The present disclosure relates generally to ignition systems for engines, including gas turbine engines and internal combustion engines, and more particularly to a high-energy remote chamber ignition system.
Combustion processes are expected to be the dominant technology used for generating the energy that is needed to power the world's economic and transportation infrastructure for the foreseeable future. It is well known that the emissions from such processes can be harmful to the environment, both on a local scale and globally. For instance, the combustion of fossil fuels produces carbon dioxide, which is a so-called greenhouse gas that is known to be responsible for global warming and the climate change associated therewith. Levels of carbon dioxide in the atmosphere have been increasing since the start of the industrial revolution in the 18th century, causing global concern in recent years and prompting industrialized nations to commit to reducing their carbon emissions. Unfortunately, many countries are currently on-track to miss their stated carbon emission reduction targets.
One approach to reducing carbon emissions from combustion processes involves a shift to low-to-zero-carbon fuels, which can significantly reduce or even eliminate entirely such carbon emissions. For example, when natural gas is used instead of coal for power generation, CO2 emissions can be reduced by over 30%. CO2 emission can be further reduced when renewable natural gas (RNG) is used. Of course, combustion processes that use fuels such as hydrogen and ammonia have zero CO2 emission, because the fuels that are being burned do not contain any carbon. However, producing the zero-carbon fuels may require energy that itself produces carbon emissions. For instance, hydrogen may be produced using non-renewable energy sources such as natural gas or coal-fired electricity plants, which do produce carbon emissions. Furthermore, combusting zero-carbon fuels such as hydrogen often produces other harmful pollutants such as NOx.
The challenge in achieving high efficiency, clean combustion of natural gas and ammonia lies in the low chemical reactivities of these two fuels. It is known that the adoption of clean combustion technologies, such as lean burn and inert gas dilution, can significantly reduce combustion temperature, which reduces pollutant emissions for traditional fuels. Unfortunately, for renewable fuels such as natural gas and ammonia, which have low chemical reactivities, achieving complete combustion of the fuel continues to be a challenge.
It therefore follows that an ignition source, capable of supplying sufficient ignition energy to establish a fast and reliable combustion of the air/fuel mixture, is required for the further development of combustion systems that use low carbon or zero carbon renewable fuels with low chemical reactivity, such as renewable natural gas and ammonia fuels.
Several ignition technologies have already been proposed and developed, none of which are completely satisfactory. For instance, a passive pre-chamber ignition system has been developed to generate local turbulence to shorten the combustion duration of the air fuel mixture, leading to higher engine efficiencies. This technique is mostly used in stationary natural gas generators, where in-cylinder turbulence intensity is low because of the lower piston speed. Limited applications are also seen in automotive engines to reduce the combustion duration of the air/fuel mixture.
Active pre-chamber ignition systems can further adjust the air/fuel ratio in the pre-chamber, which is suitable for lean and EGR (exhaust gas recirculation) diluted combustion strategies to further improve engine efficiency. Unfortunately, the potential improvement in combustion efficiency is limited because of the limited volume of the pre-chamber.
Diesel-natural gas dual fuel engines use the autoignition of pilot injection diesel as the ignition source for the natural gas air/fuel mixture. The ignition is normally in the range of ˜30 to ˜200 J, which is much higher than that of the pre-chamber ignition systems that have been discussed above. Ignition capability is significantly improved, but at the cost of increased soot emission because of the direct-injected diesel fuel.
It would be beneficial to provide a method and apparatus that overcomes at least some of the above-mentioned disadvantages and/or limitations.
