• No results found

STATIC AND VIBRATION ANALYSIS OF COMPOSITE BEAMS USING FINITE ELEMENT METHODS

N/A
N/A
Protected

Academic year: 2022

Share "STATIC AND VIBRATION ANALYSIS OF COMPOSITE BEAMS USING FINITE ELEMENT METHODS"

Copied!
7
0
0

Loading.... (view fulltext now)

Full text

(1)

STATIC AND VIBRATION ANALYSIS OF COMPOSITE BEAMS USING FINITE ELEMENT

METHODS

G. Kalyan Chakravarthi

1

, G. Venkatasubbaiah

2

1

Pursuing M.Tech Machine Design (Mechanical),

2

Asst. Professor of Mechanical Department

Vignana Bharathi Institute of Technology, Pallavolu (V),Chapadu(M),Proddatur(T), Kadapa (D), (India)

ABSTRACT

Beams are structural members which are widely used and its dynamic characteristics under loading has great importance. Thus, the purpose of this paper is to carry out an efficient and accurate simulation for static and modal analysis of uniform beam using Ansys 14.5. Displacement and frequencies of cantilever beam are studied with distributed as well as surface load. Composite materials have interesting properties such as high strength to weight ratio, ease of fabrication, good electrical and thermal properties compared to metals. A composite material consists of layers of a composite mixture consisting of matrix. In this project a cantilever composite beam with both upper and lower surfaces symmetrically bonded by piezoelectric ceramic and the beam is made up of t300/976 graphite/epoxy composites. Design engineer must consider several alternatives such as best stacking sequence, optimum fiber angles in each layer as well as number of layers itself based on criteria such as achieving highest natural frequency loads of such structure. Analysis of such composite materials starts with estimation of resultant material properties. The created configuration interface rearranges the outline procedure to some degree. The dynamic examination as far as central normal recurrence and basic static burden is delineated by utilizing these general material constants as a later piece of investigation.

I. INTRODUCTION

A combination of two or more materials with different properties, or a system composed of two or more physically distinct phases separated by a distinct interface whose combination produces aggregate properties that are superior in many ways, to its individual constituents. A material with combination of two or more material can provide enhanced properties that produce a synergistic effect.

In composite materials there are two constituents one is grid and other is fortification. The constituents which is continuous and present in greater quantity is called matrix. The main functions of the matrix is to holds or bind the fibre together, distribute the load evenly between fibres, protect the fibre joint from mechanical and environmental damage and also carry shear. While the other is reinforced; its primary objective is to enhance the mechanical properties e.g. solidness, strength and so on. The mechanical property depends upon the shape and dimensions of reinforcement. On the premise of sort framework material, composites can be grouped into three

(2)

main categories, polymer, metallic and ceramic

II. OBJECTIVES

The project aims at detail FEM examination of shaft. The accompanying are the primary destinations of the venture.

1. Building a 3-D Solid parametric model of cantilever beam in CATIA V5.

2. Meshing the model by ANSYS MESHER in ANSYS 14.5.

3. Rigid body modes and Normal modes- we have calculated in free vibration analysis for cantilever composite beam.

4. Experimental modal analysis carried out using FFT ANALYSER MACHINE to validate our CAE work.

5. Behaviour of torsional modes, twisting modes and joined methods of vibration we have concentrated on for all frameworks.

6. ansys 14.5 is used to find out the deformation and stress-strain from given boundary condition.

7. Analysis is done for both ordinary cantilever beam and coated cantilever beam Dynamic response and investigation of critical stresses are found out by incorporating the boundary conditions at the journal bearing positions and tangential and radial forces on corresponding nodes.

For this ANSYS MESHER used for meshing and ANSYS used as solver.

Beams have always been used extensively in building materials and structures. Depending on the application and working environment they are frequently under dynamic loading condition. Hence, from the standpoint of proper functioning and safety, study of response of these structural elements under dynamic loading is of utmost importance.

