1. Field of the Invention
This application relates generally to engines and power generation systems that use high viscosity, high auto ignition temperature liquid fuels for generating power and heat. More particularly, it relates to an open cycle air engine where regenerative heating is used to preheat and vaporize glycerin, and where the combustion inlet air is also preheated by the afterburning power generation cycle, so that it the glycerin fuel may be cleanly and completely combusted to provide heat energy to operate the engine.
2. Description of Prior Art
Glycerin, C3H5(OH)3, is also known by other names including glycerol; glycerine; and 1,2,3-Propanetriol. It is widely used in industry for applications such as paints, antifreeze, pharmaceuticals, and cosmetics. Typically, glycerin has been manufactured as a byproduct of soap or from processing propylene. However, recently, very large quantities of glycerin have become available as a byproduct of the production of biodiesel fuel. The biodiesel production process generates a gallon of glycerin for approximately every 10 gallons of biodiesel. As biodiesel production has grown, the glycerin market has become saturated. Instead of receiving the anticipated revenue from selling the glycerin byproduct to chemical companies, biodiesel manufacturers are now having to pay for disposal of what has become an unwanted waste product.
Ideally, the waste glycerin could be combusted to produce heat for the biodiesel production process, making it a self fueling process; much like 19th century whaling ships burned waste portions of whales as they rendered blubber for oil. Unfortunately, glycerin is very difficult to burn for three reasons: First, it has a high viscosity and that makes it difficult to inject into a combustion process. Second, it has a high auto ignition temperature (393 C. or 739 F.) that makes ignition difficult to initiate and sustain. Finally, it begins to decompose to form toxic acrolein at temperatures above 150 C. or 302 F. For these reasons, the biodiesel industry does not currently use glycerin to fuel its process.
The following table illustrates the key property differences between gasoline and glycerin that make glycerin combustion difficult. Glycerin's viscosity is orders
of magnitude larger than gasoline, making it much more difficult to effectively force through injectors and nozzles. Glycerin requires significantly higher temperatures and energies to vaporize and auto ignite while releasing much lower specific energy from the combustion process.
The difficulties of glycerin combustion have similarly made it unsuitable for an engine fuel. It cannot be burned in an internal combustion engine and has previously been impractical for fueling turbine engines.
Nevertheless, the prior-art contains several means for combusting glycerin and similar high viscosity, high auto ignition temperature fuels.
U.S. Pat. No. 4,188,782 (“Fuel Vaporizing Combustor Tube”, Smith et al., 1980) and U.S. Pat. No. 4,242,863 (“Dual Fuel Vaporizing Combustor”, Baily, 1981) teach methods for combusting high viscosity fuels by vaporizing, or partially vaporizing, the fuel with preheated air and then impinging the fuel/air mix onto a hot surface plate located in the combustion zone.
U.S. Pat. No. 4,838,029 (Externally Vaporizing System for Turbine Combustor”, Gleason, deceased et al., 1989) teaches a gas turbine combustor where compressor bleed air is mixed with fuel in an auxiliary burner to generate “very hot, nearly-inert gases for vaporizing the main fuel supply” and then injecting the combined hot gases and vaporized fuel into the combustion chamber where it mixes with additional air to complete the combustion.
A promising prior-art is contained in US 2008/0305445 A1 (“Process for Combustion of High Viscosity Low Heating Value Liquid Fuels”, Roberts et al. 2008). Roberts teaches preheating the glycerin to reduce its viscosity and then atomizing it with high pressure (190 psig) air.
The prior-art methods for combusting glycerin typically are based on a process of preheating the liquid fuel to reduce viscosity and then mixing the preheated fuel with air or combustion products to further atomize or vaporize the fuel for complete combustion. All these methods require fairly complex and expensive burners. In addition, Gleason's and Roberts' methods require a source of high pressure air.