In accordance with an aspect of at least one embodiment there is provided an ignition system for an internal combustion engine having an engine cylinder, the ignition system comprising: a remote ignition chamber enclosing an ignition source; and a tubing assembly, comprising: a tube disposed between the remote ignition chamber and a main combustion chamber defined within the engine cylinder, the tube having a central passageway bounded by a wall and defining a flame propagation pathway between the remote ignition chamber and the main combustion chamber; a plurality of high-voltage electrodes arranged along a length of the tube and extending through the wall of the tube into the central passageway: a plurality of high-energy discharge sparkplugs arranged along the length of the tube and being mounted through the wall of the tube such that a spark gap of each of the high-energy discharge sparkplugs is positioned within the central passageway; and an electronic controller in electrical communication with the plurality of high-voltage electrodes and in electrical communication with the plurality of high-energy discharge sparkplugs, the electronic controller, in use, for providing first control signals for controlling the plurality of high-voltage electrodes for pretreating a combustible charge gas inside the tube prior to combustion thereof, and the electronic controller, in use, for receiving signals relating to properties of a flame propagating within the tube and sensed using the plurality of high-energy discharge sparkplugs, the signals for use in determining spark timing of at least one sparkplug of the plurality of high-energy discharge sparkplugs for stimulating deflagration-to-detonation transition.
In an embodiment there is provided a temperature control layer at least partially surrounding the tube along at least a portion of the length of the tube for controllably varying a temperature of the wall of the tube during use.
In an embodiment there is provided a first injector in fluid communication with the remote chamber for injecting a fuel into the remote chamber, wherein the injected fuel is a first component of the combustible charge gas.
In an embodiment there is provided a second injector in fluid communication with the remote chamber for injecting a gas comprising molecular oxygen into the remote chamber, wherein the injected gas is a second component of the charge gas.
In an embodiment there is provided a valve disposed proximate an end of the tube that opens into the main combustion chamber, the valve being controllably switchable between an open position allowing fluid flow through the valve and a closed position preventing fluid flow through the valve.
In an embodiment there is provided a high voltage power drive in electrical communication with the plurality of high-voltage electrodes and with the electronic controller, wherein the electronic controller provides the first control signals to the high voltage power drive and the high voltage power drive energizes the plurality of high-voltage electrodes in dependence thereon.
In an embodiment the sparkplugs of the plurality of sparkplugs comprise: a first set of two or more spark plugs disposed at a first distance along the length of the tube and circumferentially spaced-apart one from the other, and a second set of two or more spark plugs disposed at a second distance along the length of the tube and circumferentially spaced-apart one from the other.
In an embodiment the sparkplugs of the plurality of sparkplugs are arranged along a spiral path extending along at least a portion of the length of the tube.
In an embodiment there is provided a gas exchange valve disposed within a gas exchange port that is defined through a wall of the remote ignition chamber, the gas exchange port defining one end of a gas exchange conduit that fluidly connects an intake manifold of the engine to the remote ignition chamber.
In an embodiment there is further provided an auxiliary compression cylinder fluidly coupled to the remote ignition chamber and fluidly coupled to the intake manifold of the engine, for equalizing pressure in the remote ignition chamber and in the engine cylinder.
In an embodiment both the gas exchange conduit and the auxiliary compression cylinder are fluidly coupled to a region of the intake manifold that is upstream of a main fuel injector of the internal combustion engine.
In accordance with an aspect of at least one embodiment, there is provided an ignition method for an internal combustion engine having an engine cylinder defining a main combustion chamber and having a remote ignition chamber enclosing an ignition source and being in fluid communication with the main combustion chamber via a tubing assembly having a tube, the method comprising: charging the remote ignition chamber and the tube with a first combustible charge gas; charging the main combustion chamber with a second combustible charge gas: using a plurality of high-voltage electrodes arranged along a length of the tube, pretreating the first combustible charge gas to generate radicals therein: using the ignition source, igniting the pretreated first combustible gas to produce a deflagration flame: using a plurality of high-energy discharge sparkplugs arranged along the length of the tube, sensing a property of the deflagration flame: when the sensed property of the deflagration flame is within predetermined threshold limits, providing a transient high energy spark to the deflagration flame using at least one of the high-energy discharge sparkplugs for stimulating deflagration-to-detonation transition.
In an embodiment the first combustible charge gas has a higher chemical reactivity than the second combustible charge gas.
In an embodiment there is a step of heating the tube to a temperature within a predetermined range of temperatures prior to igniting the pretreated first combustible gas.
In an embodiment charging the remote ignition chamber with the first combustible charge gas comprises injecting a fuel into the remote ignition chamber using a first fuel injector.
