The invention pertains to gas exchange in internal combustion engines for increased efficiency.
The requirements to reduce CO2 emissions have led to there being increased focus on low and zero-emissions solutions for all types of propulsion machinery and other types of energy plant, including electric power production.
The challenges posed by eco-friendly fuels include their being more expensive than traditional fossil fuels. A realistic zero-emissions solution for shipping is ammonia, but this costs more than traditional operation using bunker oil.
One solution to compensate for the increased fuel costs is to improve the efficiency of the engines. In a traditional Otto process the efficiency of the process is a function of the expansion ratio. Efficiency can be improved by increasing the expansion ratio, but this is limited by the amount of cylinder pressure the engines can withstand and, in certain cases, the spontaneous ignition temperature of the fuel that is mixed with air in the cylinder.
Known technology includes engine designs using variable compression ratios. Coal and wood gas generators for running internal combustion engines.
Norwegian patent application 202000463 “Combustion chamber design in piston engines that use low-flammability fuels”.
Norwegian patent application 20191482 “Hybrid system for drones and other modes of transport”.
And Norwegian patent 343554, (PCT-WO/2019/035718)
“Zero emission propulsion systems and generator sets using ammonia as fuel.” that describes ignition of ammonia using pilot ignition.
In this description the term ‘compression stroke’ is used to describe the piston travel from bottom dead centre (BDC) up to top dead centre (TDC) before combustion and ‘expansion stroke’ is used for the piston travel from top dead centre (TDC) down to bottom dead centre (BDC) after combustion. The engine's cycles are the different processes carried out during a full work cycle.
The compression and expansion ratios in a piston engine are normally the same. The advantage of this invention is the way in which the gas exchange in the engine is changed, so that the compression cycle is reduced and only implemented in the final part of the compression stroke. By this means the engines can have a higher expansion ratio than traditional engines. This is achieved by reducing the quantity of air that is used in the combustion process by allowing the exhaust valve(s) to remain open through part of the compression stroke, thereby also reducing compression and thus the pressure increase before combustion. What is envisaged is a non-turbocharged engine running on an Otto process, where the optimal pressure in the cylinder, after the expansion is complete, will be the same as the pressure in the exhaust system or the pressure outside the engine. The engine has then made maximum possible use of the pressure increase from the combustion. The heat from the exhaust can also be used to drive other power-generating units, or as a heat source for various purposes such as heating water. This will enable even better utilisation of the fuel.
For 2-stroke engines, the gas exchange will be regulated by the opening times of the exhaust valves combined with compressors that regulate the quantity of air or air/fuel mixture supplied.
For 4-stroke engines, the inlet and exhaust valves will be regulated as follows:
Ammonia is a flammable substance that can be used as fuel for air-, sea- and land-based transport as well as in units designed for various purposes such as electric power production, water pumps etc. The disadvantage is that the flammability of ammonia is low, but as zero-emissions systems are defined as systems that do not emit CO2 the field is in practice limited to electric-, nuclear- or hydrogen-powered systems. Ammonia is the most straightforward means of storing hydrogen for hydrogen-powered systems.
In order to use ammonia as a fuel it will be advantageous to be able to use several propulsion systems, or alternatively to be able to use propulsion systems that can use several different fuels, such as dual-fuel or flex-fuel engines. The combustion characteristics of ammonia also mean that it will be advantageous for such engines to form part of a hybrid system, so that the internal combustion engines can operate at static load (constant load) and the hybrid system can deal with any load variations in the system. This can be achieved either using electrical hybrid systems where batteries and condensers will act as buffers to even out variations in the loads, or by using hydraulic or pneumatic hybrid systems where pressure tanks or pressure-loaded cylinders/vessels function as energy stores. The system will then have hydraulic pumps and motors, or compressors and turbines for pneumatic systems. If required, the power delivered by the internal combustion engines can be increased by supplying more air and fuels to the engine, or alternatively by running the engines purely on pilot fuel. This is realistic for ammonia-powered engines using diesel as the pilot fuel. If necessary, the engines can run as pure prechamber diesel engines. The exhaust valves will then close further down in the compression stroke and the ignition timing will be delayed in order to prevent cylinder pressure from being too high during combustion. This will reduce the efficiency, but will be a simple solution to enable high power output. Another solution is to use additional internal combustion engines, with traditional combustion, as part of the hybrid system to deliver high power when required.
