The present invention pertains to methods and apparatus for igniting a gas flow. More particularly, one preferred embodiment of the invention comprises a two-stage ignition method for creating a flow of elevated temperature combustion product using bipropellants. The present invention includes a number of methods for ignition and re-ignition of propellants for a broad range of ground and flight applications including rocket engines, reaction control system thrusters, rocket turbomachinery gas generators, propellant conditioning systems and pressurization heaters.
The current art of ignition methods for creating a flow of elevated temperature combustion product using bipropellants (oxidizer and a fuel) all employ a single “stage.” The term “stage” refers to a series of uninterrupted, sequential events, including introducing propellants into a chamber or area and igniting the mixture, and in some cases, including propagating the combustion product through various means to ignite other propellants to produce an ignition combustion product such as a torch. Conventional single stage ignition methods create a final combustion product using bipropellants in a relatively short period of time through a series of precise, time-synchronized events such as opening propellant valves, allowing the flows to pre-mix in a chamber, and then introducing a spark to this mixture at a certain specific time lag from the initial valve openings. Interrupting this series of precise, time-synchronized events with a significant time lag generally leads to failure of the method to produce its final elevated temperature combustion product.
An ignition system is required for liquid bipropellant rocket engines that do not use hypergolic propellants (hypergolic propellants ignite spontaneously upon contact with each other). Proper engine combustion chamber ignition for liquid bipropellant rockets is crucial to the success of a space launch mission. Failed ignition in flight can leave a payload in a useless orbit or even cause a catastrophic loss of the payload. Rocket engine ignition (and re-ignition for restartable engines) has historically been a significant source of unreliability for space launch vehicles, and the main cause of a number of mission failures. Among others, in-flight Ariane rocket mission failures occurred due to third stage HM-7B rocket engine ignition failure on 12 Sep. 1985 for an Ariane 3 and on 31 May 1986 for an Ariane 2.1 Similarly, two launches of Japan's LS-4 rocket in the mid-1960s, and a series of launches of the Russian LV Molniya launch vehicle in the 1960s all failed due to upper stage engine ignition failures. Engine ignition failure has also been blamed for costly launch vehicle aborts on the launch pad such as for a 28 Jan. 1999 Delta II launch attempt which was aborted due to first stage vernier engine ignition failure. Failed ignition on the launch pad can also possibly result in unburned engine fuel and oxidizer expelled from the rocket engine onto the launch pad which could, in-turn, cause an explosion.
Most modern liquid bipropellant rocket engines used for space launch employ either a spark-torch igniter (e.g. the Space Shuttle Main Engine, RL-10, and J-2) or a pyrophoric (hypergolic) igniter (e.g. RD-180, F-1). Pyrotechnic and pyrogen igniters contain explosive materials and are commonly used in solid rocket motors but not in liquid bipropellant rocket engines.
The start-up of rocket engines, including initiation of combustion, is a complex, dynamic process that challenges rocket engine designers due to the possible presence of combustion instabilities and vibrations that can cause operational inefficiencies, structural damage, or even catastrophic engine failure. Combustion instabilities derive from specific combinations of rocket combustion chamber, injector, igniter, and propellant feed geometries and operational dynamic interactions. One such instability is a hard start, caused when too much propellant enters the combustion chamber prior to ignition and the resultant rate of build-up of combusted gasses results in an excessive pressure spike. Another instability example is combustion vibration sometimes caused when combustion chamber pressure rises too slowly due to a temporary too low injector pressure drop during thrust build-up. Rocket engines thus typically have very exact start-up timing sequencing—often to within milliseconds—to ensure the occurrence and magnitude of such instabilities are minimized. Further, propellant flows that are too strong can quench the ignition spark or flame. In current art rocket ignition systems, the ignition method is a critical part of this sequencing.
Spark-torch igniters typically burn a bipropellant mixture obtained from the main engine feeds although some utilize a separate propellant supply. Spark-torch igniter systems require significant development and integration into the overall engine system to ensure ignition occurs at the precise time synchronized with other engine processes such as propellant flow into the combustion chamber. Timing errors as short as a few tens of milliseconds can potentially cause hard starts or even engine failures. Spark-torch igniter systems also require high voltage electrical components which may need special handling and shielding, especially in a vacuum or space environment. The performance of some spark-torch igniter systems is sensitive to oxidizer-to-fuel mixture ratio, flow rates, excitation voltage, and spark rate, making the system relatively complex.
Catalytic-torch igniters have been studied extensively and successfully applied to ground systems but have had only limited application to date on rockets.