In an embodiment charging the remote ignition chamber with the first combustible charge gas further comprises injecting a gas comprising molecular oxygen into the remote ignition chamber using a second fuel injector.
In an embodiment the sensed property is a deflagration flame speed determined based on sensed times of arrival of the deflagration flame at at least two sparkplugs of the plurality of high-energy discharge sparkplugs.
In an embodiment charging the remote ignition chamber and the main combustion chamber occur during an intake stroke of the engine, and further comprising closing a valve disposed along a length of the tube after at least partially charging the remote ignition chamber and the tube with the first combustible charge gas, to prevent fluid flow between the tube and the main combustion chamber during a subsequent compression stroke of the engine.
In an embodiment there is a step of opening the valve prior to igniting the pretreated first combustible charge gas.
In an embodiment the first combustible charge gas and the second combustible charge gas have a same composition.
The instant invention will now be described by way of example only, and with reference to the attached drawings, wherein similar reference numerals denote similar elements throughout the several views, and in which:
The following description is presented to enable a person skilled in the art to make and use the invention and is provided in the context of a particular application and its requirements. Various modifications to the disclosed embodiments will be readily apparent to those skilled in the art, and the general principles defined herein may be applied to other embodiments and applications without departing from the scope of the invention. Thus, the present invention is not intended to be limited to the embodiments disclosed but is to be accorded the widest scope consistent with the principles and features disclosed herein.
Throughout the disclosure and in the appended claims, the following terms shall be understood to have the following meanings.
The term “low carbon fuel” is defined as a material that contains carbon, but when burned provides thermal energy with fewer carbon-containing emissions than fossil fuels from a well-to-wheel perspective. Some non-limiting examples include natural gas, propane, and biofuels made from plant waste or algae.
The term “zero-carbon fuel” is defined as a material that does not contain carbon, and therefore when burned provides thermal energy with no carbon-containing emissions. Some non-limiting examples include hydrogen and ammonia.
The term “carbon emissions” is defined as the release of carbon compounds into the atmosphere. Carbon emissions have both natural sources and human-made sources. Herein, carbon emissions will refer specifically to the release of carbon compounds that are produced when a material is burned to provide energy.
The terms “renewable natural gas” and “RNG” are defined as a biogas which has been upgraded to a quality similar to fossil natural gas and has a methane concentration of 90% or greater. Renewable natural gas can be distributed via existing natural gas pipelines.
The term “deflagration” is defined as a mode of combustion in which the propagation speed of the combustion wave-front is subsonic. A deflagration wave propagates via the diffusion of heat and mass from a flame zone to effect ignition in the reactants ahead.
The term “detonation” is defined as a mode of combustion in which the propagation speed of the combustion wave-front is supersonic. A supersonic compression shock wave ignites the mixture ahead by adiabatic heating across the leading shock front. The shock is in turn maintained by the backward expansion of the reacting gases and products relative to the front, thus providing the forward thrust needed to drive the shock.
The term “deflagration-to-detonation” is defined as the transition from the deflagration combustion mode to the detonation combustion mode. Thus, deflagration-to-detonation indicates a change or transition in the mechanism of wave propagation rather than simply in a change of wave speed.
The term “hypersonic speed” is defined as one that exceeds five times the speed of sound.
The terms “flame propagation speed” and “speed of propagation of a flame” are used interchangeably herein to refer to the speed at which a combustion wave front is travelling in both the deflagration combustion mode and in the detonation combustion mode. The speed is measured relative to the tube within which the wave front is travelling.
Previous studies have shown that the speed of propagation of a flame, traveling through a tube, can be accelerated with proper matching of the dimension of the tube and the chemical reactivity (stoichiometry) of the air/fuel mixture being combusted. Under the correct conditions, the flame can be accelerated to supersonic speed and transformed into detonation waves. This process of deflagration-to-detonation transition (DDT) has been investigated for various applications, including pulse detonation engines and power generation. Heretofore, most tube-related detonation research has been performed under vacuum conditions, where atmospheric pressure is considered to be “high pressure.” Under these conditions, it has been observed that the detonation cell size must be 13 times smaller than the inner diameter of the tube to allow a detonation wave to propagate. Therefore, the inner diameter and volume of detonation tubes that have been used in previous studies are large, making them suitable for applications such as generating power as a stand-alone system but unsuitable for use as an ignition source for internal combustion engines.
