REDUCED DIESEL FUEL CONSUMPTION USING MONATOMIC OXYGEN

Abstract

One approach to providing atomic oxygen for the purpose of promoting more rapid and compact combustion is to disperse a low concentration of an atomic oxygen precursor, such as nitrous oxide (N.sub.2O), into the compressed air in the cylinder before or close to the time of ignition. The introduction of N.sub.2O may take place in the intake manifold, directly into the combustion chamber through a small orifice in the base of the fuel injector or a small nozzle located elsewhere in the cylinder head, or the N.sub.2O can be added as a solute to the injected fuel.

Claims

1. A method, comprising: providing monatomic oxygen in a combustion chamber in a diesel engine sufficiently prior to or at the time of ignition of diesel fuel in the combustion chamber at a time relative to the time of ignition and in an amount sufficient so that combustion of the diesel fuel in the combustion chamber adjacent a wall of the combustion chamber is reduced.

2. The method of claim 1, wherein the presence of the monatomic oxygen results in a layer of gas that at least partially insulates the wall of the combustion chamber.

3. The method of claim 2, wherein the partially insulating layer reduces heat transfer from the combustion chamber to the wall of the combustion chamber.

4. The method of claim 1, wherein a fuel efficiency of the diesel engine is improved by the monatomic oxygen.

5. The method of claim 4, wherein the fuel efficiency is improved by at least about 2%.

6-12. (canceled)

13. The method of claim 1, wherein the monatomic oxygen reduces a duration of combustion of the diesel fuel.

14. The method of claim 1, wherein the monatomic oxygen reduces a size of a combustion zone of the diesel fuel.

15. The method of claim 1, wherein the monatomic oxygen reduces an amount of heat transferred to the wall of the combustion chamber during combustion of the diesel fuel.

16. The method of claim 1, wherein providing the monatomic oxygen comprises introducing nitrous oxide (N.sub.2O) into the combustion chamber.

17. The method of claim 16, wherein the N.sub.2O is introduced at a rate in the range from 0.001% to about 10% of the rate of fuel consumption.

18-20. (canceled)

21. The method of claim 16, wherein the N.sub.2O is introduced into the combustion chamber via an intake manifold airstream.

22-23. (canceled)

24. The method of claim 16, wherein introducing the N.sub.2O comprises sensing one or more parameters associated with the diesel engine and modifying one or more parameters associated with introducing the N.sub.2O, wherein the one or more parameters associated with the diesel engine are selected from the group consisting of a vehicle speed, an engine load, an amount of N.sub.2O, a frequency of the pulses, and a timing of the pulses with respect to the ignition of the diesel fuel.

25-26. (canceled)

27. The method of claim 16, wherein the N.sub.2O is introduced as a solute in the injected diesel fuel.

28-33. (canceled)

34. The method of claim 1, wherein the monatomic oxygen is provided by introducing ultraviolet light in the combustion chamber.

35. The method of claim 34, wherein the ultraviolet light is introduced within about 10 ms of the time of ignition of the diesel fuel.

36-50. (canceled)

51. The method of claim 34, wherein the electrical discharge is timed based on a signal from a crankshaft angle detector.

52. A diesel engine, comprising: a means for providing monatomic oxygen in a combustion chamber in the diesel engine sufficiently prior to or at the time of ignition of diesel fuel in the combustion chamber and in an amount sufficient so that combustion of the diesel fuel in the combustion chamber adjacent a wall of the combustion chamber is reduced.

53-80. (canceled)

81. A diesel engine, comprising: one or more combustion chambers; a diesel fuel delivery system arranged to deliver diesel fuel from a fuel tank to the one or more combustion chambers; a light source module arranged to provide ultraviolet radiation to at least one of the combustion chambers; and an electronic control module in communication with the diesel fuel delivery system and the light source module and programmed to coordinate delivery of diesel fuel to the combustion chambers and delivery of ultraviolet radiation to provide monatomic oxygen in the combustion chamber at a time of combustion of diesel fuel in the combustion chamber.

82-92. (canceled)

Description

DESCRIPTION OF DRAWINGS

[0039] FIGS. 1A-D show the sequence of strokes of an example diesel internal combustion engine.

[0040] FIG. 2 shows an example diesel engine fuel delivery system equipped for addition of N.sub.2O to the fuel.

[0041] FIG. 3 shows an example diesel engine fuel delivery system modified for addition of nitrous oxide to the fuel.

[0042] FIG. 4 shows an example nitrous oxide delivery system in which liquid N.sub.2O is delivered directly to a fuel line on its way from a common rail to a fuel injector.

[0043] FIG. 5 shows an example UV light injection assembly for supplying a pulse of UV-rich light to the interior of an diesel engine combustion chamber.

[0044] FIG. 6 shows the top of one cylinder of an internal combustion engine installed with the UV light injection assembly of FIG. 5.

[0045] FIG. 7 shows an example electric arc flash unit for creating an intense flash of light.

[0046] FIG. 8 shows an example electronic circuit used to create an electric arc.

[0047] FIG. 9 shows an example configuration for testing the performance of an engine with a nitrous oxide delivery system.

