Friday 30 September 2011

MICROTURBINES


                                                      ABSTRACT
              Distributed generation is one of the important field of research now a days. Market prospect for microturbine for distributed power generation and their associated high grade heat extremely encouraging. Therefore microturbines are becoming a point of study. Presented paper tries to discus the microturbine concept, technology description gives technical and practical background through basic process and thermodynamic cycle. Various components of microturbine and their performance is briefly analyzed.
             To improve this characteristics and efficiency the points like development of chemically recuperated gas turbine is added. Microturbine economics is a big question .Fuel used for microturbine gives list of all possible fuel to be used. Manufacturers and availability of microturbine is one important discussed point. Application gives idea about customer range, customer targeted stand by power, hybrid   electric vehicles, CHP operation, etc. At the end conclusion is drawn for the feasibility study of microturbine                                         



  TECHNOLOGY   DISCRIPTION OF MICROTURBINES

2.1 Basic Processes
                               Microturbines are small gas turbines, most of which feature an internal heat exchanger called a   recuperator. In a microturbine, a radial flow (centrifugal) compressor compresses the inlet air that is then preheated in the recuperator using heat from the turbine exhaust. Next, the heated air from the recuperator mixes with fuel in the combustor and hot combustion gas expands through the expansion and power turbines. The expansion turbine turns the compressor and, in single shaft models, turns the generator as well. Two-shaft models use the compressor drive turbine’s exhaust to power a second turbine that drives the generator. Finally, the recuperator uses the exhaust of the power turbine to preheat the air from the compressor. Single-shaft models generally operate at speeds over 60,000 revolutions per minute (rpm) and generate electrical power of high frequency, and of variable frequency (alternating current --AC).  This power is rectified to direct current (DC) and then inverted to 60 hertz (Hz) for U.S. commercial use. In the two-shaft version, the power turbine connects via a gearbox to a generator that produces power at 60 Hz. Some manufacturers offer units producing 50 Hz for use in countries where 50 Hz is standard, such as in Europe and parts of Asia.
2.2 Thermodynamic Cycle
Microturbines operate on the same thermodynamic cycle, known as the Brayton cycle, as larger gas turbines. In this cycle, atmospheric air is compressed, heated, and then expanded, with the excess power produced by the expander (also called the turbine) over that consumed by the compressor used for power generation. The power produced by an expansion turbine and consumed by a compressor is proportional to the absolute temperature of the gas passing through those devices. Consequently, it is advantageous to operate the expansion turbine at the highest practical temperature consistent with economic materials and to operate the     compressor with inlet airflow at as low a temperature as possible. Higher temperature and pressure ratios result in higher efficiency and specific power. Thus, the general trend in gas turbine advancement has been towards a combination of higher temperatures and pressures. However, microturbine inlet temperatures are generally limited to 1,800ºF or below the use of relatively inexpensive materials for the turbine wheel, and to maintain pressure ratios at a comparatively low 3.5 to 4.0.

2.3 Basic Components

2.3.1 Turbo-Compressor Package

                                           The basic components of a microturbine are the compressor, turbine generator, and recuperator   Figure 2.3.1. The heart of the microturbine is the compressor-turbine package, which is commonly mounted on a single shaft along with the electric generator. Two bearings support the single shaft. The single moving part of the one-shaft design has the potential for reducing maintenance needs and enhancing overall reliability. There are also two-shaft versions, in which the turbine on the first shaft directly drives the compressor while a power turbine on the second shaft drives a gearbox and conventional electrical generator producing 60 Hz power. The two shaft design features more moving parts but does not require complicated power electronics to convert high frequency AC power output to 60 Hz.         
                            