Embodiments of the invention provide methods and systems that use transient high energy electric discharge, in combination with pretreatment prior to deflagration, to stimulate the deflagration-to-detonation transition. It has been found that high energy electric discharge alone does not provide sufficient ignition energy to cause “direct initiation” of detonation. This problem is solved using a suitable pretreatment strategy prior to deflagration to modulate the reactivity of the air/fuel mixture, which enhances the flame deflagration speed such that an additional amount of ignition energy provided by a high energy electric discharge is sufficient to stimulate deflagration-to-detonation. The timing of the high energy electric discharge release is important. In particular, according to the disclosed embodiments the energy release is timed to occur directly behind the combustion wave front, when the flame speed exceeds a certain threshold, to further accelerate the combustion wave front along the direction of flame propagation. If the energy release occurs ahead of the flame front, then the flame speed will be decreased. On the other hand, if the energy release occurs after the flame front has passed then there is only a limited impact on the flame propagation speed. As will be discussed in more detail below, the timing of high energy electric discharge is determined using the ion sensors located along the flame propagation path, which can promptly calculate flame speed and the position of the flame front, to allow the energy release to be delivered at the right place and at the right time.
Even if the high energy electric discharge occurs at precisely the right time, the status of the flame, or the velocity of the flame, is critical for determining the DDT stimulation requirements. The lower flame speed is below the detonation speed, the higher the energy demand from the high energy electric discharge to initiate a detonation event. Depending on the flame speed, this may be orders or tens of orders of magnitude higher than the energy an electric spark can provide. On the other hand, if the flame speed is already very close to detonation speed, then even a spark would not be necessary to initiate a detonation event. As will be apparent, the pretreatment strategy must produce a flame speed that is high enough such that a relatively small amount of extra energy, provided by the electric discharge, can transition the flame status from the deflagration to the detonation stage.
The systems and methods disclosed herein provide a deterministic and fast ignition process and remote chamber ignition system, which are suitable for use with multiple applications, such as for instance internal combustion engines, gas turbines, etc., including applications in which fuels with low flame velocities are ignited, such as for instance natural gas or ammonia. For natural gas, which is composed mostly of methane, complete combustion is quite challenging because of the low reactivity of the fuel. For ammonia, which is about seven times “lazier” than natural gas, it is even more challenge to achieve complete combustion. For a deflagration flame, the low speed and low flame temperature make it difficult to overcome the low reactivity of the fuels. In contradistinction, detonation produces extremely high flame speeds and temperatures, making it possible to achieve complete or near complete combustion even using relatively low reactivity fuels such as natural gas and ammonia.
Referring still to
Referring now to
The small inside diameter of the tube 200 enhances flame speed acceleration, but a low wall-temperature of the tube 200 can contribute to flame quenching. Accordingly, a temperature-control layer 202 is disposed outwardly of the tube 200 to control the wall temperature of the tube 200, under control of the controller 110. The controlled wall temperature of the tube 200 prevents flame speed deacceleration and flame quenching prior to deflagration-to-detonation transition. During operation, the wall temperature of the tube 200 is maintained below a predetermined value to avoid autoignition of the air/fuel mixture inside the tube 200, which would not be synchronized with spark timing for igniting the air/fuel mixture in the main combustion chamber 104. In one specific example, the temperature of the temperature-control layer 202 is controlled using an electric heating element. In another specific example, the temperature of the temperature-control layer 202 is controlled using engine coolant via a heat exchanger.
