Design and Analysis of Crankshaft Using Topology Optimization in ANSYS

Design and Analysis of Crankshaft Using Topology Optimization in ANSYS: A Study on Internal Combustion Engine

by Mukund Hingne*, Dr. Rashmi Dwivedi,

- Published in Journal of Advances and Scholarly Researches in Allied Education, E-ISSN: 2230-7540

Volume 15, Issue No. 11, Nov 2018, Pages 103 - 113 (11)

Published by: Ignited Minds Journals


ABSTRACT

The crankshaft is an important component of an engine. Crankshaft is one of the critical components for the effective and precise working of the internal combustion engine. A crankshaft can be called as the heart of any I.C. engine since it is the first recipient of the power generated by the engine. Its main function is to convert the oscillating motion of the connecting rod into rotary motion of the flywheel. The main function of a camshaft is to convert rotary motion of the crankshaft into vertically reciprocating motion of the valves required to open and close the intake and exhaust valves of engine cylinders, with the assistance of cams located on it and an intermediate mechanism. This paper presents the design connecting rod of internal combustion engine using the topology optimization. This paper 1 basic model and 3 implement model is proposed. The crankshaft model 3D geometry is created by using CATIA V5 and then it is import in ANSYS 19.0. and check all the result in three different load case 22624N, 32624N and 42624N.

KEYWORD

crankshaft, topology optimization, ANSYS, engine, internal combustion engine, connecting rod, camshaft, flywheel, oscillating motion, rotary motion

1. INTRODUCTION

The crankshaft is a moving part of the internal combustion engine (ICE). It‘s main function is to transform the linear motion of the piston into rotational motion. The pistons are connected to the crankshaft through the connecting rods. The crankshaft is mounted within the engine block. The crankshaft is fitted into the engine block through its main journals. The connecting rods are fixed on the conrod journals of the crankshaft. On opposite sides of the conrod journals the crankshaft has counterweights which compensates outer moments, minimizes internal moments and thus reduces vibration amplitudes and bearing stresses (Reddy, et. al., 2017). In the present work, one crank throw model was used to calculate the static strength of crankshaft. Software based analysis techniques use multi-body simulation tools for accurately predicting the operating loads acting on the engine components. The 3D model of crankshaft system, obtained from CATIA V5 software is analyzed in Ansys Software to assess the motion and loads acting on the crankshaft.

Fig.1 Crankshaft (Patil, et. al., 2017)

For the design optimization process of crankshaft further topology optimization technique of Ansys is used to remove the unnecessary material from the crank shaft.

2. TOPOLOGY OPTIMIZATION IN ANSYS

Unless it has been topologically optimized, every part in an assembly probably weighs more than it needs to. Extra weight means excess materials are being used, loads on moving parts are higher than necessary, energy efficiency is being compromised and shipping the part costs more. Now, with Topology Optimization technology, ANSYS Mechanical gives you the tools you need to design

minimum material thicknesses are set and exclusion areas are defined (Pandiyan, et. al., 2016). Topology optimization in ANSYS Mechanical allows you to: • Take into account multiple static loads combined with optimizing for natural frequencies (modal analysis) • Satisfy requirements for minimum material thickness • Observe rules around feature direction (for machining operations for example) • Have scope for both cyclic and planar symmetry • Easily validate results

Fig.2 Topology Optimization

3. METHODOLOGY

3.1 Modelling

In this modelling section 1 basic model and 3 implement model is proposed. The crankshaft model 3D geometry is created by using CATIA V5 and then it is import in ANSYS 19.0. and check all the result in three different load case 22624N, 32624N and 42624N.

Fig.3 Different Crankshaft Model

mechanical property are used in ANSYS are shown in table below:

Table 1. Material Property

Material Forget steel Density (Kg/m3) 7833 Young‘s Modulus (MPa) 2.21E+05 Poisson‘s Ratio 0.3

3.3 Meshing

After applying meshing 26641 nodes and 19234 elements is generated in crankshaft.

Fig.4 meshing of crankshaft

3.4 Boundary condition

The FE model created was subjected to static structural analysis after assigning suitable material properties and boundary conditions. The force acting on the crankpin for case-1 due to gas loads at 4500 rpm. The maximum force acting on the crankpin is 22624 N.

Fig.5 Applying force

The force acting on the crankpin for case-2 due to gas loads at 4500 rpm. The maximum force acting on the crankpin is 32624 N.

Fig.6 Applying force

The force acting on the crankpin for case-3 due to gas loads at 4500 rpm. The maximum force acting on the crankpin is 42624 N.

Fig.7 Applying force

3.5 Fixed support

The crankshaft is fixed in both the end of shaft.