                                       Moderate to large-size gas turbines use multi-stage axial flow turbines and compressors, in which the gas flows along the axis of the shaft and is compressed and expanded in multiple stages. However, microturbine turbo machinery is based on single-stage radial flow compressor and turbines. Rotary vane and scroll compression are the most commonly used technology in the microturbine industry. Second generation gas compressor technologies are in development or being introduced. That may reduce costs and target on-board application Rotary vane compression technology offers a wide range of gaseous fuel flexibility Parasitic loads vary based on type of gas and inlet  pressures available, general rule 4 to 6% for natural gas and 10 to 15% for bio gas.
2.3.2 Generator
                    The microturbine produces electrical power either via a high-speed generator turning on the single turbo-compressor shaft or with a separate power turbine driving a gearbox and conventional 3,600 rpm generator. The high-speed generator of the single-shaft design employs a permanent magnet (typically Samarium-Cobalt) alternator, and requires that the high frequency AC output (about 1,600 Hz for a 30 kW machine) be converted to 60 Hz for general use. This power conditioning involves rectifying the high frequency AC to DC, and then inverting the DC to 60 Hz AC. Power conversion comes with an efficiency penalty (approximately five percent).To start-up a single shaft design, the generator acts as a motor


turning the turbo-compressor shaft until sufficient rpm is reached to start the combustor. Full start-up requires several minutes. If the system is operating independent of the grid (black starting), a power storage unit (typically a battery UPS) is used to power the generator for start-up.
2.3.3 Recuperators
                    Recuperators are heat exchangers that use the hot turbine exhaust gas (typically around 1,200ºF) to preheat the compressed air (typically around 300ºF) going into the combustor, there by reducing the fuel needed to heat the compressed air to turbine inlet temperature. Depending on microturbine operating parameters, recuperators can more than double machine efficiency. However, since there is increased pressure drop in both the compressed air and turbine exhaust sides of the recuperator, power output typically declines 10 to 15% from that attainable without the recuperator. Recuperators also lower the temperature of the microturbine exhaust, reducing the micro turbine’s effectiveness in CHP applications.
2.3.5 Air bearings
                 They allow the turbine to spin on a thin layer of air, so friction is low and rpm is high. No oil or oil pump is needed. Air bearings offer simplicity of operation without the cost, reliability concerns, maintenance requirements, or power drain of an oil supply and filtering system. Concern does exist for the reliability of air bearings under numerous and repeated starts due to metal on metal friction during startup, shutdown, and load changes. Reliability depends largely on individual manufacturers' quality control methodology more than on design engineering, and will only be proven after significant experience with substantial numbers of units with long numbers of   operating hours and on/off cycles.
2.3.6 Power Electronics
.              The high frequency AC is rectified to DC, inverted back to 60 or 50 Hz AC, and then filtered to reduce harmonic distortion.. To allow for transients and voltage spikes, power electronics designs are generally able to handle seven times the nominal voltage. Most icroturbine power electronics are generating three phase electricity. Electronic components also direct all of the operating and startup functions.

                                                                 
                    FIG 2.3.1 MICROTURBINE BASED CHP SYSTEM ( SINGLE SHAFT )

                               
             
FIG  2.3.2   BASIC  PARTS OF MICROTURBINE
                                                                     
                                                                        
                                                                       

 FIG 2.3.3 MICROTURBINE CONSTRUCTION

Chapter 3
                                  

Design Characteristics 0f microturbines

                                  Thermal output: Microturbines produce thermal output at   temperatures     in the  400 to 600°F range, suitable for supplying a   variety of building  thermal needs.
                  
Fuel flexibility:       Microturbines can operate using a number of different fuels:                                 
                                 Sour gases (high sulfur, low Btu content), and liquid fuels such                               
                                 as gasoline, kerosene, natural gas and diesel fuel/heating oil.

Life                          Design life is estimated to be in the 40,000 to 80,000 hour range.             

Size  range:              Microturbines available and under development are sized                                                                                                                              
                                  From 25 to 350 KW

Emissions:              Low inlet temperatures and high fuel-to-air ratios result in   NO                                                                                                                            
                                 Emissions of less than 10 parts per million (ppm) when
                                  Running on natural gas               

Modularity:            Units may be connected in parallel to serve larger loads and     
                                 Provide power reliability
                      
Dimensions:            About 12 cubic feet.        