A much simpler means of combusting glycerin and similar fuels is possible for the specific case where the fuel is intended for use in an Indirectly Fired Gas Turbine (IFGT) or Afterburning, Recuperated, Positive Displacement (ARPD) engine (U.S. Pat. No. 7,028,476B2 “Afterburning, Recuperated, Positive Displacement Engine”, Proeschel, 2006).
Both the IFGT and ARPD engines operate as shown in
The primary aim of the glycerin combustion process for afterburner fired powerplants is to overcome the disadvantages of the prior art by using the unique configuration of the IFGT and ARPD family of engines to provide an integrated system to completely and cleanly combust glycerin or similar fuels to achieve an economical and efficient means of producing electric and/or mechanical power.
It is an object that the Glycerin Combustion Process for Afterburner Fired Powerplants utilize the waste heat in the exhaust of an IFGT or ARPD power generation unit, to the maximum extent possible, to preheat glycerin or a similar fuel to lower its viscosity while also recovering exhaust heat to increase the enthalpy of the liquid fuel.
It is a further object that the glycerin or similar fuel utilize regenerative heating so it is completely vaporized and superheated above the auto ignition temperature of the fuel air mix prior to entering the burner.
It is also an object that, under steady state operation, the air entering the burner also be above the auto ignition temperature of the fuel air mix.
It is, therefore, a primary object that fuel and air enter the burner in high temperature vapor and gaseous states respectively so that they auto ignite hypergolicly when mixed.
It is a key object that the resulting combustion take place completely, cleanly, efficiently, and safely.
It is an object that the process be capable of automatic control.
It is also an object that the powerplant be applicable to both indirectly fired gas turbine (IFGT) and Afterburning, Recuperated, Positive Displacement (ARPD) power generation units.
It is another object that the process be simple, allow easy maintenance, and be capable of being performed with low cost components.
A Glycerin Combustion Process for Afterburner Fired Powerplants has been devised to implement the stated objects of the invention. The process takes advantage of the ease in which fuel can be regeneratively heated in afterburner fired IFGT and ARPD powerplants. In these powerplants, hot combustion gases exit the burner at a temperature of approximately 815 C. or 1500 F. The hot gases then pass through an air heater (a counterflow heat exchanger) where heat is transferred to the compressed air in the engine cycle. After the combustion gases leave the air heater they are still at a temperature of about 227 C. or 440 F.
The glycerin combustion process causes glycerin to pass through a liquid to gas heat exchanger downstream of the air heater so that the glycerin is heated to a temperature approaching the 227 C. exhaust temperature. That part of the process allows otherwise waste heat to be used to preheat the glycerin, significantly reducing its viscosity. The glycerin then flows through a vaporizer that is located downstream of the flame in the burner. The vaporizer heats the glycerin to the 290 C./554 F. vaporization temperature and then continues to heat it until it is fully vaporized and slightly above the auto ignition temperature of 393 C./740 F. The hot glycerin vapor is then injected into the burner where it mixes with hot air from the engine and is auto ignited.
A better understanding of the invention may be gained by reference to the following Detailed Description in conjunction with the drawings provided in which:
Prior Art Components
Novel Modifications
Air Flow Process
Air enters the Power Generation Unit 1 through the compressor 1A where it is compressed to approximately 4 atmospheres absolute pressure. The compressed air exits the compressor through the Air Heater High Pressure Cold Air Inlet Tube 2A and then passes into the Air Heater 2.
The compressed air travels through the flow passages inside the Air Heater 2, in counterflow to the hot combustion gases, and is heated to approximately 790 C./1470 F. The now hot compressed leaves the Air Heater through the High Pressure Hot Air Outlet Tube 2B.
The hot compressed air expands in the Expander 1B portion of the Power Generation Unit. The expansion process extracts power from the air and that power is used to drive the Compressor and also to provide useful electrical or mechanical power through an Alternator or Power Takeoff 1C.
