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IRJET- Modelling and Vibration Analysis of Lamina Composite
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IRJET- Modelling and Vibration Analysis of Lamina Composite
1.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 302 Modelling and Vibration Analysis of Lamina Composite 1Department of Mechanical Engineering, G. B. Pant University of Agriculture and Technology, Pantnagar, India ------------------------------------------------------------------------***------------------------------------------------------------------------- Abstract - A composite material is a material made from two or more constituent materials with significantly different physical or chemical properties that, when combined, produce a material with characteristics different from the individual components. Composites are one of the most widely used materials because of their adaptability to different situations and the relative ease of combination with other materials to serve specific purposes and exhibit desirableproperties. Inthis paper, we have done static load analysis on Pre- impregnated Unidirectional EpoxyCarbon and UnidirectionalEpoxy E-Glass in different fiber orientations (from 0° to 90°) in steps of 15°. Also, we have done modal analysis on Pre- impregnated Unidirectional Epoxy Carbon in different fiber orientations. Since the compositesanalyzedhaveorthotropicproperties, the relationship between the fiber orientationandXandYstresses is shown by a graph. Key Words: Laminate Composites; Static Analysis;Vibration Analysis 1. INTRODUCTION A composite material is madebycombiningtwoor more materials – often ones that have very different properties. The two materials work together to give the composite unique properties. However, within the composite you can easily tell the different materials apart as they do not dissolve or blend into each other. Composites,alsoknown as Fiber-Reinforced Polymer (FRP) composites, aremadefrom a polymer matrix that is reinforced withanengineered, man- made or natural fiber (like glass, carbon or aramid) or other reinforcing material. The matrix protects the fibers from environmental and external damage and transfers the load between the fibers. The fibers, in turn, provide strength and stiffness to reinforce the matrix—and help it resist cracks and fractures. Although thefirstcarbon fiber waspatentedin 1961, it took several more years for carbon fiber composites to become commercially available. The use of carbon fiber helped advance many applicationsina numberofindustries, including aerospace, automotive, marine and consumer goods. In 1966, Stephanie Kwolek, a DuPont chemist, invented Kevlar, a para-aramid fiber thatisstrongenough to be used in advanced composites; Kevlar is bestknownfor its use in ballistic and stab-resistant body armour. New and improved resins helped grow the demand for composites, particularly for use in higher temperature ranges and corrosive applications. 1.1 Composite Materials Composites are composed of fiber reinforcements and a resin matrix that bonds the fibers. They can also include core materials, fillers, additives and surface finishes to provide unique performance attributes. Resins- The primary functions of the resin are totransfer stress between the reinforcing fibers, act as a glue to holdthe fibers together, and protect the fibers from mechanical and environmental damage. There aretwomajorgroupsofresins that make up what we call polymer materials—thermosets and thermoplastics.Theseresinsaremadeofpolymers(large molecules made up of long chains of smaller molecules or monomers). Thermoset resins are used to make most composites. They’re converted from a liquid to a solid through a process called polymerization, or cross-linking. When used to produce finished goods, thermosetting resins are “cured” by the use of a catalyst, heat or a combination of the two. Once cured, solid thermoset resins cannot be converted back to their original liquid form. Common thermosets are polyester, vinyl ester, epoxy, and polyurethane. Thermoplastic resins, on the other hand, are not cross-linked and, so, can be melted, formed, re-melted and re-formed. Thermoplastic resins are characterized by materials such as ABS, polyethylene, polystyrene, and polycarbonate. Reinforcements- The mechanical properties of FRP composites are dependent on the type, amount, and orientation of fiber that is selected for a particular service. Fiber reinforcements carry load along the length of the fiber to provide strength and stiffness in one direction. Many materials are capable of reinforcing polymers. Some materials, such as the cellulose in wood, are naturally occurring products. Most commercial reinforcements, however, are man-made. There are many commercially available reinforcement forms to meet the design requirements of the user. The ability to tailor the fiber architecture allows for optimized performance of a product that translates to weight and cost savings. Although many forms of fiber are used as reinforcement in composite laminates, glass fibers account for more than 90 percent of the fibers used in reinforced plastics because they are inexpensive to produce and have relatively good strength-to weight characteristics. Additive and Fillers- Additivesareusedincompositesto modify materials’ properties and tailor the laminate’s performance. When added to the resin, fillers can improve properties including water resistance, weathering, surface smoothness, stiffness, dimensionalstabilityandtemperature resistance. Prakhar Tonk, Naman Jain1, Vinay Kumar Singh1