Chapter 4
Microturbines and distributed generation
  Distributed generation, a concept first promoted by Thomas Edison in the 19th century, is rewiring the way facility. Operators and environmental mangers think about how electric power can be produced and distributed. For decades, energy users have waited for the promise of fuel cells, solar panels, and wind turbines to translate into reliable and economically viable sources of power. The table shown below compares the microturbines with other D.G.  resources. Microturbines are quietly delivering on those promises and proving to be a supplement to traditional forms of power generation.    Moving away from 100% dependence on the utility power grid to having an onsite microturbine power supplement is, admittedly, a Para diagram shift. But for progressive environment mangers worldwide, microturbines are quickly becoming an energy management solution that saves money, resources, and the environment in one compact and scalable package- is it stationary or mobile, remote or interconnected with the utility                
                                                                       


Chapter 5
Economics of Microturbines[
                                        Micro turbine capital costs range from $700-$1,100/kW. These costs include all hardware, associated manuals, software, and initial training. Adding heat recovery increases the cost by $75-$350/kW. Installation costs vary significantly by location but generally add 30-50% to the total installed cost. Micro turbine manufacturers are targeting a future cost below $650/kW. This appears to be feasible if the market expands and sales volumes increase.        
                                    With fewer moving parts, micro turbine vendors hope the units can provide higher reliability than conventional reciprocating generating technologies. Manufacturers expect that initial units will require more unexpected visits, but as the products mature, a once-a-year maintenance schedule should suffice. Most manufacturers are targeting maintenance intervals of 5,000-8,000 hours.
                                Maintenance costs for micro turbine units are still based on forecasts with minimal real-life situations. Estimates range from $0.005-$0.016 per kWh, which would be comparable to that for small reciprocating engine systems.
Micro turbine Cost
Capital Cost
$700-$1,100/kW
O&M Cost
$0.005-0.016/kW
Maintenance Interval
5,000-8,000 hrs



Chapter 6
Fuel Flexibility of microturbines[2][3]
             Microturbines are small power plants operate on natural gas, diesel, gasoline or other similar high-energy, fossil fuel. However, research is progressing on using lower grade; lower energy fuels such as gas produced from biomass to power the microturbine. This gas, called biogas, is a combustible gas derived from decomposing biological wastes that have undergone conversion by biological decomposition called anaerobic digestion or by thermal decomposition in a gasifier which is called pyrolysis.
In a forest, a gasifier could be used to convert wood chips and pine needles to a biogas on site. By making modifications, the turbine will be able to utilize low pressure fuels with lower energy content than traditional fuels. Natural gas-fired turbines have fuel with a heating value of 1,000 British thermal units per cubic foot. Biogases typically have between 10 and 20 percent of the heating value of fossil fuels. The thrust of current research is concentrated on fuel flexibility. The goal is to modify microturbines so they can utilize low energy, low pressure biogases. In order to do this, a key change is to add a catalytic combustor. An added benefit of the catalytic combustor is that it will eliminate the formation of nitrogen oxides, a technology breakthrough. These modified microturbines have been nicknamed "Flex-microturbines".                                        


Chapter 7
              
                    MIROTURBINES TEST PROCEDURE & INSTALLATION

7.1 Test Procedures [3]
                                        To fully evaluate the MTGs, a series of tests were developed. Testing of MTGs has been   categorized into the following phases:
  • Installation and Startup.
  • Operation and Maintenance.
  • Performance.
      
7.2 Installation and Startup Procedures
                                  Each MTG delivered to the test site was inspected and confirmed to include:
·         Operating instructions.
·         Repair parts or a recommended spare parts list.
·         Consumable supplies.
·         Troubleshooting and maintenance procedures/guides.
·         Drawings and diagrams sufficient to support maintenance.

7.3 Performance Procedure
      For the test program, MTGs were operated for as long as practicable at the full load the units were capable of producing under ambient conditions. Daily operating parameters: fuel flow, ambient air pressure, temperature and humidity, energy output, operating temperatures, and pressures were recorded. The recorded MTG parameters were used to determine heat rate and   efficiency, gross and net peak kilowatts, operating hours, capacity factor and availability. Capacity factor for an operating period is the ratio of the actual kilowatt hours generated to the maximum potential kilowatt hours for the rating of the unit. Availability for an operating period is the ratio of the hours the unit was not restricted from operation due to maintenance or repairs unit to the maximum possible hours of operation. Peak gross power is defined as the peak power output by the MTG inverter.


