FINITE ELEMENT AND MBD ANALYSIS OF PISTON TO PREDICT THE ENGINE NOISE

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Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al.s, 2013 Research Paper ISSN 2278 0149 www.ijmerr.com Vol. 2, No. 1, January 2013 2013 IJMERR. All Rights Reserved FINITE ELEMENT AND MBD ANALYSIS OF PISTON TO PREDICT THE ENGINE NOISE S N Kurbet 1, Vinay V Kuppast 1 and Vijaykumar N Chalwa 2 * *Corresponding Author: Vijaykumar N Chalwa, vchalwa14@gmail.com The engine vibration is considered as the major source of engine noise which deteriorates the engine performance and increases the pollution. The noise from the engine comprises of mechanical and combustion noise. Combustion noise is primarily due to rapid pressure fluctuations in the combustion chamber. The mechanical noise is due to mechanical impact forces during both motions of piston viz. primary and secondary motions.in this study the effect of the piston secondary motion is taken for the analysis considering combustion pressure contributing to the dynamics of the piston. The Kirloskar Diesel Engine is considered for the present study. The geometrical modeling of the engine is done using CATIA V-5 modeling tool. The finite element meshing is done using Hypermesh 9.0 meshing tool. This work analysis is carried out in ANSYS 10 commercial finite element analysis software. To understand the complex behavior of the piston in motion relative to the other engine parts, viz., connecting rod, crankshaft, a Multi Body Dynamic (MBD) analysis is carried out. This analysis showed the occurrence of piston tilt near TDC and BDC. The stress and displacement results are viewed and analyzed using Hyperview. The analysis results can effectively be used to optimize piston geometry and hence lateral forces are minimized to obtain minimum tilt of the piston. The minimization of the piston tilt eventually leads to the reduction of engine noise. Keywords: Piston, Vibration, Finite element analysis, piston secondary motion, Hypermesh, Multibody dynamics INTRODUCTION The present work is study the engine parts viz piston considered as the main source or vibration and noise. The emphasis on the engine vibration and noise given rise to wide scope for the methods of predicting and controlling the engine noise and vibration. The noise and vibration in the IC engine is emphasis the combustion and mechanical movement of engine part. The Combustion noise is primarily due to rapid pressure fluctuations in the combustion chamber. The 1 Department of Mechnanical Engineering, Basaveshwar Engineering College Bagalkot 587102, Karnataka, India. 2 SMS Mohite Patil Institute of Technology and Research, Akluj, MH, India. 183

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al., 2013 Mechanical noise is produced by the primary and secondary motion of the engine part. Primary motion of engine part is due to combustion pressure in the combustion chamber which makes piston to move from TDC to BDC but this motion is linear in nature, Secondary motion of engine part is due to impact load of the combustion, and it is transverse motion of engine part while piston moving from TDC to BDC vice versa. The most common two internal combustion engines are petrol and diesel engines. Presently the IC diesel engines are replacing the more expensive petrol engines. The diesel engine are mostly being used as commercial engines due to high break power and high fuel economy, but it produces bad noise. The piston slap which is the result of piston side thrust on the cylinder liner as it moves TDC to BDC (Vinay and Kurbet, 2008). The objectives of the present work is, to develop 3-Dimentional Finite Element (FE) model of piston for the piston motion considering regions; piston, piston before TDC, at TDC and after TDC, and to study stress distribution and deformation of piston in different regions. An overview is given based on a literature survey of general theory for IC engine. The system is modeled using CATIA5 software to create needed geometry and finite element software to implement physics and carry out simulations. The problem is described in a single finite element model. 3-D models of the system are analyzed. The next would be a force analysis of the piston slap followed by the simulation aspects of the Finite element Method. Using commercial software ANSYS 10 and then meshing with software Hypermesh-9. The Objectives of the paper is To develop 3-Dimentional Finite Element Model of piston liner assembly for piston motion considering regions: Piston at TDC. Piston after TDC. Piston before TDC. To study stress distribution and deformation in liner assembly in region of objective 1. To study the mechanical impact loading on the piston for deformation of slap in the region of objective 1. To develop 3-Dimentional Finite Element Multi body dynamics Model of complete IC engine of real Kirlosker engine and applying Real boundary condition and working gas pressure curve of Kirlosker engine taken at 1500 rpm on piston head and observe the output. To study stress distribution and piston-slap of MBD analysis of Kirlosker engine. INTERNAL COMBUSTION ENGINES Engine Parts The essential parts of automobile engine are as follows: cylinder block, cylinder head, crank case, piston, piston rings, piston pin, connecting rod, crank shaft, fly wheel, valves and mechanism. Piston Piston is considered to be one of the most important parts in a reciprocating engine in which it helps to convert the chemical energy obtained by the combustion of fuel into useful mechanical power. The purpose of the piston 184