2.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 303 Core- Core materials are used extensivelythroughoutthe composites industry to fabricate stiff and yet lightweight composites products. Corematerialis“sandwiched”between fiber reinforced laminate skins to significantly increase stiffnessand flexural strength while reducing warpageofflat surfaces. 2. MATERIAL AND METHOD For Analysis Purposes, we used Mechanical APDL. For analysis of composites, we used Shell type 4 node 181 elements. Two Material Models were made and material propertiesforPre-impregnatedUnidirectionalEpoxyCarbon and UnidirectionalEpoxyE-Glasswereadded.Theproperties for the two materials are as shown in Table 1 and Table 2: Table1: Material Properties of Pre- impregnated Unidirectional Epoxy Carbon S. No. Property Value 1 Density (kg/m3) 1490 2 Young’s Modulus X direction (GPa) 121 3 Young’s Modulus Y direction (GPa) 8.6 4 Young’s Modulus Z direction (GPa) 8.6 5 Poisson’s Ratio XY 0.27 6 Poisson’s Ratio YZ 0.4 7 Poisson’s Ratio ZX 0.27 8 Shear Modulus XY (GPa) 4.7 9 Shear Modulus YZ (GPa) 3.1 10 Shear Modulus ZX (GPa) 4.7 Table2: Material Properties of Unidirectional Epoxy E- Glass S. No. Property Value 1 Density (kg/m3) 2000 2 Young’s Modulus X direction (GPa) 45 3 Young’s Modulus Y direction (GPa) 10 4 Young’s Modulus Z direction (GPa) 10 5 Poisson’s Ratio XY 0.3 6 Poisson’s Ratio YZ 0.4 7 Poisson’s Ratio ZX 0.3 8 Shear Modulus XY (GPa) 5 9 Shear Modulus YZ (GPa) 3.846 10 Shear Modulus ZX (GPa) 5 New Lay-up is been created for modeling of composites as a rectangular area of dimensions 80mm × 20mm on the XY plane. For analysis purposes, we will be using a single layer of 1 mm thickness and orientation is been varies from 0° to 90° in steps of 15°. For meshing smart size at 3 and Quadrilateral elements is been used. Fixed support on one end and 100 N force in the X direction on one node at the other end are applied for static analysis. For vibration analysis changed the analysis type to modal. Going to analysis options, we chose to extract 10 modes and the frequency range was set from 0 to 10Hz. 3. RESULTS AND DISCUSSIONS 3.1 Static Load Analysis For Static Load Analysis we used two materials, Pre- impregnated Unidirectional Epoxy Carbon and Unidirectional Epoxy E-Glass. Using each material, we changed the fiber orientation with respect to the applied load direction from 0° to 90° in steps of 15°. Table 3: The tabulated results Pre-impregnated Unidirectional Epoxy Carbon Angle Stress in X- direction (MPa) Stress in Y- direction (MPa) 0 35886.6 31677.3 15 36234.2 27475.2 30 37206 21772.1 45 38955.7 16755.8 60 41726.3 11818.9 75 45176.2 7476.53 90 47151.1 5564.73 Figure 1: graph for stress vs fiber orientation Pre- impregnated Unidirectional Epoxy Carbon Pre-impregnated Unidirectional Epoxy Carbon The results obtained for the X-direction and Y-direction stresses are presented in Table 3 and Figure 1. We can see from the following graph that as the fiber orientation changes from 0° to 90°, the maximum induced stresses in X-
3.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 304 direction increases and maximum stresses in Y-direction decreases. Table 4: The tabulated results Unidirectional Epoxy E- Glass Unidirectional Epoxy E-Glass The results obtained for the X-direction and Y-direction stresses are presented in Table 4 and Figure 2. We can see from the following graph that as the fiber orientation changes from 0° to 90°, the maximum induced stresses in X- direction increases and maximum stresses in Y-direction decreases. The increase and decrease is less pronounced in UD E-Glass Epoxy as compared to UD Carbon Epoxy. As UD Carbon Epoxy is more anisotropic than UD E-Glass Epoxy and thus, change in fiber orientation causes more change in the induced stresses. Figure 1: graph for stress vs fiber orientation Unidirectional Epoxy E-Glass 3.2 Vibration Analysis In present investigation vibration analysis of Pre- impregnated UD Epoxy Carbon as shown in figure 3, 4 & 5 has been performed to investigate the behaviour of composite under free vibration. Angle Stress in X-direction Stress in Y-direction 0 37459.2 24651.1 15 37584.7 23175.7 30 38093.4 20201.9 45 39259.4 16840.7 60 41180.9 13310.2 75 43358.9 10298.2 90 44424.8 9047.44