Referring still to
A detonation wave demonstrates much stronger ignition capability compared to a deflagration wave, but a prompt deflagration to detonation transition (DDT) is essential. Direct initiation of detonation without DDT process is possible, assuming that the volumetric ignition energy density is sufficient. However, for low reactivity fuels, such as methane and ammonia, the minimum ignition energy is in the MJ range, which is impractical for repeated use in engine applications. The existence of a suitably pre-treated air/fuel mixture before ignition can enhance the flame acceleration along the tube, which significantly reduces the energy demand for detonation initiation, but the timing and energy release profile is critical to achieve a successful DDT transition. Transient electric energy release via capacitive discharge can generate a local thermal explosion in microseconds, but this technique is most efficient within a limited range of flame speeds. Furthermore, if an ignition event is triggered before the arrival of the flame front, the DDT transition will be interrupted. On the other hand, if an ignition event is triggered after the arrival of the flame front, the ignition has only a limited impact on the DDT process.
As will be apparent, in view of the above discussion, the ignition timing should be controlled such that the ignition event is triggered immediately behind the flame front, thereby pushing the flame front along the flame propagation direction within the tube 200. As is shown in
Referring now to the flow diagram that is shown in
The system that has been described above with reference to
Referring now to
Referring still to
The second sparkplug arrangement, which is shown in
Referring again to
Operation of the rotary valve will now be discussed with reference to
Now referring to
The high-voltage electrode assembly 204 begins pretreating the unburned second charge gas inside the tube 200 at time t2 using low-temperature plasma and/or high frequency oscillating electric fields to generate radicals suitable for promoting high speed flame propagation along tube 200. The rotary valve 220 is switched from the closed condition to the open condition during pretreatment, preferably close to the end of the engine compression stroke. After the pretreatment ends at t3, a sparkplug 704 mounted on the remote chamber 102 is used to initiate the combustion process and generates a flame kernel within the second charge gas inside the remote chamber 102. The sparkplug 704 is energized t4 and initiate the spark event at t5.
The flame propagates initially within the remote chamber 102, then exits into the tube 200. At t6 the flame passes the sparkplugs 214A and 214B, which serve both as ion sensors and ignitors. By determining the time it takes for the flame to travel from spark gap 219A to spark gap 219B, it is possible to estimate a local flame speed. If the flame speed falls within a predetermined range that is deemed suitable for detonation stimulation at t7, then at t8 a transient high energy spark is initiated within spark gap 219B of spark plug 214B, directly behind the flame front, to push the flame faster, reaching detonation stage.
The flame eventually passes through the open rotary valve 220 and exits from tube 200 into the main combustion chamber 104, producing a flame front 706 that generates a detonation wave 708 igniting the air/fuel mixture of the first charge gas 710 within the main combustion chamber 104. The ignition energy delivered to the combustion chamber 104 depends on various parameters, including but not limited to i) the size of the remote chamber 102 and ii) the pressure of the air/fuel mixture prior to ignition. Compared with plasma-based ignition techniques, the system 100 can deliver much higher ignition energies into the combustion chamber 104. By way of a specific and non-limiting example, the system 100 may deliver between ˜200 J and ˜400 J of energy. Furthermore, compared to diesel high-pressure direct fuel injection as the ignition source of a dual-fuel natural gas engine, the systems and methods described in accordance with the various embodiments of the instant invention use a pre-mixed combustible mixture, generating zero particulate matter emissions despite the oxygen concentration inside the main combustion chamber 104. The detonation wave increases the combustion efficiency and results in clean combustion.
Referring now to
In the system that is shown in
At the end of the compression stroke in both the first and second modes of operating the system of
Operation of the system that is shown in
The closing times of the engine intake valve 1014 and of the gas exchange valve 1012 should be controlled such that the remote chamber 102 and the tube 200 of the tubing assembly 106 are filled with the fuel-enriched air/fuel mixture, while only a limited amount of fuel-enriched air/fuel mixture flows into the main combustion chamber 102. As will be apparent, in this example the air/fuel ratio within the remote chamber 102 and the tubing assembly 106 is adjusted such that flame propagation is achieved, and in particular the flame is not quenched before it reaches the main combustion chamber 104 and ignites the air/fuel mixture therein.