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al.s, 2013 is to provide a means of conveying the expansion of the gasses to the crankshaft, via the connecting rod, without loss of gas from above or oil from below. Piston is essentially cylindrical plug that moves up and down in the cylinder. It is equipped with piston rings to provide a good seal between the cylindrical wall and piston. Although the piston appears to be a simple part, it actually quite complex from the design point of view. The efficiency and economy of the engine primarily depends on the working of piston. it must operate in the cylinder with minimum of friction and should be able to with stand the high explosive force developed in the cylinder and also the very high temperature ranging from 2000 C to over 2800 C during operation. The piston should be as strong as possible, however its weight should be minimized as for as possible in order to reduce the inertia due to its reciprocating mass (Nagaraj et al., 2005). Functions of Piston To receive the thrust force generated by explosion of the gas in the cylinder and transmits it to the connecting rod. To reciprocate in the cylinder as a gas tight plug causing suction, compression, expansion and exhaust stroke. To form a guide and bearing to the small end of the connecting rod and to take the side thrust due to the obliquity of the rod. The top of the piston is called head ring grooves are located at the top circumference portion of the piston. Portion below the ring grooves is called skirt. The portion of the piston that separates the grooves iscalled the lands. Some pistons have a groove in the top land called a heat dam which reduces heat transferred to the rings. The piston bosses are those reinforced section of the piston designed to hold the piston pin. Piston Materials The material used for pistons is mainly aluminium alloy. Aluminium pistons can be either cast or forged. Cast iron is also used for pistons. In early years cast iron was almost universal material for pistons because it posses excellent wearing qualities, coefficient of expansion and general suitability in manufacture. But due to the reduction of weight in reciprocating parts, the use of aluminium for piston was essential. To obtain equal strength a greater thickness of metal is necessary. But some of the advantage of the light metal is lost. Aluminium is inferior to cast iron in strength and wearing qualities, and its greater coefficient of expansion necessitates greater clearance in the cylinder to avoid the risk of seizure. the heat conductivity of aluminium is about thrice that of cast iron and this combined with the greater thickness necessary for strength, enables and aluminium alloy piston to run at much lower temperature than a cast iron one (200 C to 250 C as compared with 400 C to 450 C) as a result carbonized oil doesn t form on the underside of the piston, and the crank case therefore keeps cleaner. This cool running property of aluminium is now recognized as being quite as valuable as its lightness. Indeed; pistons are sometimes made thicker than necessary for strength in order to give improved cooling. DESCRIPTION OF I.C. ENGINE MODELS FOR FINITE ELEMENT STUDY The Table 1 shows engine details: 185

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al., 2013 Table 1: Description of IC Engine Figure 2: Piston Solid Model S. No. Description Specification 1. Engine Kirlosker Engine 2. Bore 80 mm 3. Stroke 110 mm 4. Engine rpm taken for study 1500 rpm 5. Compression ratio 16.5:1 6. Maximum torque 66 Nm 7. Test condition/type Water cooled direct injection diesel single cylinder engine 8. Max pressure at study rpm 54 bars GEOMETRIC MODELING Important steps in Geometric modeling are: Creating part (solid) modeling of each part; Assembling; Converting solid model into IGES format. Drawing and dimension used in this study were retrieved from kirlosker engine by CMM coordinate measuring machine (Toshiyaki et al., 2007) (Figures 1 and 2). Figure 1: 2D Drawing of Piston Finite Element Modeling Finite element modeling and analysis is one of the most popular mechanical Engg applications offered by existing cad /cam systems. This is attributed to the fact that the FEM is perhaps the most popular numerical technique for solving Engg problems. The method is general enough to handle any complex shape or geometry, any material properties, any boundary conditions, and any loading conditions.the generality of the FEM fits the analysis requirements of the complex Engg systems and designs, where closed form solutions of governing equilibrium equations are usually not available. In addition it is an efficient design tool by which designers can perform parametric design studies by considering various design cases, analyzing them and choosing the optimum design (Kurbet and Krishnakumar, 2004). The finite element model of the piston is developed using ANSYS 11 modeling tool (Figure 4). The meshing the model was done with axisymmetric PLANE 42 elements. The 186

