysis. The objectives of this research are:  To determine the effects of low velocity impact on density graded E-glass composite laminate.  Linear and Symmetric density grading is tested to find low velocity impact behavior on their structures.  To analyze the deformation, stress and the strain energy distribution of the laminateswhenstruck by an indenter at low velocity. 3. EXPERIMENTAL DETAILS For conducting the low velocity impact test, the drop weight impact test is used shown in figure 1. The testing is done under low acceleration falling weight of 6.3kg from a height of 1m having a velocity of 4.429m/s at the time of impact. The indenter is cylinder of diameter 10mm and hasa conical front with a cone angle of 900. This closely simulates a real world impact conditions and the required data is obtained from the Data Acquisition System present along with the experimental setup. Fig -1: Conical indenter on impact over specimen In this study, specimens are preparedbyhandlayupprocess. The various materials used in the experiment and their
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1060 properties are given in table I. E-glass fiber mats of densities 225g/m2, 300g/m2 and 600g/m2 are used. Six different samples of 50mm X 50mm cross section area of varying density arrangements were fabricated the arrangements of the mats are shown in table II Fig -2: Specimen before and after impact Table -1: Material Property Material Density (Kg/m3) Young’s Modulus (N/m2) Poisson’s Ratio E-glass 2550 76e9 0.21 Polyester 1120 2.1e9 0.37 Structural Steel 7850 2e11 0.3 Table -2: Arrangement of Fiber Mat Specimen Stacking Sequence 1 225g/m2 [00 15] 2 300g/m2 [00 15] 3 600g/m2 [00 15] 4 [c00 2/b450 3/a450 2/a450 1]sym 5 [c00 2/b900 3/a900 2/a900 1]sym 6 [c00 2/b450 3/a450 2]2 Where a represents the fiber mat density of 225g/m2, b represents density 300g/m2, and c represents density 600g/m2 in the above stacking sequence table 2. 3.1 Experimental Results Table -3: Deformation and Load at Impact Specimen Total Deformation (mm) Peak Load Measured (N) 1 9 5239 2 9 4953 3 8.2 5821 4 6.4 7354 5 5.1 10532 6 6.1 9841 The load versus deformation curve is obtained in real time using the Data Acquisition System which is integrated along with the Drop weight impact tester, thecurveisshown in figure 3. Fig -3: Load vs. Deformation of specimen 1 Fig -4: Load vs. Deformation of specimen 2 Fig -5: Load vs. Deformation of specimen 3 Fig -6: Load vs. Deformation of specimen 4
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1061 Fig -7: Load vs. Deformation of specimen 5 Fig -8: Load vs. Deformation of specimen 6 4. FEM DETAILS In this study test laminate materials are density graded E- glass fiber reinforced in polyester resin and the projectile material is structural steel. The test plate is a square laminate of 50mm X 50mm and 9mm thickness and the impact indenter is conical. Modeling is done in Catia. The boundary conditions used for low velocity impact on the laminate has less effect on the final results, so reduction in the test laminate size is not affecting the FEM results thus user can reduce computational time. Finite elementanalysis is done in Ansys 15 Explicit Dynamics workbench. The indenter is considered as a rigid body and no deformation is taken into account, and flexible body consideration is used for the test laminate. To save computational time the distance between the indenterandthelaminateisreducedin the modeling. The specimen is meshed with minimum edge length of 0.65mm shown in figure 4 and quad element is chosen for the specimen since it is a flat laminate. Fig -9: FE Model of the laminate and indenter after mesh Fig -10: Boundary Condition applied to FE Model 4.1 FEM Results Fig -11: Deformation of Specimen 1 Fig -12: Deformation of Specimen 2 Fig -13: Deformation of Specimen 3
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1062 Fig -14: Deformation of Specimen 4 Fig -15: Deformation of Specimen 5 Fig -16: Deformation of Specimen 6 4.2 Comparison of Experimental and FEA Results Chart -1: Comparison of Experimental andFEADeformation 5. CONCLUSIONS The present study focused on determining the low velocity impact strength of density graded E-glass fiber reinforced composite laminates. To find out the optimum density grading for impact resistance composite laminates of 9mm thickness were prepared by hand layup process. The specimens are then subjected to drop weight impact test at low velocity of 4m/s to 5m/s. It is found thatoptimal density grading is found for 900 symmetrically graded laminate which had the least deformation for the maximum load. The same results are validated through FEM software Ansys in explicit dynamics work bench. The factors that influencethe impact performance include material property of the yarn, indenter geometry,impactvelocityandboundaryconditions. The individual effects cannot lead to a conclusive result. A combination of computational modeling and simulation is required to understand the deformation and low velocity failure mechanism. REFERENCES 1. Volnei Tita, Jonas De Carvalho and Dirk Vandepitte. “Failure analysis of low velocity impact on thin compoxite laminates: Experimental and Numerical approaches”. Elsevier 2008, Composite Structure 83, pp. 413-428. 2. Costantino Menna, Domenico Asprone, Giancarlo Caprino, Valentina Lopresto and Andrea Prota. “Numerical simulation of impact tests on GFRP composite laminates”. International Journal of Impact Engineering 38,2011, pp. 677-685. 3. Balasubramani.V, Rajendra Boopathy and Vasudevan.R. “ Numerical analysis of low velocity impact on laminated composite plates”. Elsevier 2013, Procedia Engineering 64, pp. 1089-1098. 4. N.Razali, M.T.H.Sultan, F.Mustapha, N. Yidris and M.R. Ishak. “Impact damage on composite structures”. The International Journal of Engineering and Science, 2014, Vol.3, Issue 7, pp.8- 20. 5. S.N.A.Safri, M.T.H.Sultan, N.Yidris and F.Mustapha. “Low velocity and high velocity impact test on composite materials”. The International Journal of Engineering and Science, 2014, Vol.3, Issue 9, pp. 50-60. 6. Sunith Babu L and H.K. Shivanad. “ Impact analysis of laminated composite on glass fiber and carbon fiber”. International Journal of Engineering and Technology and Advanced Engineerinng, Vol.4, Issue 6, June 2014, pp. 824-829.
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 08 | Aug -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 1063 7. Rakesh Reghunath, Mahadevan Lakshman and K.M.Mini. “Low velocity impact analysis on glass fiber reinforced composites with varied volume fractions”. IOP conference series, Materials Science and Engineering 73, 2015. 8. Baliga and Sarvesh. “LowVelocityimpactanalysisof composite repair patches of different shapes”. 2015.Dissertions and theses paper 197. 9. Yehia Abdel Nasser, Ahmed M.H Elhewy and Al Mallah. “Impact analysis of composite laminate using finite element method”. Taylor and Francis, Ships and Offshore Structures 2016.