After expansion, the air is at a pressure just slightly above atmospheric but still at a very warm temperature of approximately 490 C./900 F. The air leaves the Expander via the Expander Exhaust Tube 1D and flows into the Burner 3.
Because the air from the Power Generation Unit is above the auto ignition temperature of glycerin, 393 C./740 F., when it is used as blast air in the Burner, it allows glycerin, or similar fuel, to be cleanly and completely combusted without the concern for the fuel becoming cooled below the ignition point, and thus extinguishing combustion. After firing, the hot combustion products enter the Air Heater 2 through the Low Pressure Hot Combustion Product Inlet Tube 2C at a typical temperature of 815 C./1500 F. The combustion products transfer heat to the incoming high pressure air and, by doing so, are cooled to approximately 227 C./440 F. when they leave the Air Heater through the Exhaust Tube 2D.
Fuel Flow Process
The fuel flow process has the objective of converting ambient temperature liquid glycerin, or similar fuel, to a superheated vapor at a temperature above the fuel's auto ignition temperature.
As shown in
The metered fuel from the Fuel Control Valve enters the Fuel Heater Circuit 5 through the Pre-Heater Inlet Tube 5A. From there the fuel passes through the Fuel Pre-Heater 5B. The Fuel Pre-Heater is a liquid to gas heat exchanger that allows the otherwise wasted heat in the Exhaust Tube 2D to be recovered to pre-heat the fuel. This pre-heating part of the process greatly reduces the fuel viscosity and allows it to pass more easily through the rest of the Fuel Heater Circuit. However, the gas in the Exhaust Tube is not hot enough to obtain the objective of converting the fuel to a vapor at a temperature greater than the auto ignition temperature. Therefore, additional heating is required in a hotter location.
The necessary additional heating is available after the fuel flows through the Pre-Heater Outlet Tube 5C to the Vaporizer 5D. As also shown in
The hot vapor is conveyed to the Burner 3 through the Vaporizer Outlet Tube 5E and into the Fuel Gas Inlet Tube 3C. The preferred configuration of the Burner is shown. With this process the Burner is a gas fuel/air burner where the vaporized fuel is injected into the flame through a Nozzle 3B. The main air flow enters the Burner through the Expander Exhaust Tube 1D. The flame is shielded from the high air flow by a Flame Holder 3A. The Flame Holder allows the air to mix in eddy currents that anchor the flame and also limit the air flow to the flame zone to assure a proper air/fuel ratio in the flame. Afterburner fired IFGT and ARPD engines have a high overall air/fuel ratio. Therefore most of the air bypasses the flame zone. The near stoichiometric flame combustion gases mix with the main air flow downstream of the initial flame. In this manner, the combustion is staged so that initial combustion is slightly richer than stoichiometric and then additional air is added to completely combust the mixture, avoid excess NOx production, minimize unfavorable combustion products such as acrolein and aldehydes, and to achieve the design burner exit temperature of about 815 C./1500 F.
In an alternative to the preferred configuration of the burner, a plurality of burner nozzles and flame holders may be utilized to better optimize the combustion process (
Operation
Under steady state conditions the Glycerin Combustion Process for Afterburner Fired Powerplants is completely regenerative. Both the combustion air and vaporized fuel are indirectly pre-heated by the heat from the flame prior to entering the Burner. Therefore, although the process is self sustaining once started, it cannot start by itself. Consequently, the Start System 6 shown in
Fuel for starting is an easily combusted fuel such as propane or natural gas provided by a regulated Start Fuel Supply 6A. Air for starting is provided by a Start Blower 6B. The Burner is lit by opening the Start Valve 6C and turning on the Start Blower to begin air flow. Next, the Ignitor 6D, a sparking or glowing device, is started to provide an ignition source. Fuel is then provided by the Start Fuel Supply and the flame is initiated. The Ignitor can then be turned off. Once the Air Heater 2 reaches operating temperature, the powerplant is turned over by a start motor (not shown) or by motoring the Alternator or Power Takeoff 1C. The engine will then begin to run, although still fueled from the Start Fuel Supply. As the engine reaches operating speed, the Start Valve is closed and the Start Blower is turned off. Then, when the Pre-Heater 5B, and the Vaporizer 5D reach operating temperatures, the primary fuel is started through the Fuel Control Valve 4E, the Start Fuel Supply is stopped and the powerplant operates in steady state.