                                                        Chapter 8
  
             Development of Chemically Recuperated Micro gas turbine [1]       

outline of the chemically Recuperated Gas Turbine (CRGT) System

              Figure 8.1 shows a block diagram of a CRGT system. In an MGT system, turbine exhaust temperature is about 600°C, and the power generation efficiency is increased by heat recovery of air recuperator, but in CRGT system, the reformer recovers the turbine heat first. As shown in Fig. 8.1 .The equipment after the reformer is the air recuperator, and next is the evaporator, but the system works if sequence of lie equipment after the reformer is arranged in accordance with layout of the engine system of micro gas turbines The amount of   heat recovered by the reformer is determined by enthalpy change of chemical reaction which converts fuel and steam into hydrogen rich gas. The principal reactions in a reformer are expressed as follows:
                                                                                                                                
                  The reaction rate of water gas shift is larger than that of steam reforming, and it is regarded as equilibrium. Thus, the molar stoicometric ratio between methane and steam (i.e., steam carbon ratio, SIC) in the above reactions is 2.0, but SI\C is operated from 3 to 4 in order to avoid deposition of carbon by Boudouard’s reaction expressed as follows:
                        The steam reforming reaction occurs partially below 600°C, methane of 100% is not converted into hydrogen-rich gas. The maximum conversion of methane is limited thermodynamically, which is influenced  by physical conditions: temperature T, total pressure P. and SI\C   For example, equilibrium conversion is about 35% under the conditions of ‘I’ 500°C, P=0.4 MPa, and S/C = 4.0. The reaction pressure P in the reformer is higher than that in the combustor and it ranges between 0.3 and 0.5 Mpa. The more temperature or S/C increases, the more equilibrium conversion increases. Therefore, it is preferable that temperature and SIC in the reformer are set high to enlarge heat recovery.                   
However, configurations of the gas turbine and the evaporator restrict the amount of steam, and S/C has an upper limit. In the gas turbine, surge limit of the compressor determines the maximum flow rate including steam through the turbine. In the evaporator, the upper limit of    steam generation is determined because the pinch point temperature difference becomes critical. Hence, the maximum S/C is set to approximately 7 Besides, the temperature in the reformer   is influenced by the configuration of the reformer because the reaction occurs in the reformer exchanging heat with turbine exhaust. Hence, the design of the reformer is very important
 Figure 8.1 shows the principal stream conditions of a chemically recuperated MGT based on a commercial 75 kW MTG system using natural gas as fuel. Figure8.2 shows a schematic illustration of heat balance in the system .Figure 8.2 also shows each energy percentage of natural gas LHV (lower heating value) .. In the system shown in Fig. 8.1, as much steam possible is generated to enlarge heat recovery by large conversion and S/C is set to 6.3. The heat duty of the reformer is estimated considering reactions as equilibrium, and the reformer uses exhaust heat from 656°C to 561°C. The mole fraction of hydrogen is the reformer output is 24%, and the conversion rises to 51%. The heat recovery at the reformer is 82.4 kW, which recovers 25.6% of fuel LHV. The air   recuperator is placed after reformer and it heats compressed air until 520°C using exhaust heat from 561°C to 274°C. This recovers 40.5 kW. The evaporator uses the bottom of exhaust heat from 274°C to 121°C. According to this system analysis, the output and the efficiency were expected to improve up to 98 kW and 30.4%, respectively, comparing with 75 kW and 28% of the original MGT.