Combustion wave ignition systems are sometimes used in large segmented or compartmentalized rocket engines that require propellant ignition in several combustion chambers at the same time. Such systems use a spark igniter to combust premixed propellants in a specially designed chamber that creates a combustion wave which propagates very rapidly through connected, propellant-filled manifolds to reach all of the combustion chambers or possibly individual torches for each combustion chamber. Combustion wave igniters use a single stage ignition method in that the final combustion product—a flame to enter a rocket combustion chamber—is produced by a single series of uninterrupted, sequential events, propagating from the initial combustion.
Pyrophoric or hypergolic igniters inject a chemical into a rocket engine's combustion chamber along with the propellants. The chemical, often triethylaluminium (EADS 300N cryogenic rocket engine) or a mixture of triethylborane and triethylaluminium (e.g., F-1), ignites spontaneously with the oxidizer and burns at a very high temperature. These chemicals are highly corrosive, toxic, and ignite spontaneously on contact with air, and are thus expensive and risky to use.
Until now, all ignition systems used to ignite liquid bipropellant rocket engines have used a single stage. Such systems create a flow of elevated temperature combustion product by a single ignition event, such as a spark-induced, catalytic-induced, or compression wave-produced ignition of propellants, or a series of dependent, time-synchronized events, such as igniting a mixture that propagates directly to light one or more torches that feed into rocket engine combustion chambers. Single stage ignition methods generally employ relatively high propellant mass flow rates (usually 0.1 to 1.0% of the main engine's propellant total flow rate) to ensure proper rocket engine combustion chamber ignition. These relatively high flow rates generally result in high temperature igniter flows which, combined with the proximity of many embodied detection devices to the very hot rocket engine combustion chamber, tend to reduce lifetime and reliability of devices used to detect successful igniter operation.
To date, rocket engine reusability has been minimal beyond that of a few restarts in a single mission. However, USAF and NASA have invested heavily in research and development of reusable or partially reusable launch vehicles. Such vehicles will require rocket engine ignition systems with improved reusability, reliability, and longer operational life.
As implied above, detection of successful operation of the igniter before committing high pressure main rocket engine propellants to the combustion chamber is important. In an attempt to lower the risk of ignition system failure, safety interlocks are sometimes used to override main propellant valves if the ignition source is not operating properly. However, the reliability of the safety interlocks has been less than ideal and accurate, reliable detection of proper ignition system operation is challenging. One detection procedure is to use thin wires stretched over the path of the ignition torch or engine nozzle which provide a positive ignition operation signal when the wires are burned through. However, this method can be compromised by wire breakage caused by wind or incomplete burn-through of the wires due to improper placement. Pressure sensors, thermocouple sensors, and cameras to detect electromagnetic spectra such as infrared are also sometimes used, but these methods have not been generally highly reliable due to the very challenging environment (very high acoustic, acceleration, and thermal loads) in the vicinity of a rocket's engine. Further, rocket engine ignition systems are generally uniquely designed, developed, and fabricated to their particular application and thus generally very unique and are not reused among various rocket subsystems, even though they share common functional needs (e.g., rocket engine ignition, reaction control system ignition, propellant conditioning system ignition, etc.) Due to this uniqueness and very small economies of scale, rocket engine ignition systems have high non-recurring development and recurring hardware costs.
Conventional single stage ignition devices are limited by their single stage design. The development of an ignition system for bipropellant applications with improved reliability, longer operational life, greater operational flexibility, lower cost through design simplicity, and reduced complexity would constitute a major technological advance, and would satisfy long felt needs and aspirations in the aerospace industry.
The invention comprises methods and apparatus for a two-stage ignition method for creating a flow of elevated temperature combustion product using bipropellants. While this elevated temperature combustion product may be used for a broad range of ground and flight applications, rocket systems form a set of important applications. The final combustion product can be integrated into and used for rocket engine ignition, for rocket turbomachinery, propellant conditioning, or pressurization systems, or expanded through a nozzle to provide thrust for a small rocket, as for a reaction control system.
In one embodiment, the invention comprises a two-stage ignition method for creating a flow of elevated temperature combustion product. Instead of only a single stage employing a relatively high propellant mass flow rate as with the conventional ignition system, the present invention adds a preliminary stage, or “pilot stage,” which employs a relatively low propellant mass flow rate. The pilot stage produces a combustion product through ignition of bipropellants, that is then used to ignite propellants in the main combustion stage. The pilot stage can be operated alone, independent of the main combustion stage. The main combustion stage can be switched on and off, or pulsed, depending upon need.