Dynamic analysis of a structure or structural element consists of two different aspects, namely, free and forced vibration studies. The main purpose of a free vibration analysis is to predict the natural frequencies of various vibration modes of the component under no load and loaded conditions. The natural frequencies of the structure under some form of static loading are generally known as loaded natural frequencies. Determination of these frequencies is important to avoid resonance condition, where the external excitation frequency coincides with the system natural frequencies. At resonance condition, the element vibrates with large amplitude resulting in deterioration of structural health. This deterioration usually causes local increase in flexibility, which is a serious threat to life and performance of structural component.

These analyses are made in the static analysis module under ANSYS solution task. The stiffness matrix of the system is obtained with the static analysis by using the finite component strategy. Relocation values for each hub are computed by utilizing the comparison beneath under particular stacking. The overall equilibrium equations for linear structural static analysis are:

KuF Where; K= Total stiffness matrix u= Nodal displacement vector F= Total applied load vector Modal Analysis:

Natural frequencies of the system and mode shapes have to be calculated for the full solution method and mode superposition method which will be used in dynamic analysis step. Reaction of the framework for the outer constraining is dictated by compelling recurrence shapes.

(3)

ANSYS software is used for creating the model and performing the analysis of this study. APDL stands for ANSYS Parametric Design Language, a scripting that one can use to automate the common tasks or even building the model in term of parameters. In this paper, a double-acting hydraulic cylinder is used in the analysis. The model shown in Figure 4.1 is created as finite elements. In this fem, with eight nodes and three degrees of freedom in each node and layered 191 is chosen from ANSYS element library. All the dimensions of the cylinder are parametric and the dimensions used in the analysis are shown in Figure shown below

Figure 4.1 The Finite Element Model

In the analysis, two different boundary conditions are considered for bar with coating and with out. It is assumed that, the surface force is directly applied to the surface or to the body in two different coundation types and the static and dynamic analyses is made for these two mounting types. The degree of freedom boundary conditions is shown in Figure 4.2 and 2.3 working surface force of bar is taken as 10000N.

Figure 4.2 Boundary Condition a) with Coating-Type 1

Cantilever , modelled as FEM, is made of t300/976 graphite/epoxy composites

l. The properties of steel is given as

Modulus of Elasticity, E 150 GPa

Poisson Ratio, n 0.3

Density, 1600 Kg / m3

Cantilever beam coating, modeled as FEM, is made of piezoelectric ceramic properties. The properties of steel are given as.

(4)

Modulus of

Elasticity, Poisson Shear

E (GPa) Ratio, n ModuluGPa Density

E1=63 0.3 24.2 1.5(10)6

E2=63 0.3 24.2

E3=63 0.3 24.2

III. RESULTS AND DISCUSSIONS

Figure 4.4 Static Displacement Distributions of Cantilever Beam,

Figure 4.5 Static Stress Distributions of Cantilever Beam,

Figure 4.5 Static Stress Distributions of Cantilever Beam,

(5)

Figure 4.6 Von Mises Stress

Figure 4.7 Static Strain Energy

Figure 4.8 Modal Deformation

WITH COATING

WITH OUT COATING TOTAL

DEFORMATION,(M)

0.16989 0.66672

EQUIVALENT ELASTIC STRAIN,(M/M)

0.055383 0.14821

EQUIVALENT STRESS,(PA)

8.2026e9 2.2138e10

STRAIN ENERGY,(J) 82.62 J 48.663

Table 4.1Comparision of Deflection of Cylinder for Different Materials and Boundary

Conditions

(6)

mode With out coating

deformation With coating

deformation

Mode 1

174.85 Max :

4.5706

Freq : 152.67

Max : 1.4822

Min : 0 Min : 0

Mode 2

687.63 Max : 4.549 Freq : 383.35

Max : 1.4732

Min : 0 Min : 0

Mode 3

1090 Max : 4.5683

Freq:

942.58

Max : 1.476

Min : 0 Min : 0

Mode 4

2290.4 Max : 5.6795

Freq : 1685.1

Max : 1.6938

Min : 0 Min : 0

Table 4.3 Natural Frequencies of Cylinder, Bc-1type of carbon/Epoxy

Figure 4.Modal Deformation IV. CONCLUSIONS

Composite design is designed using CATIA V5 R20 and analysis is done in ANSYS 16 in structural and modal workbench. We first designed a rectangle bar in CATIA with required dimensions and then it is imported in ANSYS 16 work bench for further structural and modal workbench...later on the same process is repeated with coating. After thorough analysis we conclude that by applying piezoelectric ceramic coating there is change in deformation, von misses stress and strain. We even observed very low damping frequency in modal workbench with very low deformation.

