Finite Element Analysis of Particulate composite embedded in Fibrous Composite Layer

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International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007 Finite Element Analysis of Particulate composite embedded in Fibrous Composite Layer Nikhil J.Chaudhari 1 A.S.Rao Vinaay Patil 3 1Post Graduate Student, Asst. Professor Department of Mechanical Engineering Veermata Jijabai Technological Institute Mumbai, India 3 Manager, Vaftsy CAE, Pune, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Composite can be defined as a structural material consisting two or more combined constituents that are combined at a macroscopic level and are not soluble in each other. In order to improve the properties of existing composites, a newer trend is towards the development of combination of one or more types of Composites together to form hybrid structure. Generally this combination of fibre composites by inclusion of particulate composite layers applies to advanced composites and refers to use of various combinations of fibers or particulate in matrices. They have unique feature that can be used to meet the diverse and competing design requirements in a more cost effective way than either advanced or conventional composites. This paper devoted to fiber Reinforcement is the requirements of certain application can be achieved not only by sizing the cross sectional areas and thickness of components but by changing the material system design i.e. optimizing the material system itself such as fiber orientation angle. The optimization techniques are being used to assist the designer in finding an optimized solution. Key Words: Composites, Finite Element analysis, ANSYS, Optimization, Fibre orientation. 1. INTRODUCTION By inclusion of particulate composite layers in fibre composite flexibility as compared to other reinforced composites. Normally it contains a high modulus fiber with low modulus Particles. The high-modulus fiber provides the stiffness and load bearing qualities, whereas the low-modulus particles make the composite more damage tolerant and keeps the material cost low. It also helps to reduce weight without sacrificing strength and improves electrical and thermal characteristics of the composite material. The mechanical properties of a hybrid composite can be varied by changing volume ratio and stacking sequence of different plies. De-lamination is major problem which is observed in fibre reinforced composite is reduced by including particulate composite layers because of increasing adhesion forces between consecutive layers of the composite. This paper is explains modeling the composite laminate. And also proposes a methodology to model a composite laminate with a composite material to analyze its stress, Strength and stiffness using ANSYS software. In order to evaluate the effectiveness of composite, stress analysis is performed on composite using ANSYS. In this work effort is made to find out optimum angle of fibre which gives reduced stress levels so that advantage of ultimate weight reduction along with stresses can be obtained.. MATERIALS AND METHOD Composite model is created using ANSYS workbench. Model is consisting of various layers of particulate composite along with the fibrous composite. Cylindrical rods are taken as a fibre and ellipsoidal particulate is taken as particle reinforcement which is embedded in to matrix material. Alternate layers of particulate and fibre layer is stacked one above other. By using add frozen operation in extrude is created which helps to create contact non-linearity between matrix and reinforcement..1 Properties of material Table -1: Properties of Material Material Properties Young's Modulus in X,Y & Z direction (GPa) Poisson s Ratio PRXY Poisson s Ratio PRYZ Poisson s Ratio PRXZ Matrix Material (Epoxy Resin) Reinforcing Fibers (Carbon Fibre) Particulate Material (Glass Fibre) 183 3.3.3 0.3 0.3 0.41 0.3 0.3 0.41 0.3 0.3 0.41 01, IRJET.NET- All Rights Reserved Page 64

International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007. Modeling and material assignment Composite model is created using matrix fibre and particulate. Material mentioned in table 1 is added in engineering data of ANSYS workbench and then its assigned the respective component in the model which is shown in fig given below Fig -: Meshing of Particulate and fibre reinforcement Fig -1: Model of Composite. Meshing of Model Meshing is done for creation of nodes and element. In above model Different types of meshing are used for fibre, particulate and matrix material to form optimum mesh. For particulate ellipsoidal Tetrahedron mesh is used by patch conforming method. Mesh Element size is taken as 10µm.For proper definition of contact between particulate and matrix material sphere of influence is used by taking 30 µm. as radius of the sphere which helps to fine meshing at contact surface. Now Mapped face meshing is done with element size of 3 µm. by defining contact sizing and multizone method for obtaining the proper mesh at contact region between fibre and matrix material. The number of nodes obtained is 36641 and numbers of elements are 1813.Meshed model is shown in Fig. and Fig 3 Fig -3: Meshing of model.3 Boundary conditions In the static analysis, to find out total deformation and equivalent stress (Von-mises) boundry conditions are applied in such a way that one end of the laminate constrained i.e all degrees of freedom is zero and other end of the composite laminate is applied force along Cartesian direction. In this model force of N is applied along X-direction as shown Fig 4 01, IRJET.NET- All Rights Reserved Page 60

International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007 Fig -4: Boundary condition of Composite along X-direction.4 Solution After applying boundary conditions solution is simulated for Deformation and Equivalent (von-mises) of all the components associated with the model. It is done for all layers and its reinforcement element. Various plots of deformation of whole composite and Equivalent (vonmises) for each component in the model is shown below. (d) Fig -: Deformation& Equivalent (Von-mises) stress plots.4.1 Plots for Layer 1 Fig shows deformation and stress plot for complete composite structure. Now stress plots for various elliptical particulate and fibre as per layer of composite as shown in figs given below. (e) Fig -6:(a-e) Equivalent (Von-mises) stress plots for (Particulate) Layer 1 01, IRJET.NET- All Rights Reserved Page 61

International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007.4. Plots for Layer Fig -8 :(a-d) Equivalent (Von-mises) stress plots for (Particulate) Layer 3.4.4 Plots for Layer 4 (d) Fig -7 :(a-c) Equivalent (Von-mises) stress plots for (Particulate) Layer.4.3 Plots for Layer 3 01, IRJET.NET- All Rights Reserved Page 6