The relatively benign heating environment of this pilot stage compared to the main combustion stage (and thus current art torch igniter systems) reduces stress on the igniter improving overall ignition system reliability and increasing operational life. This seclusion of the igniter to the pilot stage likewise allows for the elevated temperature combustion product resulting from the main combustion stage to use higher propellant flows and have higher temperatures than most current art systems. This serves to allow the elevated temperature combustion product to be used for a variety of applications for which a current art ignition system would be inadequate.
The present invention enables the same design to be used for multiple uses in different rocket systems or subsystems that need a flow of elevated temperature combustion product, lowering non-recurring development costs, increasing production economies of scale and thus lowering recurring hardware acquisition costs. These different rocket systems include, but are not limited to, main rocket engine torch ignition, propellant conditioning heaters, turbomachinery preburners, and small rocket engines, such as reaction control system thrusters.
An appreciation of the other aims and objectives of the present invention, and a more complete and comprehensive understanding of this invention, may be obtained by studying the following description of preferred and alternative embodiments, and by referring to the accompanying drawings.
One embodiment of the present invention comprises a two-stage ignition method for creating a flow of elevated temperature combustion product using bipropellants. In one particular embodiment, the invention utilizes two different ignition stages, a “pilot stage,” which ignites relatively low mass flow rates of bipropellants to create a pilot flame, and a “main combustion stage,” which utilizes the pilot flame to ignite relatively high mass flow rates of bipropellants to produce a flow of elevated temperature combustion product.
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Main streams of methane and oxygen 60 & 62 are introduced into the third and fourth ports 53, and flow into the igniter combustion chamber 64. These streams are ignited by the pilot flame 22. The main streams of methane and oxygen 60 & 62 are supplied at relatively high mass flow rates compared to the relatively low mass flow rates 18 & 20 which feed the pilot stage 16. A final elevated temperature combustion product 30 is formed within the igniter combustion chamber 64, and propagates out of the igniter at the terminal end of the igniter body 40 through an igniter exit/injector interface 70, which may also function as a generalized nozzle.
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In one embodiment of the invention, the igniter body is manufactured from metal. The metal machining and fabrication processes which may be employed to build the igniter body are generally well known in the art.
The pilot stage consists of a means of introducing separate, controlled, relatively low mass flow rate, flows of oxidizer and fuel into a mixing chamber to produce a controlled oxidizer-to-fuel mixture ratio of propellant which then flows into a pilot combustion chamber containing an ignition source. The propellant is then ignited with an electrically-produced spark, a chemical reaction due to contact with a catalytic reactor, a laser or by other suitable means, producing a relatively small, continuous combustion product called the pilot flame. In some embodiments for certain propellant and ignition source combinations, the mixture is regulated to be fuel-rich (low oxidizer-to-fuel mixture ratio) to reduce temperatures in the pilot stage. The pilot flame propagates from the pilot combustion chamber into a main combustion chamber. In some embodiments using certain propellants, an additional “bypass” flow of oxidizer at a relatively low mass flow rate is introduced either into the pilot combustion chamber or into an intermediate bypass combustion chamber between the pilot combustion chamber and the main combustion chamber, serving to increase the oxidizer-to-fuel mixture ratio and strengthen the pilot flame.
The main combustion stage consists of a means of introducing separate, controlled, relatively high mass flow rate, flows of oxidizer and fuel at a controlled oxidizer-to-fuel mixture ratio into the main combustion chamber, whereupon the propellants are ignited by the pilot flame to form a final, combined, relatively large, elevated temperature combustion product which is expelled from the main combustion chamber through an exit orifice. The oxidizer could be cryogenic liquid or gaseous oxygen, or a myriad of other oxidizing propellants. The fuel could be kerosene or kerosene-based rocket fuel, cryogenic liquid or gaseous hydrogen, cryogenic liquid or gaseous methane, or a myriad of other fuel propellants.
For embodiments concerning rocket applications, the propellants may be obtained either directly from the main propellants tanks or from independent tank sources. The ignition source may be an electrical spark exciter, a laser, a catalyst device, or other ignition source. The catalyst device may be a bed, metal sleeve, wire, or mesh composed of or containing a catalyst. Depending on the propellants selected for use in this method, the catalyst device may be pre-heated by any one of a variety of means including electrical resistance heating.
The pilot stage may be used continuously as a pilot light to produce its relatively low flow rate, self-sustaining, high-temperature gas stream suitable for ignition of the propellants introduced into the main chamber, or switched on and off as needed. The main combustion stage may be operated in either a steady state (on or off) or pulsed mode, enabling a single physical embodiment device of this method to serve multiple applications.
