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Design, Analysis and Comparative Study of Exhaust Manifold for a Multi-Cylinder Four Stroke SI Engine using CFD
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Design, Analysis and Comparative Study of Exhaust Manifold for a Multi-Cylinder Four Stroke SI Engine using CFD
1.
© 2023, IRJET
| Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1845 Design, Analysis and Comparative Study of Exhaust Manifold for a Multi-Cylinder Four Stroke SI Engine using CFD Vivek Chaudhary1, Dr G. Amba Prasad Rao2 1Post Graduate Student, Dept. of Mechanical Engineering, NIT Warangal 2Professor, Dept. of Mechanical Engineering, NIT Warangal, Telangana, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Gas exchange phenomena of an IC Engine take place through intake and exhaust manifolds. The engine’s performance is influenced by the gas exchange process. The engine's performance improves when the exhaust manifold is in good condition. In the present work, an attempt is made to the modify exhaust manifold by upgrading its design for improved performance for a chosen multi-cylinder engine configuration. The primary objective of the present work is to enhance the design to reduce backpressure in the exhaust manifold for enhanced engine performance. Computational fluid dynamics (CFD) is a popular and current operating software that is widely used. CFD is largely used in the automobile industry to lower the cost of designing and analyzing various models in the fluid flow area. The flow through the exhaust manifold is performed using commercially available software. Efforts are made through CFD software to analyze various shapes of exhaust manifolds. Five distinct models were built and thoroughly analyzed using velocity and pressure contours to get the optimum shape for minimal backpressure and high exhaust velocity. The velocity contour and pressure contour are used to comparesix distinct models, and the best potential modelforlowbackpressureand high exhaust velocity is given. Among the six models designed, model 6 yielded satisfactory performance. Key Words: Multi-Cylinder Engine, Exhaust Manifold, Back Pressure, Exhaust Velocity, Exhaust Temperature. 1.INTRODUCTION One of the most significant components of an ICengineis the exhaust manifold. Exhaust manifold design is a challenging technique because it is dependent on manyparameterssuch as exhaust velocity, backpressure,mechanical efficiency,and so on. The importance of any of these criteria is determined by the designer's requirements. Backpressure, exit exhaust velocity, and power required are some of the exhaust manifold design considerations. The exhaust manifold is constructed of cast iron or stainless steel. It collects gases from several cylinders and routes them to the exhaust manifold. Many studies andresearchhavebeenconductedin this topic. The study's goal is to gain a thorough understanding of the manifold operation, flow property distribution, and heat transfer details.Duetotheinclusionof so many components, it is impossible to replicate the actual scenario in a model. The output gases from more than two cylinders are collected into a single pipe in an exhaust manifold of any multicylinder engine. The outlet of the multicylinder heads is connected to the inlet of the multicylinder exhaustmanifold.Inmulticylinderengines, the exhaust manifold is attached to the engine and is the principal portion where the stream from multiple cylinders is to be collected into a single pipe. The accumulated hot exhaust gases exit throughthesingle exhaustmanifoldoutlet from the cylinder header. For the engine to work optimally, the backpressure of the exhaust manifold at the output should be reduced. For domestic automobiles,thehigherthe backpressure, the poorer the performance or economy. Higher backpressure is requiredforracecarstoreachhigher speeds in less time. To achieve optimal mechanical and thermal efficiency, the exhaust gases should have a high velocity at the exhaust manifold's exit. Table -1: Engine Specifications Engine 4 Stroke 4 Cylinder SI Engine Make Maruti-Suzuki Wagon-R Calorific Value of Fuel (Gasoline) 45208 KJ/KG-K Specific Gravity of Fuel 0.7 Bore and Stroke 69.05 mm x 73.40 mm Swept Volume 1100 cc Compression Ratio 7.2:1 Dynamometer Constant 2000 Diameter of Orifice 29 mm Coefficient of Discharge of Orifice 0.65 International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072