DETAILED DESCRIPTION

[0048] Other than mechanical friction, factors limiting the efficiency of diesel engines are generally tied to the conditions prevailing during the in-cylinder combustion. In particular, it is believed that causing the air-fuel mixture to burn more rapidly and completely before reaching the cylinder walls may allow a less heated layer to persist near the walls, reducing heat loss to the walls and thereby improving engine efficiency. It is further believed that causing the air-fuel mixture to burn more rapidly and completely may provide more time for the combustion gases to expand against the piston, thereby delivering more mechanical work and lowering the heat and pressure lost when the exhaust is vented.

[0049] One factor controlling both the duration of combustion and the size of the zone in which combustion takes place is the nature of the oxidizing species encountered by the fuel. Normally the only such species is molecular oxygen, O.sub.2, which for quantum mechanical reasons is believed to react relatively slowly with fuel molecules. It is believed that monatomic oxygen atoms is capable of reacting more rapidly than molecular oxygen, but engine temperatures are not generally high enough to dissociate O.sub.2 into significant amounts of free O. Thus auto-ignition of diesel fuel during compression relies on a gradual increase in local temperature caused by relatively slow reactions involving molecular oxygen, such as

RH+OO.fwdarw.R+HOO.,

RH+HOO.fwdarw.R+HOOH

HOOH.fwdarw.2 HO.,

RH+HO..fwdarw.R+H.sub.2O,

R.+OO.fwdarw.ROO., etc.

[0050] These reactions continue until they produce temperatures and free radical concentrations high enough to initiate the avalanche of combustion-propagating chain reactions. At that point, ignition has occurred and full combustion can begin.

[0051] While normal combustion in diesel engines is controlled, for example, by engine operating conditions and the kinetics of slow reactions involving fuel and O.sub.2 molecules, the situation would be far different if free O atoms were present, because such atoms can react vigorously with fuel molecules to cause rapid ignition. Because heat alone does not produce enough free O atoms, it is believed that diesel combustion can be improved by introducing free O atoms from some other source, at a time and place where they will do the most good.

[0052] Accordingly, methods are disclosed which can be used to introduce a small but effective concentration of atomic oxygen into the combustion chamber at a time and location suited to promote rapid and compact combustion at a greater distance from the cooled metal walls of the combustion chamber. In other words, the methods may reduce a duration of combustion in a cylinder relative to the duration combustion would otherwise take in the absence of the atomic oxygen. Furthermore, combustion may be confined to a zone that is smaller than the volume of the combustion chamber (e.g., 99% or less of the volume of the combustion chamber, 95% or less of the volume of the combustion chamber, 90% or less of the volume of the combustion chamber). Both the duration of combustion and the size of the combustion zone may be measured by visual observation (e.g., by use of a high speed camera) or other means.

[0053] In situations where the zone of combustion is reduced in volume relative to the size of the combustion zone without atomic oxygen and the combustion zone does not extend to the walls of the chamber, it is believe that the air between the combustion zone and the walls thus constitutes a partially insulating layer which can hinder heat loss to the walls and leave more energy available to do mechanical work. In some implementations, the increased speed of combustion may require a delay in fuel injection to ensure that the combustion peak pressure is still reached at the most effective time, for example a few crankshaft degrees after TDC (e.g., 10 or less, 8 or less, 5 or less, 4 or less, 3 or less, 2 or less, 1 or less).

[0054] One approach to providing atomic oxygen for the purpose of promoting more rapid and compact combustion is to disperse a low concentration of an atomic oxygen precursor, such as nitrous oxide (N.sub.2O), into the compressed air in the cylinder before or close to the time of ignition. The introduction of N.sub.2O may take place in the intake manifold, directly into the combustion chamber through a small orifice in the base of the fuel injector or a small nozzle located elsewhere in the cylinder head, or the N.sub.2O can be added as a solute to the injected fuel.

[0055] Introduction of N.sub.2O directly into the combustion chamber may be done continuously, or it may be pulsed so as to occur at the time of, or shortly before, auto-ignition. Introduction of N.sub.2O as a solute in the fuel may be done in the low pressure fuel line leading to the engine, into the high pressure fuel line leading to the injectors, or inside the injectors themselves.

[0056] Introduction of N.sub.2O into the fuel immediately before injection may eliminate the need to store, handle, or dispense quantities of N.sub.2O-loaded fuel which could emit N.sub.2O vapor into the atmosphere, where it acts as a greenhouse gas, or into the head space of tanks and storage vessels, where it could pose a safety risk. Instead, the N.sub.2O would be provided in pressurized containers prefilled with the compound in liquid form, ready to be attached to a coupling in the engine compartment. Tanks of liquefied N.sub.2O are classified as safe for public sale and U.S. interstate transport. It is believed that liquid N.sub.2O does not cause explosions, and it is believed that the compound is completely destroyed by diesel combustion, so the disclosed approach may fully address safety and pollution concerns.