International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007 Fig - :(a-c) Equivalent (Von-mises) stress plots for (Particulate) Layer 4.4. Plots for Layer Fig -10 :(a-e) Equivalent (Von-mises) stress plots for (Particulate) Layer. RESULT TABLE Result obtained from above plots shown in Fig 6-10 is collected and shown in table. In table L, F & P are the abbreviations used for layer, fibre and particulate followed by number of layer respectively. (d) Table -: Result Data of analysis along X-direction Deform -ation Eqv. Stress Total Layer-1 Layer- 0.14 P1 1.833 L-F1 18. 0.06 P.88 L-F 17.6.01 L-F3 18.86.141 1.6868 Layer-3 Layer-4 Layer- L3-P1 1.76 L4-F1 131.8 P1 1.74 L3-P 1.6338 L4-F 13.7 P.3 L3-1.406 L4-F3 13.87. L3-1.640 1.707 1.67.6 ANALYSIS OF COMPOSITE ALONG Y & Z DIRECTION Similarly analysis is done for applying boundary conditions along y-direction and z directions. Results are collected as discussed in.4 is tabulated which is given in table & table 3 respectively. Table -3: Result Data of analysis along Y-direction Total Layer-1 Layer- Deforma.07 L- 64.3 0.03368 tion P1 7 F1 1 Eqv..087 L- 143.8 1.06 Stress P F 4.06 8 L- F3 1.0 6.18 1 1.8 Layer-3 Layer-4 Layer- L3-P1 1.08 L4-6.0 1.041 F1 6 P1 6 L3-P 1.748 L4-1.46.8 F P 8 01, IRJET.NET- All Rights Reserved Page 63

International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007 L3-1. L3-1.167 L4- F3 63.36 Table -4: Result Data of analysis along Z-direction Deformatio n Eqv. Stress 1. 1.8 1.314 8 Total Layer-1 Layer- 0.0 6 17.6 L3-P1 L3-P L3- L3- P1 P 1.76.380 7 1.6.734 L-F1 L-F L-F3 6.8 3 118..3 1.8 Layer-3 Layer-4 Layer- 1.6 7.06 L4-F1 0.81 61.61 L4-F 4 1.318.6 L4-F3 3 1.66 P1 P 1.086 8 1.41 1.133 7 1.03 1.637 1.7 OPTIMIZATION FOR FIBRE ORIENTATION By using methodology as discussed in previously equivalent stress is calculated for model and various components of models. From all the values of the equivalent stresses optimum condition is find out. Here is the procedure for fibre orientation in single layer for finding out optimum condition. i. Tabulate all the results and find minimum value for each case. ii. Divide stress of all components by minimum value of stress as obtained in step i iii. Tabulate all ratios obtained by dividing the stresses iv. Summation is done for all the ratio of the stress v. Find out minimum value from that summation vi. Corresponding parameter along which minimum stress ratio is considered as optimum parameter. vii. Repeat this procedure for all conditions Step i) All result for equivalent stress are tabulated for angle varies from 30-60. For better strength of the composite distortion should be minimum. Stress is nothing but amount of distortion takes place in element. While doing the so for optimization of minimum value of stress is considered. One factor is obtained by the taking ratio of stress obtained to the minimum stress in that layer & which is mainly effect for Optimization for layers for fibre orientation. Table -: Result Table for (Fibrous) Layer with various angles ANGLE in Degree Layer 30 4 60 Minimum Value L-F1 11.08 1.7 18. 18. L-F 1.1 63.43 17.6 1.1 L-F3 1.08 6.6 18.86 18.86 Step ii-iii) Ratio of the stress of all component to minimum stress is calculated & its mentioned in the table given below. Table -6: Ratio of stress in fibres (Fibrous) Layer with various angles Angle(Degrees) 30 4 60 L-F1 1.173 1.6746 1 L-F 1 1.301 1.011 L-F3 1.01 3.41 1 Summation 3.3844 6.6 3.01 Step iii-iv) From above table it is concluded that minimum summation is obtained are 3.01 and corresponding orientation with respect to that value is 60 degree is considered as optimum condition. 3. CONCLUSIONS By this paper its conclude the analysis of composite laminate for finding out optimum angular orientation of fibre in particulate included composites.with the help of this paper we can analysis any composite material for in ANSYS it is proved that for particulate inclusion in fibrous composite optimum orientation of fibre angle is taken as 60 degree. Even it is observed that optimum condition remains the same for model with shuffling layers of particulate embedded fibrous composites. Fibre orientation is taken as 60 degree as at this angle minimum stress and maximum strength is obtained 01, IRJET.NET- All Rights Reserved Page 64

International Research Journal of Engineering and Technology (IRJET) e-issn: 3-006 Volume: 0 Issue: 04 July-01 www.irjet.net p-issn: 3-007 REFERENCES [1] Reference Book -Jones RM. Mechanics of composite materials. New York: Mc- Graw-Hill; 17. [] Mittelstedt C. Becker W. Inter-laminar stress concentrations in layered structures: Part I-A selective literature survey on the free edge effect since 167. J Compos Mater 004:38(1): 107-6 [3] E. J. Barbero. ''Finite Element Analysis of Composite Materials'' 011. [4] WEN-PIN LIN, HSUAN-TEH HU, Parametric Study on the Failure of Fiber Reinforced Composite Laminates under Biaxial Tensile Load, Journal of composite materials, Vol. 36, No. 1/00, pp 1481-103. [] Nirmal Saha, Amar Nath Banerjee,; Flexural behavior of unidirectional polyethylene-carbon fibers-pmma hybrid composite laminates, J. App. Poly. Sci. vol.60, 16, pp. 13-14. 01, IRJET.NET- All Rights Reserved Page 6