Fig.8 Fixed support of crankshaft

4. RESULT ANALYSIS

Case-1 (Model -1) In this case the maximum force acting on the crankpin is 22624 N.

Deformation

In this case 0.011156mm deformation is found.

Fig.9 Total deformation in Case-1

Fig.9 represents the model 1of total deformation in case 1 when the maximum force acting on the crankpin is 22624 N. in this model min. deformation is 0 and max. deformation is 0.011198.

Case-1 (Model-1) Equivalent Stress

In this case 68.42 Mpa maximum stresses is found.

Fig.10 Equivalent stress in Case-1

Fig.10 elaborates the mode 1 of equivalent stress in case 1 when the maximum force acting on the crankpin is 22624 N. In this model min. stress is 0.0018211 and max. stress is 68.42. The ANSYS 19.0 provide the feature of topology optimization. After applying 22624N force the new model is proposed. The red region show that this material is does not affect the all over stress value. So all the new design is made only change in red region.

Fig.11 Topology optimization in ANSYS Case-1 (Model-2) Deformation

In this case 0.011182mm deformation is found.

Fig.12 Total deformation in Case-1

Fig.12 shows the model 2 of total deformation in case 1 when the maximum force acting on the

Case-1 (Model-2) Equivalent Stress

In this case 68.70 Mpa maximum stresses are found.

Fig.13 Equivalent stress in Case-1

Fig.13 represents the model 2 of equivalent stress in case1 when the maximum force acting on the crankpin is 22624 N. in this model min. stress is 0.0015045 and max. stress is 68.703.

Case-1 (Model-3) Deformation

In this case 0.011202mm deformation is found.

Fig.14 Total deformation in Case-1

Fig.14 shows the model 2 of total deformation in case 1 when the maximum force acting on the crankpin is 22624 N. In this model min. deformation is 0 and max. deformation is 0.011202. Case-1 (Model-3)

Equivalent Stress

In this case 63.49 Mpa maximum stress is found.

Fig,15 Equivalent stress in Case-1

Fig.15 represents the model 3 of equivalent stress in case 1 when the maximum force acting on the crankpin is 22624 N. In this model min. stress is 0.0068849 and max. stress is 63.492.

Case-1 (Model-4) Deformation

In this case 0.011207mm deformation is found.

Fig.16 Total deformation in Case-1

Fig.16 shows the model 4 of total deformation in case 1 when the maximum force acting on the crankpin is 22624 N. In this model min. deformation is 0 and max. deformation is 0.011207.

Case-1 (Model-4) Equivalent Stress

In this case 4 74.156 Mpa maximum stress is found.

Fig.17 Equivalent stress in Case-1

Fig.17 shows the model 4 of equivalent stress in case 1 when the maximum force acting on the crankpin is 22624 N. In this model min. stress is 0.0083383 and max. stress is 74.156. Case-2 (Model-1) In this case the maximum force acting on the crankpin is 32624 N.

Deformation

In this case 0.016144mm deformation is found.

Fig, 18 Total deformation in Case-2

Fig.18 shows the model 1 of total deformation in case 2 when the maximum force acting on the crankpin is 32624 N. in this model min. deformation is 0 anjd max. deformation is 0.016144.

Case-2 (Model-1) Equivalent Stress

In this case 98.68 Mpa maximum stress is found.

Fig.19 Equivalent stress in Case-2

Fig.19 shows the model 1 of equivalent stress in case 2 when the maximum force acting on the crankpin is 32624 N. in this model min. stress is 0.0026254 and max. stress is 98.638.

Case-2 (Model-2) Deformation

In this case 0.016136mm deformation is found.

Fig.20 Total deformation in Case-2

Fig.20 represents the model 2 of total deformation in case 2 when the maximum force acting on the crankpin is 32624 N. In this model min. deformation is 0 and max. deformation is 0.016136.

Case-2 (Model-2) Equivalent Stress

In this case 108.57 Mpa maximum stress is found.

Fig.21 Equivalent stress in Case-2

0.0021071 and max. stress is 106.57.

Case-2 (Model-3) Deformation

In this case 0.016149mm deformation is found.

Fig.22 Total deformation in Case-2

Fig.22 shows the model 3 of total deformation in case 2 when the maximum force acting on the crankpin is 32624 N. In this model the min. deformation is 0 and max. deformation is 0.016149.

Case-2 (Model-3) Equivalent Stress

In this case 91.533 Mpa maximum stress is found.

Fig.23 Equivalent stress in Case-2

Fig.23 shows the model 3 of equivalent stress in case 2 when the maximum force acting on the crankpin is 32624 N. in this model min. stress is 0.012809 and max. stress is 91.533.

Case-2 (Model-4) Deformation

In this case 0.057078mm deformation is found.