4.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 305 Figure 3: 1st mode analysis of Pre-impregnated UD Epoxy Carbon for different fiber orientations
5.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 306 Figure 4:2ndmode analysis of Pre-impregnated UD Epoxy Carbon for different fiber orientations
6.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 307 Figure 5: 3rd mode analysis of Pre-impregnated UD Epoxy Carbon for different fiber orientations Table 5: 1st, 2nd and 3rd mode analysis for different fiber orientations Angle Frequency (Hz ×10-03) 1st Mode 2nd Mode 3rd Mode 0 0.0606 0.381 1.068 15 0.0615 0.386 1.082 30 0.0663 0.414 1.163 45 0.079 0.49 1.38 60 0.107 0.642 1.804 75 0.166 0.781 2.316 90 0.228 1.428 4.007 CONCLUSION In present investigation modeling of Pre-impregnated Unidirectional Epoxy Carbon and Unidirectional Epoxy E- Glass composites have been done. Static loading analysis of both the model has been done and result shows that with increase in fiber orientation stress in x-direction increases whereas in y-direction decreases. Vibration analysis of Pre- impregnated Unidirectional Epoxy Carbon has been performed and result shows that with increase in angle of orientation 1st, 2nd and 3rd mode frequency increases. REFERENCES [1] S.W. Tsai, G.S. Springer, “The determination of moduli of anisotropic plates”, ASME Trans., J. App. Mech., 30 (1963) 467–8. [2] T.H.G. Megson, “Aircraft structures for engineering students”, New York, Crane Rusak Co., 1972. [3] D. Young, “Vibration of rectangular plates by the Ritz method”, ASME Trans., J. App. Mech., 17 (1950) 448– 53. [4] M.E. Waddoups, J.R. Eisenmann, B.E. Kaminski, "Macroscopic Fracture Mechanics of Advanced
7.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 308 Composite Materials", DOI:https://doi.org/10.1177/002199837100500402 [5] Isoldi L.A. , Awruch A.M. , Morsh I.B. , Teixeira P.R.F. , “Linear Static And Dynamic AnalysisOfThinLaminated Composite Structures With A Triangular Finite Element”, Vetor, Rio Grande, v.20, n.2, p.38-57, 2010 [6] T. lchThinh, L.K. Ngoc, “Static And Dynamic Analysis Of Laminated Composite Plates With Integrated Piezoelectrics”, Vietnam Journal of Mechanics, VAST, Vol. 30, No. l (2008), pp. 55 – 66. [7] L. Muhammed, A. Ismaeel, “Optimization and Static Stress Analysis of Hybrid Fiber Reinforced Composite Leaf Spring”, DOI:http://dx.doi.org/10.1155/2015/374609 [8] N Jain, R Saxena, “Effect of self-weight on topological optimization of static loading structures” 2017 Alexandria Engineering Journal, doi.org/10.1016/j.aej.2017.01.006 [9] N. Jain, “Topological optimization of the fork-end of a knuckle joint” 2018 Journal of theMechanical Behavior of Materials, doi.org/10.1515/jmbm-2018-0022 [10] N. Jain, “MATLAB Code for Structural Analysis of 2-D Structures Subjected to Static and Self-Weight Loading Conditions” 2017, Vol. 4 Issue 1 Pg, 316-323. [11] G.D. Dean, P. Turner, “The elastic properties of carbon fibers and their composites”, Composites, 4 (1973) 174–80. [12] G.B. Warburton, “The vibration of rectangular plates”, Proc. Instn. Mech. Engrs., 168 (1954) 371–84. [13] N. Jain, V.K. Singh, S. Chauhan, “Dynamic and creep analysis of polyvinyl alcohol based films blended with starch and protein”, Journal of Polymer Engineering, 2018, https://doi.org/10.1515/polyeng-2018-0032 [14] N. Jain, V.K. Singh, S. Chauhan, “Review on effect of chemical, thermal, additive treatment on mechanical properties of basalt fiber and theircomposites” Journal of Mechanical Behaviour of material, 2017, 26, 205– 211 [15] R.R. Pinninti, P. Ramalakshmi, K.N. Kumar, “Static Analysis of Plate Made of Carbon/Epoxy Composite Material by Using ANSYS”, DOI: 10.15680/IJIRSET.2015.0410053 [16] N. Jain, V.K. Singh, S. Chauhan, “A review onmechanical and water absorption properties of polyvinyl alcohol based composites/films”, Journal of Mechanical Behaviour of material, 2017, 26, 213–222 [17] K. Deepmala, N. Jain, V.K. Singh, S. Chauhan, “Fabrication and characterization of chitosan coated human hair reinforced phytagel modified soy protein- based green composite” Journal of Mechanical Behaviour of material, 2018, DOI: 10.1515/jmbm- 2018-0007 BIOGRAPHIES Prakhar Tonk Pursuing Bachelor of Technology In Mechanical Engineering from G.B. Pant University of Agriculture and Technology, Pantnagar, India. His areas of interest are finite element analysis, thermal conduction, composites and automobiles. Naman Jain Naman Jain obtained his Master’s degree in Design and Production Engg. From G. B. P. U. A & T. He is currently pursuing Ph.D. in Mechanical Engineering from G. B. P. U. A & T. His areas of interest are finite element analysis, computer aided mechanical design, optimization and Numerical Modeling and Simulation. o
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