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[object Object],[object Object],OBJECTIVES: After studying Chapter 23, the reader should be able to: Continued
[object Object],[object Object],OBJECTIVES: After studying Chapter 23, the reader should be able to:
[object Object],[object Object],KEY TERMS:
AIRFLOW REQUIREMENTS ,[object Object],Continued The mixture is compressed before ignition to increase force of the burning, expanding gases. The greater the compression, the greater the power resulting from combustion.  All gasoline automobile engines share certain air–fuel requirements. A four-stroke engine can take in only so much air, and the fuel it consumes depends on how much air it takes in Engineers calculate engine airflow requirements using three factors: ,[object Object],[object Object],[object Object]
[object Object],Continued
Figure 23–2  A turbocharger on a Toyota engine. ,[object Object],Many vehicles are equipped with a supercharger or a turbocharger to increase power. Figure 23–1 A supercharger on a Ford V-8. Continued
[object Object]
SUPERCHARGING PRINCIPLES Figure 23–3 The more air and fuel that can be packed in a cylinder, the greater the density of the air–fuel charge. The force an air–fuel charge produces when ignited is largely a function of the charge density. Density is the mass of a substance in a given amount of space.  The greater the density of an air–fuel charge forced into a cylinder, the greater the force and engine power it produces when ignited. An engine using atmospheric pressure for intake is called  naturally  ( normally )  aspirated . A better way to increase air density in the cylinder is to use a pump. Continued
[object Object],Continued
[object Object],Continued
[object Object],Continued ,[object Object],[object Object],[object Object]
Figure 23–4 Atmospheric pressure decreases with increases in altitude. ,[object Object],Atmospheric pressure drops as altitude increases, but boost pressure remains the same. If a supercharger develops 12 psi (83 kPa) boost at sea level, it will develop the same amount at a 5,000-foot altitude because boost pressure is measured inside the intake manifold.  Continued
[object Object],See this table on Page 196 of your textbook.
SUPERCHARGERS ,[object Object],Continued There are two general types of superchargers:
[object Object],Figure 23–5 A roots-type supercharger uses two lobes to force the air around the outside of the housing and forces it into the intake manifold. Continued The  roots - type supercharger  is a  positive displacement  design. All air entering is forced through the unit.  Examples include the GMC 6-71 (used originally on GMC diesel engines that had six cylinders each with 71 cu. in.) and Eaton used on supercharged 3800 V-6 GM engines.
[object Object],Continued
[object Object],Figure 23–6 The bypass actuator opens the bypass valve to control boost pressure. Continued
[object Object],[object Object],[object Object],[object Object],Supercharger Service  Usually lubricated with synthetic engine oil inside the unit, the supercharger oil level should be checked and replaced as specified by the vehicle or supercharger manufacturer. The drive belt should also be inspected and replaced as necessary.
TURBOCHARGERS ,[object Object],Continued By connecting a centrifugal supercharger to a turbine drive wheel and installing it in the exhaust path, the lost engine horsepower is regained to perform other work and the combustion heat energy lost in the engine exhaust (as much as 40% to 50%) can be harnessed to do useful work. This is the concept of a  turbocharger .  The turbocharger’s main advantage over a mechanically driven supercharger is the turbocharger does not drain engine power.
Figure 23–7 A turbocharger uses some of the heat energy that would normally be wasted. ,[object Object],A mechanically driven pump uses some of this mechanical output. A turbocharger gets its energy from the exhaust gases, converting more of the fuel’s heat energy into mechanical energy.
Figure 23–8 A turbine wheel is turned by the expanding exhaust gases. ,[object Object],A turbocharger looks similar to a centrifugal pump for supercharging.  As hot exhaust gas enters the turbocharger, it rotates the turbine blades.  Turbocharger Design and Operation  A turbocharger consists of two chambers connected by a center housing. The chambers contain turbine and compressor wheels connected by a shaft. Continued
[object Object],Figure 23–9 The exhaust drives the turbine wheel on the left, which is connected to the impeller wheel on the right through a shaft. The bushings that support the shaft are lubricated with engine oil under pressure. To take advantage of the exhaust heat which provides rotating force, a turbocharger must be as close as possible to the exhaust manifold.  This allows exhaust to pass to the unit with minimum of heat loss. Continued
[object Object],Continued With no brake and little rotating resistance on the shaft, the turbine and compressor wheels accelerate as exhaust heat energy increases. When an engine is running full power, the turbocharger rotates at speeds between 100,000 and 150,000 rpm. Engine deceleration requires only a second or two because internal friction. The turbocharger has no such load and is turning many times faster than the engine at top speed. The oil in the center housing is then subjected to extreme heat and can gradually “coke” or oxidize. The coked oil can clog passages and will reduce the life of the turbocharger.
[object Object],Continued Both turbine and compressor wheels must operate with extremely close clearances to minimize possible leakage around their blades. Any leakage around the turbine blades causes a dissipation of the heat energy required for compressor rotation and prevents the turbocharger from developing its full boost pressure. Late-model turbochargers have liquid-cooled center bearings to prevent heat damage. Engine coolant circulates through passages in the housing to draw off excess heat, allowing bearings to run cooler and minimizing oil coking when the engine is shut down.