Powerplant control consists of matching the powerplant power output to the load demand while also maintaining the proper air/fuel mixtures.
Load matching control varies with the type of power generation unit. IFGT powerplants typically have limited capability for load following. Consequently IFGT's are normally operated at full design power. When the local demand is less than the power generation rate the excess power is stored in batteries, other storage devices, or by putting power on the grid. Afterburning, Recuperated, Positive Displacement (ARPD) engines can control the air flow through the power generation unit to provide a larger capability for load following. Powerplants using ARPD power generation units thus have more flexibility in load following.
With either type of power generation unit, air/fuel mixture control is accomplished by using the Fuel Control Valve 4E to match the air flow.
The Glycerin Combustion Process for Afterburner Fired Powerplants meets the objective of providing an extremely simple, reliable, efficient and safe method for obtaining mechanical and/or electrical power by regeneratively combusting otherwise difficult to burn fuels such as glycerin. Obviously, within the purview of the invention here disclosed, many hardware modifications and variations are possible. These include a wide variety of Air Heaters, Fuel Heaters, and Burners. It is also clear that there are numerous methods for implementing the process using a mix of new and existing components and parts. It is therefore understood that, within the scope of the appended claims and their legal equivalents, the invention may be practiced otherwise than as specifically described.
This application claims the benefit of provisional patent application U.S. 61/244,546 filed 22 Sep. 2009 by the present inventor.
Number | Name | Date | Kind |
---|---|---|---|
158315 | Robinson | Dec 1874 | A |
391018 | Budd | Oct 1888 | A |
397745 | Neilson et al. | Feb 1889 | A |
457801 | Sturtevant et al. | Aug 1891 | A |
1500376 | Delaney | Jul 1924 | A |
1672997 | Benjamin | Jun 1928 | A |
2225310 | Lindhagen et al. | Dec 1940 | A |
2298663 | Traupel | Oct 1942 | A |
2359108 | Hoskins | Sep 1944 | A |
2483045 | Harby | Sep 1949 | A |
2648950 | Miller | Aug 1953 | A |
2655788 | Sedille | Oct 1953 | A |
2677236 | Grinsted | May 1954 | A |
2692477 | Toogood | Oct 1954 | A |
2735265 | Eastman | Feb 1956 | A |
2949010 | Cederquist | Aug 1960 | A |
2958189 | Britton et al. | Nov 1960 | A |
3002347 | Sprague | Oct 1961 | A |
3057153 | Rocchini et al. | Oct 1962 | A |
3078663 | Rocchini et al. | Feb 1963 | A |
3078665 | Trautman et al. | Feb 1963 | A |
3115852 | Robertson | Dec 1963 | A |
3134228 | Wolansky et al. | May 1964 | A |
3203175 | Ladislav et al. | Aug 1965 | A |
3440821 | Waltz | Apr 1969 | A |
3656872 | Jubb | Apr 1972 | A |
3718424 | Konagai | Feb 1973 | A |
3768958 | Sakai et al. | Oct 1973 | A |