Referring still to
At the end of the compression stroke, the rotary valve 220 is switched back to the open condition such that the remote chamber 102, the tube 200 of the tubing assembly 106, and the main combustion chamber 104 are in fluid communication with one another. The sparkplug 704 is used to create a flame kernel in the remote chamber 102, and the tubing assembly 106 is used to pre-treat the flame during propagation through the tube 200 and cause DDT. The resulting detonation wave then ignites the air/fuel mixture within the main combustion chamber 104, and the products of the combustion process are removed from the system during the exhaust stroke of the piston 1002.
Operation of the system that is shown in
As is shown in
At the end of the intake stroke or the beginning of the compression stroke of the piston 1002, the rotary valve 220 is switched from the open condition to the closed condition, to prevent the air/fuel mixture in the main combustion chamber 104 from entering the tube 200. The rotary valve 220 ensures that the air/fuel mixture within the remote chamber 102 and the tube 200 is homogeneous and supports an efficient DDT. At the end of the compression stroke, the rotary valve 220 is switched back to the open condition such that the remote chamber 102, the tube 200 of the tubing assembly 106, and the main combustion chamber 104 are in fluid communication with one another. The sparkplug 704 is used to create a flame kernel in the remote chamber 102, and the tubing assembly 106 is used to pre-treat the flame during propagation through the tube 200 and cause DDT. The resulting detonation wave then ignites the air/fuel mixture within the main combustion chamber 104, and the products of the combustion process are removed from the system during the exhaust stroke of the piston 1002.
A second fuel injector 1300 is fluidly coupled to the remote chamber 102 for dynamically adjusting the fuel mixture composition in the remote chamber 102. For instance, the second fuel injector 1300 injects fuel, which may be either the same as or different than the fuel that is fed into the main combustion chamber 104. An additional injector 1502 is also fluidly coupled to the remote chamber 102, and also for use in dynamically adjusting the fuel mixture composition in the remote chamber 102. For instance, the injector 1502 is used to inject air, oxygen enriched air, or pure oxygen into the remote chamber 102. Such an arrangement is advantageous when the engine is operating under lean burn or heavily diluted conditions, in order to avoid flame quenching during flame propagation through the tubing assembly 106.
The second fuel injector 1300 is used e.g., to inject fuel with a chemical reactivity higher than the chemical reactivity of the fuel that is fed into the main combustion chamber 104. The injector 1502 is used to inject air, or oxygen enriched air, or pure oxygen, into the remote chamber 104. In some embodiments, the injector 1502 is connected directly to a high-pressure source (not illustrated in
During the compression stroke of the piston 1002, the two injectors 1300 and 1502 continue to inject fuel and air/oxygen into the remote chamber 102 to balance the pressure between the remote chamber 102 and the main combustion chamber 104, to ensure a reliable and fast DDT process. The precise control of the total flow rate into the remote chamber 102 can be realized via various technical paths, such as for instance model-based control based on engine speed and position of the piston 1002.
Additionally or alternatively, rotary valve 220 is closed during the compression stroke to prevent the in-cylinder charge from flowing into the tubing assembly 106. In that case, at the end of the compression stroke, the rotary valve 220 is switched back to the open condition such that the remote chamber 102, the tube 200 of the tubing assembly 106, and the main combustion chamber 104 are in fluid communication with one another.
The sparkplug 704 is then used to create a flame kernel in the remote chamber 102, and the tubing assembly 106 is used to pre-treat the flame during propagation through the tube 200 and cause DDT. The resulting detonation wave then ignites the air/fuel mixture within the main combustion chamber 104, and the products of the combustion process are removed from the system during the exhaust stroke of the piston 1002.
A second fuel injector 1300 is fluidly coupled to the remote chamber 102 for dynamically adjusting the fuel mixture composition in the remote chamber 102. For instance, the second fuel injector 1300 injects fuel, which may be either the same as or different than fuel that is fed into the main combustion chamber 104. An additional injector 1502 is also fluidly coupled to the remote chamber 102, also for use in dynamically adjusting the fuel mixture composition in the remote chamber 102. For instance, the injector 1502 is used to inject air, or oxygen enriched air, or pure oxygen into the remote chamber 102. Such an arrangement is advantageous when the engine is operating under lean burn or heavily diluted conditions, in order to avoid flame quenching during flame propagation through the tubing assembly 106.