To ensure good ignition of ammonia, a pilot ignition system will be essential to ignite the mixture of ammonia and air. This pilot ignition system can utilise pure hydrogen, other biofuels or traditional fossil fuels in both gaseous and liquid forms.
The system can be used for both 2-stroke and 4-stroke piston engines. Engines using the Diesel, Otto, Atkinson or other processes for piston engines are all covered by this invention.
1) The piston engine's intake system.
2) Exhaust valve.
3) The piston engine's exhaust system.
4) Control of the exhaust valves.
5) Compressor.
6) The prechamber.
7) Pilot Fuel Ignition Device
8) Connecting rod.
9) Piston rod.
10) The combustion chamber.
11) Injection Nozzle for the Main Fuel
12) Piston.
13) Cylinder head.
14) Crankshaft.
15) Cross head.
16) Temperature Sensor
17) Pressure Sensor
18) Air temperature sensor.
19) MAP sensor.
The optimal condition for achieving maximum efficiency in the process is for the pressure in the cylinder, after expansion is complete, to be the same as the pressure in the exhaust system (3) and for this exhaust pressure to be as close to the ambient or atmospheric pressure as possible.
The cylinder pressure after the expansion will be the controlling factor that determines how the gas exchange in the engine takes place. Cylinder pressure, together with the throttle setting, engine speed, data on the types of fuel used for both main and pilot fuels and signals from the emission reduction process will control the quantities of air, main fuel and pilot fuel to the engines. In turn, this will control injection and ignition timings as well as opening and closing of the exhaust valve(s) (2) with the control system for the exhaust valves (4).
The quantity of air fed to the cylinder will also include air needed for emission reduction. The quantity and types of fuel both for main and pilot fuels will give the air/fuel ratio (A/F). The quantity of air for gas exchange will be controlled by compressor(s) (5), alternatively also by inlet valves for 4-stroke engines and the height of the inlet ports (1) for 2-stroke engines. The engines can also be controlled in order to achieve a designated temperature range in the exhaust gas. The reason may be to exploit the exhaust for other purposes such as pyrolysis of solid fuels.
The principle of having pilot ignition from an additional pilot ignition system may also be applied to direct injection engines, whether they run on fossil diesel, bio-diesel, kerosene/jet fuel, gasoline, methanol/ethanol or LPG etc. The advantage is that the pressure in the compression stroke can be reduced in order to improve the efficiency of the engines by having a high expansion ratio and also ensure good combustion of the main fuel, with a greater proportion of the main fuel combusted by top dead centre (TDC). This will improve both efficiency and power output from the engines.
Instead of feeding solid fuels such as coal, lignin etc. directly to the engines, these fuels can be pyrolysed to produce gaseous fuels that are sucked into the intake system (1) together with air. Inter alia, this may be combined with coal that is used for production of coal gas and coke. The exhaust gas can then be used wholly or partially as a heat source for the pyrolysis process. For example, this can be part of a process for bio-coal production. During the 2nd World War wood gas from timber was used to produce gas by incomplete combustion in a wood gas generator. This gas was used as fuel in internal combustion engines. Coal can also be used in gas generators to produce a gas rich in carbon monoxide (CO). Some water can also be added during this combustion in order to ensure a certain hydrogen content (H2) in the gas. This will improve its combustion properties so that the gas will ignite and combust better in internal combustion engines.
When ammonia is used as a main fuel the engines will be run with a “rich” air/ammonia mixture in order to reduce NOx formation during the combustion, as well as to compensate as much as possible for the reduced power yielded by this process compared with a traditional Otto or Diesel process. A “rich” ammonia mixture, combined with an extra supply of air to the exhaust, will also assist NOx reduction using SCR.
The advantage of this process is also that if the engines are run on pure diesel oil one can reduce the excess air during combustion, compared with traditional diesel engines, for the same reasons as apply to ammonia. In these cases, the engines will operate with increased pressure in the intake system (1) in order to supply more air, so that some of the air is expelled into the exhaust system (3) to assist with reduction of the exhaust emissions. When using diesel, a supply of air to the exhaust may be required, both for reduction of exhaust emission in a particulate filter and possibly also for SCR when combined with added ammonia or urea.