[object Object],Continued ,[object Object],[object Object],[object Object],[object Object]
[object Object]
BOOST CONTROL ,[object Object],Continued The “boost” amount (pressure in the intake manifold) is measured in pounds per square inch (psi), in inches of mercury (in. Hg), in bars, or in atmospheres.  The following values vary due to altitude and weather conditions:  1 atmosphere = 14.7 psi 1 atmosphere = 29.50 in .  Hg 1 atmosphere = 1.0 bar 1 bar = 14.7 psi
[object Object],Continued ,[object Object],[object Object],[object Object],[object Object],Higher temperatures decrease the durability of the turbocharger  and  the engine
Figure 23–10  The unit on top of this Subaru that looks like a radiator is the intercooler, which cools the air after it has been compressed by the turbocharger. ,[object Object],Power can be increased about 1% per 10°F by which air is cooled .   Some intercoolers use engine coolant to cool the hot compressed air that flows from the turbocharger to the intake.
The boost pressure of a turbocharger (or supercharger) is commonly measured in pounds per square inch. If a cylinder head is restricted because of small valves and ports, the turbocharger will quickly provide boost. Boost results when the air being forced into the cylinder heads cannot flow into the cylinders fast enough and “piles up” in the intake manifold, increasing boost pressure. If an engine had large valves and ports, the turbocharger could provide a much greater amount of air into the engine at the same boost pressure as an identical engine with smaller valves and ports. Therefore, by increasing the size of the valves, a turbocharged or supercharged engine will be capable of producing much greater power. Boost is the Result of Restriction
[object Object],Continued
Figure 23–11  A wastegate is used on the first-generation Duramax diesel to control maximum boost pressure. ,[object Object],Wastegate operation is a continuous process to control boost pressure. It is the pressure control valve of a turbocharger system.  The wastegate is usually controlled by the onboard computer through a boost control solenoid.  Continued
[object Object],Continued ,[object Object]
[object Object],Figure 23–12  A blow-off valve is used in some turbocharged systems to relieve boost pressure during deceleration. Continued The pressure increase opens the valve, and vents pressurized air directly to the atmosphere.  This operation of this type of relief valve is noisy, and creates a whooshing sound when the valve opens.
If One is Good, Two are Better A turbocharger uses exhaust from the engine to spin a turbine, connected to an impeller inside a turbocharger. This impeller then forces air into the  under pressure higher than is achieved without a turbocharger. The more air that can be forced into an engine, the greater the power potential. A V-type engine has two exhaust manifolds, and so two small turbochargers can be used to force greater quantities of air into an engine. Figure 23–13 A dual turbocharger system installed on a small block Chevrolet V-8 engine.
TURBOCHARGER FAILURES ,[object Object],Continued Bearing failure is a common cause of turbocharger failure, and replacement bearings are usually only available to rebuilders.  Another common problem is excessive, continuous oil consumption resulting in blue exhaust smoke.
[object Object],[object Object],[object Object],[object Object]
SUMMARY ,[object Object],[object Object],[object Object],Continued
SUMMARY ,[object Object],[object Object],[object Object],[object Object],( cont. )
end

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Chapter 23

  • 2.
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  • 4.
  • 5.
  • 6.
  • 7.
  • 8.
  • 9. SUPERCHARGING PRINCIPLES Figure 23–3 The more air and fuel that can be packed in a cylinder, the greater the density of the air–fuel charge. The force an air–fuel charge produces when ignited is largely a function of the charge density. Density is the mass of a substance in a given amount of space. The greater the density of an air–fuel charge forced into a cylinder, the greater the force and engine power it produces when ignited. An engine using atmospheric pressure for intake is called naturally ( normally ) aspirated . A better way to increase air density in the cylinder is to use a pump. Continued
  • 10.
  • 11.
  • 12.
  • 13.
  • 14.
  • 15.
  • 16.
  • 17.
  • 18.
  • 19.
  • 20.
  • 21.
  • 22.
  • 23.
  • 24.
  • 25.
  • 26.
  • 27.
  • 28.
  • 29.
  • 30.
  • 31. The boost pressure of a turbocharger (or supercharger) is commonly measured in pounds per square inch. If a cylinder head is restricted because of small valves and ports, the turbocharger will quickly provide boost. Boost results when the air being forced into the cylinder heads cannot flow into the cylinders fast enough and “piles up” in the intake manifold, increasing boost pressure. If an engine had large valves and ports, the turbocharger could provide a much greater amount of air into the engine at the same boost pressure as an identical engine with smaller valves and ports. Therefore, by increasing the size of the valves, a turbocharged or supercharged engine will be capable of producing much greater power. Boost is the Result of Restriction
  • 32.
  • 33.
  • 34.
  • 35.
  • 36. If One is Good, Two are Better A turbocharger uses exhaust from the engine to spin a turbine, connected to an impeller inside a turbocharger. This impeller then forces air into the under pressure higher than is achieved without a turbocharger. The more air that can be forced into an engine, the greater the power potential. A V-type engine has two exhaust manifolds, and so two small turbochargers can be used to force greater quantities of air into an engine. Figure 23–13 A dual turbocharger system installed on a small block Chevrolet V-8 engine.
  • 37.
  • 38.
  • 39.
  • 40.
  • 41. end