                                                   
                      
                          Fig 8.1 The principle stream conditions for CRGT system                       
                      

                                                                                      


               Fig 8.2 heat balance in CRGT system expressed as % of natural gas LHV




Chapter 9

Applications of Microturbines [4]
Combined heat and power (co-generation) (chp)
 Waste heat from the microturbine can be transferred via a heat exchanger to produce steam or provide hot water for local area. The hot water can be used in a greenhouse to grow plants; water can be ducted to provide central heating in buildings in winter. Thermal hosts can be found easier because the heat produced by each microturbine unit is so much smaller than that by a large power station.
Distributed power generation
Hospitals, hotels, factories and holiday resorts can install distributed power systems on site to supplement power supplied by grid. Also, electricity can be generated at remote sites without grid access. Distributed generation provides a wide range of services to consumers and utilities, including standby generation, peak shaving capability, baseload generation and co-generation.
Hybrid (microturbine connected to high speed alternator):[4]
  In hybrid vehicle applications, the power produced by a microturbine is converted into electricity by a high-speed alternator. The power is used to drive electric motors    connected to   the wheels. Any excess energy is directed to an energy storage system such as batteries or flywheels.
Hybrid vehicle (microturbine and fuel):
       Hybrid systems take advantage of an increase in fuel cell efficiency with an increase in          operating pressure. The microturbine compressor stage is used to provide this pressure. The fuel cell produces heat along with power, and this heat energy is used to drive the microturbine’s turbine stage. If the fuel cell produces enough heat, the microturbine can generate additional wer. For the hybrid combination, efficiency is expected to be as much as 60% and emissions less than 1.0 ppm NOx, with negligible Sox and other pollutants.





Chapter 10

Conclusion

                                                    
                                                      The drawbacks of centralized power generation and shortage of power leading to concept of Distributed generation (DG).DG tends to several advantages and concept of DG is more feasible. Microturbine is the application of DG .The history of IC engine . Shows several year research works for todays better result. Therefore microturbine is tomorrows world. Microturbine can use low grade of fuel very effectively like waste gases, sour gases etc.
                                           Thus microturbine gives chance of low fuel cost and less emission. The dimensions of Microturbine comparatively small by which it can be installed at field where power is consumed. It has few efficiency problems. Due to chemical recuperation the thermal efficiency increases sharply. Microturbine is also effective in CHP operation .It is having  problem of   Starting time and thats why it fails as standby power generator compared to IC engines. In India the microturbine is quite useful. The power shortage effect can be solved using microturbine, using fuels like biogas, etc .But in India the technology is still underdevelopment so the present seminar is an honest attempt to introduce microturbine technology in India for solving the problem of power generation in future.


Thursday 29 September 2011

A NEW CONCEPT OF I.C. ENGINE WITH HOMOGENOUS COMBUSTION IN POROUS MEDIUM

                                                Abstract
                                At present, the emissions of internal combustion engines can only be improved by catalytic treatments of the exhaust gases. Such treatments, however, result in high costs and relatively low conversion efficiency. This suggests that a new combustion technique should be developed to yield improved primary combustion processes inside the engine with drastically reduced exhaust gas emissions. In this paper,. We report on such a technique that is applicable to direct injection, internal combustion engines, either diesel or gasoline fuelled. This technique is based on the porous-medium (PM) combustion technology previously developed in the laboratory for steady state household and industrial combustion processes. It is shown that the PM combustion technique can be applied to internal combustion engines, i.e. it is demonstrated that improvements obtained in steady state combustion are also realizable in unsteady combustion processes. Theoretical considerations are presented for internal combustion engines, indicating that an overall improvement in thermal efficiency can be achieved for the PM engine. This is explained and the general performance of the new PM engine is demonstrated for a single-cylinder, air-cooled, direct injection diesel engine. Verification experiments are described that were carried out as part of the present study. Initial results are presented and an outlook is given on how the present developments might continue in the future.