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al.s, 2013 material models is created using the Kirloskar engine data and are shown in the Table 2. S. No. Table 2: Material Properties of the Kirloskar Diesel Engine Part Name Material Name Density In Kg/ m 3 Young s Modulus In GPA In N/mm 2 Poison Ratio 1 Piston Al alloy 2630 72.4 72400 0.31 For defining boundary conditions, the pressure curve of the Kirloskar engine at running speed of 1500 rpm is considered. The variation of the pressure with a different crank angle is shown in the Figure 3. The bottom skirt of the piston is constrained in all degrees of freedom. It is solved for different pressure values corresponding to the crank angle. three dimensional form by using hexahedral elements, Tetrahedral and Pentamesh. All the meshed components are tested for the quality of the mesh. After proving the quality of the mesh, the components are assembled to represent the IC engine system. The quality setting in Hypermesh-9 preprocessor for quality check of the mesh was shown in Figure 5: Each components were meshed independently and were shown in Figures 6 and 7: Figure 4: Model Generated in ANSYS Figure 3: The Variation of the Pressure with Different Crank Angles Figure 5: Meshed Model of Piston GENERATION OF FINITE ELEMENT MESH FOR MBD ANALYSIS The required geometric information for the mesh generation is collected by importing the IGES file of the model in Hypermesh-9. The finite element mesh is generated for each of the assembly components by using standard command in the 187

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al., 2013 Piston Piston is critical to mesh with hexahedral hence it is meshed with tetrahedral mesh. Figure 7: Assembled Meshed Model in Hypermesh with Quality Check Figure 6: Boundary Conditions Applied in ANSYS MULTI BODY DYNAMIC SIMULATION OF PISTON MOTION The MBD analysis is carried out to understand the complex behavior of the engine parts during operating conditions. The pressure curve of the Kirloskar engine as considered for the structural analysis is considered for this analysis. The combustion pressure on the piston causes the piston to reciprocate between TDC and BDC. This in turn carried to the connecting rod and then to the crankshaft. Hence the engine components experience the gas force exerted on the piston. Here it is obvious to study the stress regions and displacements in different engine parts to predict the behavior of the parts. This will reveal the lateral motion of the piston for different crank angle positions and is used to predict the piston slap or tilt (Kurbet and Malagi, 2009). RESULTS AND DISCUSSION The analysis is carried out for different cases considered. The result data have been tabulated to plot the respective graph. The stress and displacement graphs have been considered to study the effect of gas pressure on the piston at different crank angle position. The displacement curves are plotted to study the piston slap (displacement in x- direction). From the finite element analysis, the various stress and displacement values have been found out corresponding to the gas pressure taken from the actual engine readings and are tabulated in the Table 3. The 3600 crank angle corresponds to the TDC of the piston position in the cylinder. From Figure 3, the pressure v/s crank angle graph, it is evident that the maximum pressure of 56 bar is observed near TDC. Hence the structural analysis of the piston is taken from TDC to BDC travel during power stroke, i.e., after combustion of fuel in the chamber. 188

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al.s, 2013 The stress developed in the piston for different crank angle position and the lateral displacements of the piston in x-axis are tabulated in the Table 3 shown in below (Malagi and Kurbet, 2009). Table 3: The Gas Pressure, Von Mises Stress and x-displacement of Piston Crank Angle Gas Pressure in N/mm 2 Von Mises Stress in N/mm 2 x- Displacement in mm 360 3.600 60.835 0.277 396 5.280 89.227 0.406 432 1.560 26.361 1.200 468 0.480 08.109 0.369 504 0.240 04.055 0.185 540 0.180 03.039 0.138 576 0.144 02.431 0.111 612 0.120 02.027 0.923 684 0.180 03.042 0.189 720 0.240 04.055 0.185 the gap between piston and cylinder reduces compared to the other region (Figure 9). This phenomenon causes the piston to tilt about the gudgeon pin axis and causes the piston to slap (Cho et al., 2005). The graph of x-displacement v/s crank angle shown in the Figure 10 which clearly indicates the change in the gap between cylinder and piston travel from TDC to BDC. This behavior of the piston tilt repeats for regular interval of the crank angle between 00 to 7200 of the complete cycle. Figure 9: VonMises Stress From the Figure 8, it was observed that the stress in the piston ismaximum near the 90 N/mm 2 pressure regions and causes the piston to deform more at this region. Hence Figure 8: Variation of Von Mises Stress for Different Crank Angles Figure 10: Variation of Piston-Cylinder Gap for Differentcrank Angles 189