The engine depicted in
Now referring to
Near the end of the intake stroke or the beginning of the compression stroke, the rotary valve 220 is closed to prevent the first combustible charge gas from the main combustion chamber 104 from mixing with the second combustible charge gas in the tube 200 of the tubing assembly 106. Gas exchange valve 1012 also closes to prevent the second combustible charge gas from flowing out of the remote chamber 102 and into the intake manifold 1010. Prior to the end of the compression stroke, the rotary valve 220 opens again (as shown in
The rotary valve 220 remains open during the expansion stroke and the exhaust stroke (as shown in
Finally, during the exhaust stroke valve 1606 in the intake port of auxiliary compression cylinder 1600 is closed whilst the valve 1608 in the remote chamber 102 is opened. Compressed air from the auxiliary compression cylinder 1600 flows into remote chamber 102 and then through the tubing assembly 106 into the main combustion chamber 104, where it is then expelled via the opened exhaust valve 1016.
As used herein, including in the claims, unless the context indicates otherwise, singular forms of the terms herein are to be construed as including the plural form and vice versa. For instance, unless the context indicates otherwise, a singular reference, such as “a” or “an” means “one or more”.
Throughout the description and claims of this specification, the words “comprise”, “including”, “having” and “contain” and variations of the words, for example “comprising” and “comprises” etc., mean “including but not limited to”, and are not intended to (and do not) exclude other components.
It will be appreciated that variations to the foregoing embodiments of the invention can be made while still falling within the scope of the invention. Each feature disclosed in this specification, unless stated otherwise, may be replaced by alternative features serving the same, equivalent or similar purpose. Thus, unless stated otherwise, each feature disclosed is one example only of a generic series of equivalent or similar features.
The use of any and all examples, or exemplary language (“for instance”, “such as”, “for example”, “e.g.” and like language) provided herein, is intended merely to better illustrate the invention and does not indicate a limitation on the scope of the invention unless otherwise claimed. No language in the specification should be construed as indicating any non-claimed element as essential to the practice of the invention.
Any steps described in this specification may be performed in any order or simultaneously unless stated or the context requires otherwise.
All of the features disclosed in this specification may be combined in any combination, except combinations where at least some of such features and/or steps are mutually exclusive. In particular, the preferred features of the invention are applicable to all aspects of the invention and may be used in any combination. Likewise, features described in non-essential combinations may be used separately (not in combination).
Number | Name | Date | Kind |
---|---|---|---|
5855827 | Bussing et al. | Jan 1999 | A |
6062018 | Bussing | May 2000 | A |
7669405 | Pinard | Mar 2010 | B2 |
7758334 | Shimo | Jul 2010 | B2 |
8650856 | Brumberg | Feb 2014 | B2 |
10337397 | Shelby et al. | Jul 2019 | B2 |
11661885 | Zhou | May 2023 | B2 |
20030182927 | Leyva | Oct 2003 | A1 |
20070137172 | Rasheed | Jun 2007 | A1 |
20080229756 | Pinard | Sep 2008 | A1 |
20090320439 | Chapin | Dec 2009 | A1 |
20110005420 | Fullerton | Jan 2011 | A1 |
20110047962 | Kenyon | Mar 2011 | A1 |
20130025256 | Lu | Jan 2013 | A1 |
20130139486 | Kenyon | Jun 2013 | A1 |
20130139487 | Kenyon | Jun 2013 | A1 |
20200070961 | Rathay | Mar 2020 | A1 |
20200072174 | Rathay | Mar 2020 | A1 |
20200378605 | Lacoste | Dec 2020 | A1 |
20230040984 | Zhou | Feb 2023 | A1 |
Number | Date | Country |
---|---|---|
4729947 | Jul 2011 | JP |
Entry |
---|
Biswas et al., Numerical Investigation of Ignition of Ultra-Lean Premixed H2/Air Mixtures by Pre-Chamber Supersonic Hot Jet, SAE Int. J. Engines / vol. 10, Issue 5, Dec. 2017, pp. 1-17. |