3895488 | Koch | Jul 1975 | A |
3978657 | Fulton et al. | Sep 1976 | A |
4086758 | Harboe | May 1978 | A |
4140473 | Hoehing et al. | Feb 1979 | A |
4188782 | Smith | Feb 1980 | A |
4238925 | Lowther | Dec 1980 | A |
4242863 | Bailey | Jan 1981 | A |
4289475 | Wall et al. | Sep 1981 | A |
4302177 | Fankhanel et al. | Nov 1981 | A |
4380147 | Zaba | Apr 1983 | A |
4392809 | Tieberg et al. | Jul 1983 | A |
4397633 | Rowlee | Aug 1983 | A |
4462206 | Aguet | Jul 1984 | A |
4532982 | Nakamura | Aug 1985 | A |
4838029 | Gleason | Jun 1989 | A |
5022851 | Reiser et al. | Jun 1991 | A |
5057010 | Tsai | Oct 1991 | A |
5080579 | Specht | Jan 1992 | A |
5121600 | Sanders et al. | Jun 1992 | A |
5149260 | Foust | Sep 1992 | A |
5161365 | Wright | Nov 1992 | A |
5617716 | Schreiber et al. | Apr 1997 | A |
5657624 | Kang et al. | Aug 1997 | A |
5816790 | Ichinose et al. | Oct 1998 | A |
5894729 | Proeschel | Apr 1999 | A |
5938427 | Suzuki et al. | Aug 1999 | A |
5944504 | Tanaka et al. | Aug 1999 | A |
6116016 | Wada et al. | Sep 2000 | A |
6123540 | Ogata et al. | Sep 2000 | A |
6210150 | Rosen et al. | Apr 2001 | B1 |
6233916 | Anand et al. | May 2001 | B1 |
6350116 | Herrmann | Feb 2002 | B1 |
6663381 | Manohar | Dec 2003 | B2 |
6702570 | Shah et al. | Mar 2004 | B2 |
6863523 | Giella | Mar 2005 | B2 |
6866091 | Autenrieth | Mar 2005 | B2 |
6932594 | Weclas et al. | Aug 2005 | B2 |
7028476 | Proeschel | Apr 2006 | B2 |
7476098 | Iio | Jan 2009 | B2 |
7500347 | Sanders et al. | Mar 2009 | B2 |
7624576 | Alkabie et al. | Dec 2009 | B2 |
7658078 | Nishida et al. | Feb 2010 | B2 |
7950919 | Johnson et al. | May 2011 | B2 |
8196388 | Park et al. | Jun 2012 | B2 |
8360770 | Canacik et al. | Jan 2013 | B2 |
8382470 | Kinnunen | Feb 2013 | B2 |
8496472 | Roberts et al. | Jul 2013 | B2 |
20030054305 | Manohar | Mar 2003 | A1 |
20040002029 | Giella | Jan 2004 | A1 |
20040002030 | Shah et al. | Jan 2004 | A1 |
20050053878 | Bruun et al. | Mar 2005 | A1 |
20050257523 | Proeschel | Nov 2005 | A1 |
20060105278 | Katayama | May 2006 | A1 |
20060210936 | Veenstra | Sep 2006 | A1 |
20070125091 | Roby et al. | Jun 2007 | A1 |
20080110083 | Baehr et al. | May 2008 | A1 |
20080115502 | Roby et al. | May 2008 | A1 |
20080145805 | Towler et al. | Jun 2008 | A1 |
20080182213 | Masin | Jul 2008 | A1 |
20080305445 | Roberts et al. | Dec 2008 | A1 |
20090120338 | Adendorff et al. | May 2009 | A1 |
20090202953 | Masin | Aug 2009 | A1 |
Number | Date | Country |
---|---|---|
19606560 | Sep 1997 | DE |
42454 | Dec 1981 | EP |
2096761 | Oct 1982 | GB |
52034148 | Mar 1977 | JP |
54141426 | Nov 1979 | JP |
55014413 | Jan 1980 | JP |
08291719 | Nov 1996 | JP |
2002115812 | Apr 2002 | JP |
WO 9811386 | Mar 1998 | WO |
WO 2006086814 | Aug 2006 | WO |
Entry |
---|
“WO—2006086814 MTrans.pdf”, Machine Translation—WO #2006086814, EPO, May 30, 2012. |
Number | Date | Country | |
---|---|---|---|
61244546 | Sep 2009 | US |