We conclude that by applying piezo electric ceramic coating to cantilever composite beam there is a lot of difference in deformation and stress factor , so it is suggestible.

REFERENCE

[1]. Eddy, Matthew Daniel (2008). The Language of Mineralogy: John Walker, Chemistry and the Edinburgh Medical School 1750-1800. Ashgate.

[2]. "For Authors: Nature Materials"

[3]. Callister, Jr., Rethwisch. "Materials Science and Engineering – An Introduction" (8th ed.). John Wiley and Sons, 2009 p.5-6

(7)

[4]. Callister, Jr., Rethwisch. Materials Science and Engineering – An Introduction (8th ed.). John Wiley and Sons, 2009 p.10-12

[5]. Cristina Buzea, Ivan Pacheco, and Kevin Robbie (2007). "Nanomaterials and Nanoparticles: Sources and Toxicity".Biointerphases 2 (4): MR17–MR71. doi:10.1116/1.2815690. PMID 20419892.

[6]. A. Navrotsky (1998). "Energetics and Crystal Chemical Systematics among Ilmenite, Lithium Niobate, and Perovskite Structures". Chem. Mater. 10 (10): 2787. doi:10.1021/cm9801901.

[7]. Shelby, R. A.; Smith D.R.; Shultz S.; Nemat-Nasser S.C. (2001). "Microwave transmission through a two-dimensional, isotropic, left-handed metamaterial". Applied Physics Letters 78 (4):

489.Bibcode:2001ApPhL..78..489S. doi:10.1063/1.1343489.[dead link]

[8]. Smith, D. R.; Padilla, WJ; Vier, DC; Nemat-Nasser, SC; Schultz, S (2000). "Composite Medium with Simultaneously Negative Permeability and Permittivity". Physical Review Letters 84 (18): 4184–

7.Bibcode:2000PhRvL..84.4184S. doi:10.1103/PhysRevLett.84.4184. PMID 10990641.

[9]. "Sto AG, Cabot Create Aerogel Insulation". Construction Digital. 15 November 2011. Retrieved 18 November 2011.

[10]. "Is graphene a miracle material?". BBC Click. 21 May 2011. Retrieved 18 November 2011.

AUTHOR DETAILS

G KALYAN CHAKRAVARTHI pursuing M-Tech in Vignana Bharathi Institute Of Technology, Pallavolu (village), Chapadu (mandal), Proddatur (taluqa), Kadapa (dist)

G.VENKATASUBBAIAH working as Associate Professor in Mechanical Engineering in Vignana Bharathi Institute of Technology, Proddatur, Kadapa dist, A. P., India , He is having more than Seven years of teaching experience.

References

Related documents

In figure 6.1, which shows a square cantilever beam (same conditions as shown above) mesh with linear quadrilateral elements.

In this work it has been concluded that, firstly, solid model created using CATIA and analyzed using finite element model of engine block with different modified fin are

[4] Analytical solution for the dynamic analysis of a delaminated composite beam traversed by a moving constant force by Mohammad H Kargarnovin, Mohammad T

This penetration is small enough and this reaction force plot will be used as the target plot and finally the solution of simplified model with beam between

Fig 7 Dynamic displacements of the mid – point of the clamped – pinned beam versus the position of the Moving load on the beam for various α values.. Fig8 Matlab results for pinned

Ships use propeller as propulsion device for converting shaft power of the engine to thrust force for the ship to move it through water. Presently conventional marine propellers

A reinforced concrete beam model was calibrated to experimental data, and predictions of initial cracking, yielding of the steel and flexural failure of the beam were compared to

The modelling, simulation and analysis of cantilever beam is done by using ANSYS & MATLAB and theoretically by finite element method (FEM) for the evaluation of natural