2.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1846 Backpressure is a typical issue connected with the exhaust manifold. According to the literature research, much work has been done to improve the exhaust manifold in order to improve the engine's performance. The CFD approach saves manufacturing costs and production time. According to a survey of the literature, many exhaust manifoldstudieshave been conducted utilizing the CFD technique. The following are some excerpts from the literature review. Dr. M. Senthil Kumar, Dr. S. Sendilvelan, PL.S. Muthaiah [1] have examined the exhaust manifold in order to reduce backpressure in the exhaust manifold and improve exhaust gas filtration. Modification of the geometry of exhaust manifold was done by shifting the size of the conical region of the exhaust manifold as well as the grid sizeofthemeshed wire packed through the exhaust manifold. When the grid size is increased, the filtration level lowers; when the filtration level decreases, the exhaust system emits more exhaust. When the grid size decreases, backpressure is formed in the exhaust manifold, causing engine efficiency to decline. CFD is used to evaluate the exhaust manifold and select the best-design model with the least amount of backpressure and the most amount of PM filtration. Siddaveer Sangamad, Vivekanand Navadagi [2] used CFD to study the flow through two distinct versions of an exhaust manifold. They analyzed two models: one with the base geometry of the exhaust manifold and one with themodified geometry of the exhaust manifold. Both models were analyzed utilizing pressure and velocitycontours.Themajor goal of this work is to enhance the exit velocity when the exhaust manifold has a low back pressure, which boosts volumetric efficiency and engine efficiency. They concluded that the present model is modified by modifying its geometry while maintaining the sameboundaryconstraints. The new model's results outperform the current model because they analyzed velocityandpressurecontourstofind the lowest back pressure while boosting the volumetric efficiency of the engine. KS Umesh, VK Pravin, K Rajagopal [3] performed both the CFD study and experimental verification of the influence of exhaust manifoldgeometry. Theydesignedandanalyzed two different models, an existing model and a modified model. They changed the geometry of the existing model of an exhaust manifold, which was then analyzed using parameters such as velocitycontoursand pressurecontours, and both models were constructed and tested. In CFD analysis, the redesigned model yielded the best results,with little backpressure in the exhaust manifold and increased volumetric efficiency of the engine. The same results were achieved afterconductingtheexperimentswith bothmodels. It is easy to deduce that the experimental results match the CFD analytical results. Experimental analysis validated the CFD analysis results. Mohdsajid Ahmed, Kailash BA, Gowreesh SS [4] constructed five alternative exhaust manifold models and analyzed in this paper. The primary task is to enhance the design of an exhaust manifold since minimizing backpressure in the exhaust manifold improves engine efficiency and performance. They analyzed the simple flow of an exhaust using velocity and pressure contours for five distinct developed models, compared the five modelsusingpressure and velocity contours, and then chose the best one model. They found that model number five is the best model because it has the lowest backpressure and smooth flow of an exhaust without recirculation. It also has the lowest turbulent kinetic energy and the highest output velocity when compared to other models. Using this exhaust manifold, higher exhaust velocity and lower back pressure can be achieved. 2. METHODOLOGY 2.1 CAD Modelling of Exhaust Manifold Thecomputeraideddrawingsoftwarenameddesignmodeler is used to create the five models. A commercial CFD tool is used to analyze six different models. Meshing software is used to name boundaries and discretize the models. Dimensions in mm are provided for the basic CAD models that were used. Fig -1: CAD dimensions of exhaust manifold 2.2 Exhaust Manifold Designs using CAD Software Model 1 In the model 1 shape of the inlet has been modified from straight inlet to convergent inlet and 3D model and its 2- D sketch is shown.