Fig.24 Total deformation in Case-2

Fig.24 shows the model 4 of total deformation in case 2 when the maximum force acting on the crankpin is 32624 N. In this model min. deformation is 0 and max. deformation is 0.057078.

Case-2 (Model-4) Equivalent Stress

In this case 176.84 Mpa maximum stress is found.

Fig.25 Equivalent stress in Case-2

Fig.25 shows the model 4 of equivalent stress in case 2 when the maximum force acting on the crankpin is 32624 N. In this model min. stress is 0.022639 and max. stress is 176.84. Case-3 (Model-1) In this case the maximum force acting on the crankpin is 42624 N.

Deformation

In this case 0.02109mm deformation is found.

Fig.26 Total deformation in Case-3

Fig.26 elaborates the model 1 of total deformation in case 3 when the maximum force acting on the crankpin is 42624 N. In this model min. deformation is 0 and max. deformation is 0.02109.

Case-3 (Model-1) Equivalent Stress

In this case 128.86 Mpa maximum stress is found.

Fig.27 Equivalent stress in Case-3

Fig.27 shows the model 1 of Equivalent stress in Case-3 when the maximum force acting on the crankpin is 42624 N. In this model min. stress is 0.0034299 and max. stress is 128.86.

Case-3 (Model-2) Deformation

In this case 0.021079mm deformation is found.

Fig.28 Total deformation in Case-3

Fig.28 show the model 2 of total deformation in case 3 when the maximum force acting on the crankpin is 42624 N. In this model min. deformation is 0 and max. deformation is 0.021079.

Case-3 (Model-2) Equivalent Stress

In this case 148.83 Mpa maximum stress is found.

Fig.29 Equivalent stress in Case-3

Fig.29 model 2 of equivalent stress in case 3 when the maximum force acting on the crankpin is 42624 N. In this model min. stress is 0.0027527 and max. stress is 141.83.

Case-3 (Model-3) Deformation

In this case 0.021096mm deformation is found.

Fig.30 Total deformation in Case-3

Fig.30 shows the model 3 of total deformation in case 3 when the maximum force acting on the crankpin is 42624 N. In this model min. deformation is 0 and max. deformation is 0.021096.

Case-3 (Model-3) Equivalent Stress

In this case 119.57 Mpa maximum stress is found.

Fig.31 Equivalent stress in Case-3

Fig.31 shows the model 3 of equivalent stress in case 3 when the maximum force acting on the crankpin is 42624 N. In this model min. stress is 0.016733 and max. stress is 119.57.

Case-3 (Model-4) Deformation

In this case 0.074564mm deformation is found.

Fig.32 Total deformation in Case-3

Fig.32 shows the model 4 of total deformation in case 3 when the maximum force acting on the crankpin is 42624 N. in this model min. deformation is 0 and max. deformation is 0.074564. Case-3 (Model-4)

Equivalent Stress

In this case 231.01 Mpa maximum stress is found.

Fig.33 Equivalent stress in Case-3

Fig.33 shows the model 4 of equivalent stress in case 3 when the maximum force acting on the crankpin is 42624 N. In this model min. stress is 0.029575 and max. stress is 231.01.

Deformation comparison

After performing analysis in ansys following deformation are found as shown in table.

Graph 1 Deformation Comparison Graph

Graph 1 shows the comparison of deformation. In this deformation analysis there are three cases used for every four model. In this graph shows the model 4 deformation is high in case 2 and case 3. In case 1 the deformation of all model is close to each other.

Stresses comparison

After performing analysis in ansys following Stresses are found as shown in table.

Table 3 Stresses comparison in all cases

Graph 2 Stress Comparison graph

Graph 2 represents the comparison graph of stress. In this stress analysis research three case used for every four model. In every case model 4 stress is very high and model 3 stress is low.

Weight comparison

After performing analysis in ansys following Weight are found as shown in table.

Table 4 Weight comparison in all 3 cases

Graph 3 Weight Comparison Graph

is lower.

5. CONCLUSION

Based on these analysis results, concepts have been developed which reduce the weight of the crankshaft to a possible extent, without affecting the performance of the engine. The 3D model of crankshaft system, obtained from CATIA V5 software is analyzed in ANSYS to assess the motion and loads acting on the crankshaft. Topology optimization is help to optimize the performance of any machine. The crankshaft model 3D geometry is created by using CATIA V5 and then it is import in ANSYS 19.0. and check all the result in three different load case 22624N, 32624N and 42624N.

REFERENCES

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Corresponding Author Dr. Rashmi Dwivedi*

Associate Professor, Department of Mechanical Engineering, Sagar Institute of Science and Technology Bhopal