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al., 2013 Figure 11: Displacement Figure 14: Piston Deformation Along X-Axis Figure 12: Deformation Zone in Piston at TDC Figure 15: Piston Deformation Along Y-Axis Figure 13: Distribution of Stresses in Piston-Cylinder Assembly at TDC MBD ANALYSIS The results obtained from the Multibody Dynamic analysis (MBD) are discussed as follows. The stress distribution in the engine components is shown in the Figure 13. It was observed from the MBD analysis that the combined effect of the various forces acting on the engine components viz, connecting rod, crankshaft, piston, is inducing stress in each component. The maximum stress level in the piston is observed as 3.584 10 2 N/mm 2. The maximum displacement observed as 1.710 mm. 190

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al.s, 2013 Figure 16: Von Mises Stress Distribution of MBD Analysis of Engine (Radioss Analysis) Figure 17: Displacement of MBD Analysis of Engine (Radioss Analysis) Table 4 shows the difference between the MBD analysis and structural analysis for stress and displacement. Table 4: Comparision Between MBD ANS Structural Analysis MBD Analysis Structural Analysis Displacement along X-axes 1.741 1.710 in mm Stress in N/mm 2 159 157 CONCLUSION The structural analysis of the piston for the various pressure on the piston for different position of the piston in the cylinder moving between TDC to BDC have been studied and the following conclusions are made. The piston experiences maximum stress in the region where the combustion of the fuel takes place, i.e., at the piston head and skirt. This high stress region in the piston deforms more than the other region of thepiston. The maximum x-displacement of the piston for structural analysis resembles the maximum displacement of the piston in MBD analysis. Hence the piston experiences maximum displacement in this region. The deformation in the piston causes it to displace more in this region and this cycle repeats even for the reduction in combustion pressure. The MBD analysis confirms the relative motion between the parts and reveals that the engine noise is associated with the stress developed in the engine parts. FUTURE SCOPE MBD Analysis is proposed, to incorporate the forces in motion for prediction of piston tilt and optimization of the geometry of the piston to reduce engine noise and vibration (NVH). REFERENCES 1. Cho S H, Ahn S I and Kim Y H (2005), A Simple Model to Estimate the Impact Forces Induced by Piston Slap, Korea Advanced Institute of Science and Tech., Daejon, Korea. 2. Kurbet S N and Krishnakumar R (2004), A Finite Element Study of Piston Tilt 191

Int. J. Mech. Eng. & Rob. Res. 2013 Vijaykumar N Chalwa et al., 2013 Effects on Piston Ring Dynamics in IC Engines, Proc. Instn. Mech. Engrs. (IMECHE), Part K, pp. 107-117. 3. Kurbet S N and Malagi R R (2009), A Comprehensive Model to Study Dynamic Motion of Piston and Friction and Lubrication in IC Engines, Journal of Tribology Trans., ASME Tribo-081024. 4. Malagi R R and Kurbet S N (2009), Stress Analysis of Piston Ring-FE Approach, 2 nd International Conference on Recent Advances in Manufacturing Held at Kovilpetti TN from February 25-27. 5. Nagaraj Nayak, Reddy P V, Yogesh Aghav, Navtej Singh Sohi and Dani A D (2005), Study of Engine Vibration Due to Piston Slap on Single Cylinder, High Powered Engine, SAE Iternational, 2005-26-046. 6. Toshiyaki Kobayashi, Yukitaka Takahashi and David J Bell (2007), How to Predict the Piston Slap-Noise Using 3D Piston Motion Simulation, SAE International, 2007-01-1245. 7. Vinay V Kuppast and S N Kurbet (2008), Review of Finite Element Analysis of the IC Engine Noise and its Experimental Validation, International Conference on Total Engineering Analysis, IISC, Bangalore. 192