3.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1847 Fig -2: CAD and sketch for Model 1 Model 2 In model 2 outlet of exhaust manifold is modified from converging outlet to divergent-straight-convergent outlet. Fig -3: CAD and sketch for Model 2 Model 3 In model 3 the divergence length of the outlet is increased and convergence length is decreased. Fig -4: CAD and sketch for Model 3 Model 4 In model 4 the divergence length of the outlet is decreased and the convergence length is increased. Inlet 1 Inlet 2 Inlet 3 Inlet 4 Outlet
4.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1848 Fig -5: CAD and sketch for Model 4 Model 5 In model 5 the divergent area and convergent area of theoutlet are kept equal and straight area is decreased. Fig -6: CAD and sketch for Model 5 Model 6 In model 6 the the elliptical cross-sectionhasbeenused with sharp expansion and convergence shape towards outlet. Fig -7: CAD and sketch for Model 6 2.3 Boundary Conditions Table -2: Boundary Conditions Named Selection Boundary Type Boundary Condition Inlet Patch Mass flow rate inlet Outlet Patch Pressure outlet Walls Wall No Slip and Convection The fluid considered is air and defaultmaterialpropertiesfor air have been imported from Fluent library. The flow was assumed to be steady state, turbulent along with heat transfer phenomenon. The boundary conditionsusedatinlet and outlet boundaries are mass flow rate inlet and pressure outlet boundary conditions. Air temperature at inlet is used as 313 oC. No slip boundary condition was used on the walls along with convection value of 10W/m2Kforheatdissipation through walls to atmosphere. Inlet 1= 0.00188kg/s,Inlet2=0.00188kg/s,Inlet3=0.00188 kg/s, Inlet 4 = 0.00188 kg/s, Outlet= 0Pa. 2.4 Meshing Details Fig -8: Mesh for Model 1 Total number of nodes - 23052 Total number of nodes - 113977 Maximum Skewness - 0.67 Average Skewness - 0.222
5.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1849 Fig -9: Mesh for Model 2 Total number of nodes - 29329 Total number of nodes - 148220 Maximum Skewness - 0.698 Average Skewness - 0.221 Fig -10: Mesh for Model 3 Total number of nodes - 27608 Total number of nodes - 138885 Maximum Skewness - 0.697 Average Skewness - 0.222 Fig -11: Mesh for Model 4 Total number of nodes - 29650 Total number of nodes - 150082 Maximum Skewness - 0.698 Average Skewness - 0.219 Fig -12: Mesh for Model 5 Total number of nodes - 30317 Total number of nodes - 153864 Maximum Skewness - 0.7 Average Skewness - 0.22
6.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1850 Fig -13: Mesh for Model 6 Total number of nodes - 30751 Total number of nodes - 156290 Maximum Skewness - 0.669 Average Skewness - 0.221 3. RESULTS AND DISCUSSION 3.1 Model 1 Results Fig -14: Pressure Contour Fig. 14 gives the variation of pressure in the exhaust manifold for model 1. It is seen that pressure at outlet is 0Pa as specified in the boundary condition. However, backpressure is generated and can be seen increasing gradually from outlet towards inlet. Fig -15: Temperature Contour Fig. 15 gives the variation of temperature in the exhaust manifold for model 1. It can be seen that hot air is coming though all 4 inlets at same temperature and as the air passes through the manifold it loses heat to the environment due to convection boundary condition through walls. Relatively cooler temperature regions are formed at the side extended region of exhaust manifold as hot air tries to flow out through the outlet directly without flowing to the side extended regions. Fig -16: Velocity Streamlines From the fig. 16 it is evident that due to the convergent shape of the inlet, velocities are found to be lower at the connecting area and inlet. The low velocity results in high
7.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1851 backpressure. It is observed that exhaust velocities considerably decrease by designing the manifold using the convergent inlet. It is observed that air circulates in the side extended regions of the exhaust manifold. 3.2 Model 2 Results Fig -17: Pressure Contour Figure 17 gives the pressure distributionoverentiredomain for model 2. Pressure is higher at the outlet in comparison with model 1. It is evident that the pressure is high at the inlets of model 2. Pressure is high at the middle of the exhaust manifold in comparison with the exit of the outlet. Fig -18: Temperature Contour Fig. 18 gives the variation of temperature in the exhaust manifold for model 2. Same cold region phenomenon like model 1 on the extended side region is observedformodel 2. It can also be seen that cold temperature spot is getting formed on the divergent portion of the exhaust outlet. This occurs due to sudden expansion of air flow cross section. Fig -19: Velocity Streamlines Figure 19 shows velocity distribution inside exhaust manifold. It is observed that the velocity at the inlets is less and it increases at the outlet. It is seen that the velocities are found to be slightly higher at the outlet in comparisons with model 1. It is observed that the exhaust velocities are considerably increasing by designing the exhaust manifold using this outlet in comparison with model 1. 3.3 Model 3 Results Fig -20: Pressure Contour