                                                     Introduction

                        Gradually came the days when man started imagining huge & started striving for bringing his imagination to the day of light Today after having reached such heights of advancement we the human beings are still in thirst of technology indeed very desperately. One such field for current discussion and interest of brilliant brains is that how we developed such a engine which would give non-zero emission and as well as less fuel consumption to with stand under wild range of speed and load?  the answer to this question is homogeneous combustion in I.C. engine using porous medium Technology.
                        The process of mixture formation, ignition & combustion in conventional engine is not effective due to the lack of mechanisms for homogenous combustion process.
                        Two parameters will be required for future internal combustion engine i.e. non-zero emission level & low fuel consumption. These parameter is strongly dependant the process of mixture formation & combustion which are difficult to controlled in a conventional engine combustion system.                  
                        The question is remain unsolved is the method for realization of homogenous combustion in IC engine, specially if the variable engine operational conditions are considered.
                        So here porous medium concept is introduced in order to overcome above difficulty. PM utilize the special features of highly porous media to support and controlled the mixture formation and combustion process in IC engine.

                      Main requirements for future engine

                        Basic requirements for future clean internal combustion (I.C.) engine concern very low that is exhaust emissions level for both gaseous and particulate matter components under as low as possible fuel consumption. Internal combustion engine has to operate in a wide range of speeds and loads and should satisfy selected requirements under all operational conditions. For vehicle application, the following conditions are required for future engine:
                        Operation with a homogeneous stoichiometric charge for high power density  Operation with a homogeneous-lean charge for low specific fuel consumption
                        Realization of homogeneous combustion, for all mixture compositions for the lowest combustion emissions.
                        For significant reduction of specific fuel consumption and for a near-zero combustion emissions especially attractive would be realization of engine operating with a lean-homogeneous charge at part loads, assuming that the combustion process is homogeneous.                

                     HOMOGENEOUS COMBUSTION
                         Homogeneous combustion in an IC engine is defined as a process characterized by a 3D-ignition of the homogeneous charge with simultaneous-volumetric-combustion, hence, ensuring a homogeneous temperature field. According to the definition given above, three steps of the mixture formation and combustion may be selected that define the ability of a given combustion system to operate as a homogeneous combustion system
                        The PM has homogeneous surface temperature over the most of the PM-volume, higher than the ignition temperature. In this case the PM-volume defines the combustion chamber volume. Thermodynamically speaking, the porous medium is here characterized by a high heat capacity and by a large specific surface area. As a model, we could consider the 3D-structure of the porous medium as a large number of “hot spots” homogeneously distributed throughout the combustion chamber volume. Because of this feature a thermally controlled 3D-ignition can be achieved. Additionally, the porous medium controls the temperature level of the combustion chamber permitting the NOx level control almost independently of the engine load or of the (A/F) ratio
                                                                       




POROUS MEDIUM (PM) TECHNOLOGY
                        The porous medium technology for IC engines means here the utilization of specific features of a highly porous media for supporting and controlling the mixture formation and combustion processes in I.C. engines. The employed specific features of PM are directly related to a very effective heat transfer and very fast flame propagation within the PM. close view of a magnified 3D-structure of SiC ceramic foam is given in Figure
                                                                    



 Generally, the most important parameters of PM for application to engine combustion technology can be given as follows: heat capacity, specific surface area, heat transport properties, transparency for fluid flow, spray and flame propagation, pore sizes, pore density, pore structure, thermal resistance of the material, mechanical resistance and mechanical properties under heating and cooling conditions, PM material surface properties. For IC engine application, the thermal resistance of the porous medium is one of the most important parameter defining its applicability of a given material to combustion in engine. A view of the thermal test of SiC-reactors for engine application is shown in Fig.




                                                                                                                                       
New concept of mixture preparation for homogeneous combustion in engines using porous medium technology


                                          

                        Different R&D activities of the author using porous materials (highly porous 3D-structures) (see LSTM at University of Erlangen-Nürnberg and Promos GmbH in Erlangen) indicated unique features of this technology for mixture formation and combustion processes, also as applied to IC engines.


                   Energy recirculation in engine cycle in the form of hot burned gases recirculation or combustion energy:- This may significantly influence thermodynamic properties of the charge in the cylinder and may control its ignitability (activity). This energy recirculation may be performed under different pressures and temperatures during the engine cycle. Additionally, this heat recuperation may be used for controlling the combustion temperature level.