If desirable, the power output can be increased at the expense of efficiency through more air or air/fuel mixture being sucked or forced into the cylinder while the exhaust valve(s) (2) are closed earlier i.e., further down in the compression stroke. By this means the engine will have more air and can combust more fuel. To prevent combustion pressure from being too high under such operating conditions, the combustion will occur later in the process so that more of the combustion takes place in the expansion stroke.
This method can also be utilised with other fuels. When using LNG/CNG/LPG as a main fuel an injection nozzle (11) may be used for supplying main fuel, or the main fuel may be mixed with air in the intake system (1).
If the main fuel is mixed in the intake system (1), the amount of air/fuel fed to the cylinder might need to be adjusted so that non-combusted fuel is not expelled into the exhaust (3). This can be done using a vane valve or other type of air regulator fitted to the intake system (1) or by controlling the quantity of air/fuel by regulating the compressor (5). Alternatively, both methods may be combined. In 4-stroke engines the intake valve(s) can also be controlled using the same type of control mechanisms as for the exhaust valves (4).
A possible means of optimising the gas exchange is for the cylinder to have several valves that can be operated individually. In 4-stroke engines especially, the exhaust valve(s) (2) and inlet valves can be opened and closed individually. This may be essential in order to ensure that air, which will subsequently be expelled for emission reduction, can be mixed in. During the induction stroke the intake valves will first open for air, then one of them will close while another is held partly open, so that further on in the induction stroke the exhaust valves (2) can be opened in order to reduce the pumping effort required. The quantity of exhaust that is sucked back into the engine will be mixed with a small quantity of air. The compression stroke will proceed with closed inlet valves, while the exhaust valves (2) will stay open some way up the compression stroke so that the exhaust and then a little air will be expelled again before the exhaust valves (2) close and compression of the remaining air starts.
A compressor (5) is not essential for 4-stroke engines, as these can function as traditional engines where air is drawn into the cylinder.
If the main fuel is mixed with air in the intake system (1), a special inlet valve to the combustion chamber (10) as described in Norwegian patent 343554 can be used to achieve good ignition of a pilot fuel.
If for example a main fuel such as propane (LPG) is mixed with air in the intake system (1) it is not necessary to have a separate prechamber (6) with its own injection nozzle or ignition device (7). Then the ignition device can be a spark plug placed in the combustion chamber (10) instead of an injection nozzle (11). If a spark plug is used, it must be positioned so that it can ignite the air/fuel mixture. Typically, it can be positioned so that the air/fuel mixture is ignited from the middle of the combustion chamber (10). This will give the quickest combustion of the fuel. It will also ensure that the spark from a spark plug is not prevented from igniting the air/fuel mixture by any exhaust remaining in the cylinder and combustion chamber (10) and being compressed into the top of the combustion chamber (10). A spark plug should therefore be positioned so that any remaining exhaust does not prevent the fuel from being ignited.
It may be desirable for some exhaust to remain in the cylinder during operation because it will act as EGR. This can be regulated by controlling the quantity of air or air/fuel mixture that is sucked or forced into the cylinder and by controlling the exhaust valve(s) (2).
The principles for the processes in a 2-stroke engine with ammonia as the main fuel, which is ignited using a pilot ignition of diesel, based on the embodiment in
The process described is based on the principles from a theoretical Otto process with the pressure increase at top dead centre (0 degrees).
Between point 1 and point 2 is the EXPANSION cycle.
Between point 2 and point 3 is the first part of the GAS EXCHANGE cycle.
Between point 3 and point 4 is the second part of the GAS EXCHANGE cycle.
Between point 4 and point 5 is the third and last part of the gas exchange which is EXHAUST EXPULSION together with air for emission reduction.
Between point 5 and point 1 is the COMPRESSION cycle.