8.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1852 Figure 20 gives the pressure distribution for model 3. It is found that the pressure is higher at the inlets. Pressure is higher at the inlet in comparison with the model 1 and almost same in comparison to model 2. It is observed that exhaust pressure is almost same by designing the manifold by decreasing the convergent length of the outlet even further compared to model 2. Fig -21: Temperature Contour Fig. 21 gives the variation of temperature in the exhaust manifold for model 3. Cold region phenomenon like model 1 and 2 is observed on the extended side region of exhaust manifold. It can also be seen that cold temperature spot is getting formed on the divergentportionofthe exhaustoutlet like model 2. This again occurs due to sudden expansion of air flow cross section area. Fig -22: Velocity Streamlines Figure 22 gives the velocity contour of the model 3. It is seen that the velocity is higher at the outlet in comparison with the model 1 and 2. It is observed that exhaust velocities considerably increase by designing the manifold using the divergent-convergent outlet. It is observed that the velocity is higher at the outlet. 3.4 Model 4 Results Fig -23: Pressure Contour Figure 23 gives the pressure distribution for model 4. It is found that the pressure is lower in comparison with the model 2 and 3 but slightly higher than model 1. Higher pressures are observed at the inlets. It is observed that by reducing the divergent length of the outlet the pressure decreases compared to model 2 and 3. Fig -24: Temperature Contour
9.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1853 Fig. 24 gives the variation of temperature in the exhaust manifold for model 4. Cold region phenomenonlikemodel 1, 2 and 3 is observed on the extended side region of exhaust manifold. It can also be seen that cold temperature spot is getting formed on the divergentportionofthe exhaustoutlet like model 2 and 3. This phenomenon occurs due to sudden expansion of air flow cross section area. Fig -25: Velocity Streamlines Figure 25 gives the velocity contour of model 4. It is observed that due to the sudden expansion of the area of outlet velocities are found to slightly increase compared to model 1 at the outlet. It is observed that the exhaust velocities are slightly increasing by designing the exhaust manifold by reducing the divergent length of the outlet in comparison with model 1. Velocities are found to be higher at the outlet due to convergent cross sectionarea nearoutlet of the exhaust manifold. 3.5 Model 5 Results Fig -26: Pressure Contour Figure 26 gives the pressure distribution for model 5. It is found that the pressure is higher in comparison with the model 1 but it is lower compared to model 2 and 3. Back pressure is slightly higher than model 4. Higher pressure is observed at the inlets. It is observed that by reducing the straight length of the outlet the pressure increases considerably. Fig -27: Temperature Contour Fig. 27 gives the variation of temperature in the exhaust manifold for model 5. Cold region phenomenon is again occurring like model 1, 2, 3 and 4 and is observed on the extended side region of exhaust manifold. It can also beseen that cold temperature spot is getting formed on the divergent portion and straight portion of the exhaust outlet like model 2, 3 and 4. This phenomenon occurs due to sudden expansion of air flow cross section area after the connecting region. Fig -28: Velocity Streamlines
10.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1854 Figure 28 gives the velocity distribution in model 5. It is observed that due to the divergent convergent shape of the outlet, velocity is almost similar at the outlet in comparison with model 1. It is observed that the exhaust velocities remain almost same by designing the exhaust manifold by reducing the straight length of the outlet in comparisonwith model 1. The velocity streamlines of the model 5 show that the flow is uniform in comparison with the other models. Very less recirculation is observed in themodel comparedto all other models. 