                   Fuel injection in PM-volume:- Especially unique features of liquid jet distribution and homogenization throughout the PM-volume
Fuel vaporization in PM-volume:- Cmbination of large heat capacity of the PM-material, large specific surface area with excellent heat transfer in PM volume make the liquid fuel vaporization very fast and complete.
                   Mixing and homogenization in PM-volume:- Unique features of the flow properties inside 3D-structures allow very effective mixing and homogenization in PM-volume.
                   3D-thermal-PM-ignition:- (if PM temperature is at least equal to ignition temperature under certain thermodynamic properties and mixture composition): there is a new kind of ignition, especially effective if the PM-volume creates the combustion chamber volume.
                   Heat release in PM-volume:- Under controlled combustion temperature that permits homogeneous combustion conditions almost independently of the engine load with possibility of controlling the combustion temperature level.

                                   PRINCIPLE OF THE PM-ENGINE

                                The PM-engine is here defined as an internal combustion engine with the following processes realized in a porous medium: internal heat recuperation, fuel injection, fuel vaporization, mixing with air, homogenization of charge, 3D-thermal self-ignition followed by a homogeneous combustion. PM-Engine may be classified with respect to the heat recuperation.
                        One of the most interesting features of PM-engine is its multifuel performance. Independently of the fuel used, this engine is a self-ignition engine characterized by its 3D-thermal ignition in porous medium. Finally, the PM-engine concept may be applied to both two- and four-stroke cycles. Owing to the differences in thermodynamic conditions, the PM-engine cycle has to be separately analyzed for closed and open chambers
PM-engine with closed chamber


                

                        Let us start an analysis of the PM-engine cycle with a case of closed PM chamber, i.e. engine with a periodic contact between working gas and PM-heat recuperator. At the end of the expansion stroke the valve controlling timing of the PM-chamber closes and fuel is injected in the PM-volume. This volume represents in thermodynamic sense a low pressure chamber and a long time is available for fuel injection and its vaporization in the PM. These processes may continue through exhaust, intake and compression strokes (see Fig.)

                                                                     


Near the TDC of compression the valve in PM-chamber opens and the compressed air flows from the cylinder into the hot PM volume containing fuel vaporous. Very fast mixing of the gaseous charge occurs and the resulting mixture is ignited in the whole PM volume. The resulting heat release process performs simultaneously in the whole PM volume. The three essential conditions for a homogeneous combustion are here fulfilled: homogenization of charge in PM-volume, 3D-thermal self-ignition in PM and volumetric combustion with a homogeneous temperature field in PM-volume. Additionally, the PM-material deals as a heat capacitor and, hence, controls the combustion temperature. 
                           Advantages of PM Technology
1)Very low emissions level due to homogeneous combustion and controlled           temperature in the PM-combustion zone (e.g. NOx between 100 and 300mg/kWh for the (A/F) ratio from 1 to 5;. CO can be reduced by several times; (almost) eliminated soot formation).
            2) Theoretically higher cycle efficiency due to similarity to the Carnot cycle.
            3) Very low combustion noise due to significantly reduced pressure peaks.
4) Nearly constant and homogeneous combustion temperature field in the PM-       volume.
            5) Very fast combustion.
            6) Multi-fuel system.
7) May operate with homogeneous charge: from stoichiometric to very lean mixture  compositions.
            8) Weak effect of in-cylinder flow structure, turbulence or spray atomization              

                                              Conclusion
                        There is no doubt that the future of internal combustion engine is related to the homogeneous combustion process in a wide range of engine operational conditions.
This technique shows potential for a near-zero combustion emissions (especially NOx and soot) as well as high cycle efficiency (low fuel consumption). Moreover, this kind of combustion system is less fuel specific. However, the realization of homogeneous combustion in IC engine under variable loads and speeds will probably require new concepts for mixture formation and controlled ignition conditions under different engine loads. The future engine operating with a homogeneous combustion process in a wide range of load and speed will require variable temperature history during the compression stroke, variable TDC compression temperature, completely vaporized fuel prior the ignition process, variable mixture composition (A/F ratio), variable reactivity (ignitability) of the charge, homogeneity of the charge, volumetric ignition conditions, variable heat capacity of the cylinder content. But the research has been carried out to make this process more & more economical.