The method of the present invention may incorporate one or more thermocouple and/or pressure transducer sensors and associated electrical circuits to directly or indirectly verify the pilot flame and/or final elevated temperature combustion product are operational. The thermocouple and pressure transducer sensors and associated electrical circuits may be used as part of a safety interlock between an embodiment of this method and its application to an external system, such as the case of a safety interlock used to confirm proper rocket engine igniter operation before initiating propellant flows into the rocket engine combustion chamber.
The final combustion product may be used directly or indirectly for many purposes, including, but not limited to, thrust generation (e.g., reaction control system for a rocket, satellite, or spacecraft), heat generation (e.g., to create warmed inert gas as part of a pressurization system), or as a means to initiate combustion in a broader process (e.g., torch igniter for ignition of propellants in a rocket engine main combustion chamber or in a rocket turbopump preburner.)
The exit orifice (and exterior of the apparatus) is generally uniquely fashioned to serve an appropriate function and as an appropriate interface to other fixtures depending upon its particular application. For example, when the elevated temperature combustion product produced by the method is used for thrust generation for a reaction control system, the exit orifice (and exterior of the apparatus) serves as a throat and interface to an attached nozzle.
One embodiment of the method of the present invention is for a single design fulfilling the dual application of a rocket engine torch igniter and rocket reaction control system thruster. This embodiment uses a heterogeneous Group VIII metal catalyst (Platinum, Rhodium, Palladium, etc.) as the ignition source for the pilot stage. In this embodiment of this method, first the catalyst is pre-heated by electrical resistance heating. The relatively low flow rate oxidizer and fuel flows are then individually modulated and pre-mixed in a small mixing chamber using a fuel-rich mixture, after which they flow through a flame arresting screen or device, and then over the hot catalyst bed. A relatively low oxidizer-to-fuel (fuel-rich) mixture ratio is used to keep combustion temperatures within the pilot stage at moderate levels to increase device durability and operational lifetime. The hot catalytic bed activates oxidizer molecular dissociation at the catalyst bed surface and enables a catalytic reaction that automatically promotes self-sustaining combustion. In this embodiment, an oxidizer bypass between the propellant feedlines for the main combustion stage and the pilot stage injects a relative low mass flow rate of bypass oxidizer downstream of the catalyst bed. This additional oxidizer mixes with the hot fuel-rich gases from the catalyst bed and spontaneously ignites to a diffuse pilot flame in the pilot combustion chamber, serving to increase the oxidizer-to-fuel mixture ratio and create a more energetic, diffuse pilot combustion jet which propagates into the main combustion chamber. The catalyst heater is then turned off and relatively high flow rates of additional fuel and oxidizer are injected into the main combustion chamber through the main oxidizer and fuel feedlines and are ignited by the pilot flame. The final, combined, elevated temperature, combustion product is expelled from the main combustion chamber through an exit orifice. For the reaction control system thruster application of this embodiment, the main combustion chamber exit orifice is the throat of the reaction control thruster nozzle and the surface around the orifice is designed to be attached to the reaction control thruster nozzle. For the reaction control system thruster application of this embodiment, the pilot flame is maintained continuously on by maintaining the low mass flow rate propellant flows during the entire flight phase while the high flow rate main combustion stage is switched on and off to produce thrust as needed. For the rocket engine torch igniter application of this embodiment, the main combustion chamber exit orifice is a nozzle interface into the rocket engine's injector, and the elevated temperature combustion product serves as a torch to ignite the rocket engine propellants. For the rocket engine torch igniter application of this embodiment, both the pilot and main combustion stages may remain continuously on during the entire flight phase, and thermocouple and pressure transducer sensors may be used to verify pilot flame is operational before flowing main rocket engine propellants into the rocket engine combustion chamber.
Although the present invention has been described in detail with reference to one or more preferred embodiments, persons possessing ordinary skill in the art to which this invention pertains will appreciate that various modifications and enhancements may be made without departing from the spirit and scope of the Claims that follow. The various alternatives for providing an Two-Stage Ignition System that have been disclosed above are intended to educate the reader about preferred embodiments of the invention, and are not intended to constrain the limits of the invention or the scope of Claims.
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10b
The Present Non-Provisional patent application is related to Pending Provisional Patent Application Ser. No. 60/907,084, filed on 19 Mar. 2007, entitled Catalytic Combustion Device for Space Vehicle Applications. The Applicants hereby claim the benefit of priority under 35 U.S.C. Sections 119 or 120 for any subject matter which is commonly disclosed in the Present Non-Provisional patent application and Pending Provisional Patent Application Ser. No. 60/907,084.
The Applicants developed some of the Inventions described in the Present Non-Provisional Patent Application under a Contract with NASA Glenn Research Center, Contract No. NNC06CB27C.
Number | Date | Country | |
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60907084 | Mar 2007 | US |