The principles for a 2-stroke engine with LNG as the fuel based on the embodiment in
This type of engine does not require a prechamber (6) with an injection nozzle/ignition device (7). LNG will be mixed stoichiometric ally with air in the intake system (1) in a gas mixer, so an injection nozzle for the main fuel (11) is replaced by a spark plug positioned in the middle of the combustion chamber (10) to ensure good ignition. A spherical combustion chamber (10) will be used because of the combustion rate of methane gas. A compressor (5) regulates the amount of air fed to the gas mixer, which supplies a quantity of air/fuel to the cylinder. After the gas exchange there will be a remnant of exhaust left behind as EGR. Among other reasons, this is because the calorific value of LNG is much higher than for ammonia. Otherwise, the progression of compression and expansion will be as described above. LNG (and the same applies to LPG and ammonia) must be heated in an evaporator before entering the gas mixer. In an LNG system there will also be a pressure buildup unit (PBU) in order to ensure even pressure in the fuel.
The progression of one full work cycle (one revolution) will be as for other fuels, but the values for position (degrees), and thereby volume (m3), cylinder pressure (bar) and temperature (° C.) at the end of each cycle will naturally enough be different from those shown in Table 1 (below) which is for ammonia operation.
Values for the theoretical processes for a 2-stroke engine with ammonia as fuel based on the embodiment in
Table 1 is a simplified table showing values for the embodiment of a 2-stroke engine as illustrated in
The process in Table 1 is calculated on the following engine dimensions:
Bore: 1000 mm, Stroke: 2000 mm, Length of connecting rod: 2500 mm.
Height of inlet ports: 422.35 mm, which gives an expansion length in the cylinder of 1577.65 mm. This corresponds to an expansion ratio of 40:1 with a compression volume of 31.8 L.
The calculations for the process in Table 1 are based on pure air.
This applies to the compression from point 5 to point 1, the pressure increase in point 1 and the expansion from point 1 to point 2. The mass of air in these cycles is 387.17 g.
(There will be small variations in the values in Table 1 compared with calculations from one point to the next in the table. This is due both to the numerical values in Table 1 being rounded to one decimal point and to the values stated in Table 1 being based on a complete process from point 1 and back to point 1).
A natural starting point for a more detailed explanation of the values in Table 1 is point 5, which is where the compression begins.
Point 5 in Table 1 is where the exhaust valve (2) has been closed and the compression starts. The volume in this embodiment is 331.7 L with a pressure of 1 bar and temperature of 27° C. This corresponds to an air mass of 385.17 g. An isentropic compression to a volume of 31.8 L begins, and will result in a pressure after compression (TDC) of 26.9 bar and 498.6° C.
At point 1 (TDC) a pressure increase occurs, based on the amount of energy from a stoichiometric combustion of ammonia. There is an air mass of 385.17 g, with a volume of 31.8 L, pressure of 26.9 bar and temperature 498.6° C. to which an amount of energy equal to 1182.2 kJ is now introduced. This corresponds to the energy in 63.56 g of ammonia. This results in a temperature increase for 385.17 g air of 4305.4K to 4804.0° C. (Only the amount of energy introduced by the ammonia is used in the calculation; no admitted mass of ammonia is included.) This would have equated to an air/fuel ratio between air and ammonia of 385.17 g/63.56 g which is an A/F ratio of 6.06, or λ=1 for air/ammonia. The pressure increase after combustion will take place after an isochoric process and the pressure will increase to 176.7 bar. An isentropic expansion will begin.
At point 2 there has been an isentropic expansion of a mass of air of 385.17 g from point 1 to a volume of 1270.9 L. This gives a pressure after expansion of 1 bar and a temperature of 876.3° C.
From point 2 to point 4 is gas exchange. For this embodiment, this takes place at a pressure of 1 bar and the air that is forced in maintains a temperature of 27° C.
From point 4 to point 5, exhaust will be expelled. For this embodiment the quantity of air forced in between point 2 and point 4 is the quantity of air required for the combustion, so no air is expelled in the process between point 4 and point 5. The air will still have a pressure of 1 bar and a temperature of 27° C.
Number | Date | Country | Kind |
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20200639 | May 2020 | NO | national |
Filing Document | Filing Date | Country | Kind |
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PCT/NO2021/050130 | 5/23/2021 | WO |