3.6 Model 6 Results Fig -29: Pressure Contour Figure 29 gives the pressure distribution for model 6. It is found that the back pressure is higher in comparison with the model 1, 2, 3, 4 and 5. Higher pressure is observed at the inlet region. It is observed that by increasing the straight length of the outlet the pressure increases considerably. Fig -30: Temperature Contour Fig. 30 gives the variation of temperature in the exhaust manifold for model 6. Cold region phenomenon is again occurring like model 1, 2, 3, 4, 5 and is observed on the extended side region of exhaust manifold. It can also beseen that cold temperature spot is getting formed on the divergent portion and straight portion of the exhaust outlet. This cold region is bigger and forming over entire circumference of the outlet near the connecting region. This phenomenon occurs due to sharp expansionofairflowcross section area after the connecting region. Fig -31: Velocity Streamlines Figure 31 gives the velocity distribution in model 6. It is observed that due to the sharp divergent convergent shape of the outlet, velocity is lower at the outlet in comparison
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 05 | May 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 1855 with model 1, 2, 3, 4 and 5. It is observed that the exhaust velocity decreases by designing the exhaust manifold by increasing the straight length of the outlet in comparison with model 5. The velocity streamlines of the model 5 show that the flow is recirculating in the side extended regions as well as the sharp divergent outlet region. Comparison of all the results from model 1, 2, 3, 4, 5 and 6 have been listed down in the table below. Table -3: Results comparison for all models Design Pressure (Pa) Outlet Temperature (oC) Outlet Velocity (m/s) 1 1.7805 219.63492 1.3709575 2 2.3489877 210.6744 1.3822167 3 2.3197141 212.04085 1.3769754 4 2.073618 212.85724 1.3769688 5 2.0756424 210.60634 1.3799083 6 2.7409584 206.5805 1.174578 4. CONCLUSIONS Different exhaust manifolds are analyzed in this work using commercial CAE software, and the flow of exhaust isseen,as well as the velocity, pressure and temperature distribution throughout the length of the exhaust manifold isdetermined through simulation.CFDPostprocessingwasusedtoanalyze the outcomes of six different models. The usage of various shapes of exhaust manifolds aids in the easy flow of exhaust as well as reduction in exhaust outlet temperature. Model 6 facilitates low velocity flow of exhaust and high backpressure at the exhaust outlet but the outlet temperature is lowest in comparison with all other models. Velocity at the outlet of model 6 is lesscomparedtoall other models and hence the backpressure increases considerably. The optimum design for an exhaust manifold to achieve lowest outlet temperature is Model 6 with 2.74 Pa back pressure, outlet velocity 1.17m/s and outlet temperature of 206.58oC. Temperature reduction of 5.94% at outlet is observed with this design in comparison to model 1. Larger backpressure and lower exhaust velocities are achieved by using exhaust manifolds with sharp convergent divergentshape andlongerstraightlength but it also reduces the outlet temperature. The next best design would be model 5 with slightly higher back pressure and slightly higher velocity compared to model 1 along with outlet temperature value of 210.6oC. Temperature reduction of 4.11% at outlet is observed with this design in comparison to model 1. ACKNOWLEDGEMENT The authors are grateful to the authorities of NIT Warangal for providing all facilities. REFERENCES [1] PL.S. Muthaiah, Dr. M. Senthil kumar, Dr. S. Sendilvelan, “CFD analysis ofcatalyticconvertertoreduceparticulate matter and achieve limited back pressure in Diesel engine”, volume:10 Issue:5 Oct-2010. [2] Vivekanand Navadagi, Siddaveer Sangamad. “CFD analysis of exhaust manifold of multi-cylinder petrol engine for optimal geometry to reduce back pressure”, volume: 3 Issue :3 March-2014. [3] KS Umesh, VK Pravin, K Rajagopal, “CFD analysis of exhaust manifold of multi-cylinder SI engine to determine optimal geometry for reducing emission”, volume:3 Issue:4 Oct- 2013. [4] Mohd Sajid Ahmed, Kailash B A, Gowreesh, “Design and analysis of a multi-cylinderfourstrokeSIengine exhaust manifold usingCFDtechnique”,volume:02Issue:09Dec- 2015. [5] P. Seenikannan, V. M. Periasamy and P. Nagaraj, “ A design strategy for volumetric efficiency improvement in a multi-cylinder stationary diesel engine its validity under transient operation”,volume:5 issue:3, 2008. [6] Kim et al, “A non-noble metal based catalytic converter for two strokes, two-wheeler applications”, SAE Paper No. 2001011303, 2001. [7] C. Lahousse, B. Kern, H. Hadrane and L. Faillon Multi- cylinder SI Engine” International Journal of Engineering & Science Research IJESR/July 2013/ Vol-3/Issue- 7/342-353. [8] Binachiet al, “Possibilities of the application of catalyst technologies for the control of particulate emission for diesel vehicles”, SAE Transaction 2001, paper no. 2001280044.
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