[0057] Without wishing to be bound by theory, it is believed that when heated, nitrous oxide dissociates to produce nitrogen and atomic oxygen:

##STR00001##

This heat-catalyzed reaction begins near the time and place of auto-ignition, specifically in the sheath of combustion which originates along the surface of the jet of vaporizing fuel where vaporized fuel mixes with atmospheric oxygen. Thereafter the thermally initiated release of monatomic oxygen from N.sub.2O follows the expanding flame front, assisting in flame propagation and leading to more rapid and compact combustion which is separated from the cooled walls of the combustion chamber by a partially insulating region of flame-free air.

[0058] It has been found that as little as 1.25 wt-% of nitrous oxide for example, based on the rate of fuel consumption, can lead to a reduction in fuel consumption in excess of 25%.

[0059] Implementations of this technique are not to be confused with the practice of introducing a pound or more per minute of N.sub.2O into racing engines to produce a large but necessarily brief increase in engine power. Such power enhancement is attributable to two factors: [0060] 1. N.sub.2O contains 36% oxygen, compared with 21% in air, so when N.sub.2O is used to replace a large fraction of the incoming air the engine can burn more fuel and produce more power. [0061] 2. N.sub.2O is a refrigerant which, when stored as a pressurized liquid and then released into the inlet airstream, causes a drop in temperature. This increases the density of the intake gas and provides even more oxygen.

[0062] This practice relies on very rapid consumption of N.sub.2O, typically pounds per minute, to produce a very large increase in power, typically tens of horsepower. In contrast, implementations of the techniques disclosed here rely on a comparatively low consumption rate of N.sub.2O, typically grams per minute (e.g., 20 g/min or less, 10 g/min or less, 5 g/min or less, 3 g/min or less, 2 g/min or less, 1 g/min or less), to produce an economically attractive reduction in fuel consumption of 25% or more. It is believed that the two schemes differ in their method, their purpose, and their underlying mechanisms.

[0063] Introduction of monatomic oxygen into the combustion chamber may be achieved using other means. For example, in some implementations, an intense burst of short wavelength UV light is projected through a UV-transparent window directly into the combustion chamber of a diesel engine at the time of, or shortly before the time of auto-ignition. Such irradiation can produce sufficient free O atoms to promote more rapid and compact combustion, away from the combustion chamber walls, to reduce the rate of heat loss, improve engine efficiency, and reduce fuel consumption.

[0064] The dissociation energy of an O.sub.2 molecule corresponds to a photon wavelength of 242 nm, which is in the ultraviolet (UV) portion of the electromagnetic spectrum. Radiation at shorter wavelengths is strongly absorbed by O.sub.2, with copious production of free O atoms. Ambient air, which is 21% oxygen, interacts with such UV so strongly that it can travel only a short distance before being absorbed.

[0065] The degree of absorption of UV light by O.sub.2 increases rapidly at wavelengths shorter than 242 nm. In order to produce a burst of monatomic O atoms throughout a significant volume near the top of the compression stroke, the UV radiation should be largely absorbed while traveling a distance between 0.5 and 5.0 cm, which will allow it to deposit most of its energy over a significant volume before reaching the walls. In compressed air that path length corresponds to wavelengths just below 220 nm, so UV with a wavelength of about 180 to 220 nm can be taken as representative of radiation suitable for dissociating O.sub.2 into O atoms throughout a significant volume of a combustion chamber.

[0066] In general, a variety of UV light sources may be used. An exemplary light source is a short-arc xenon discharge lamp. In a short-arc xenon discharge lamp, a brief high current arc is struck between two closely spaced metal electrodes in a xenon atmosphere. The result is a powerful burst of visible and ultraviolet radiation comprised of characteristic xenon emission lines superimposed on a background of black-body radiation. Such a lamp, for example, the Excelitas model 4402 (commercially available from Excelitas Technologies Corp., Waltham, Mass.), can be operated at power levels as high as 60 watts while flashing 60 times a second and delivering up to 100 mJ of total optical energy per flash. As much as 2 mJ of that radiation can be at wavelengths below 220 nm. That proves to be sufficient to dissociate enough O.sub.2 molecules to promote more rapid and compact combustion out of contact with the walls, thereby diminishing heat loss and reducing fuel consumption by over 25%.

[0067] To make effective use of the optical output of a xenon flash lamp, optics (e.g., lenses, mirrors, etc.) can be used to efficiently direct light from the lamp to the combustion chamber. Such optics can be fabricated from a material highly transparent in the 180 nm to 220 nm range and thermally and mechanically strong enough to survive prolonged exposure to combustion conditions. Commercially-available synthetic fused silica and sapphire are examples of such materials. Such UV-transparent optical components should not become occluded by combustion products, because enough UV, visible, and infrared energy will be absorbed by any deposit to vaporize or displace it.

[0068] Other techniques for generating monatomic oxygen are also possible. For example, certain implementations involve striking a high-current electric arc directly in the compressed air inside the combustion chamber rather than in an enclosed lamp external to the combustion chamber. In such implementations, the electrodes that create the electrical arc are not enclosed, and therefore produce UV and other radiation which illuminates the entire combustion chamber, generating monatomic oxygen and promoting flame propagation over a large volume.

[0069] A high current electrical arc in air is known to produce a significant amount of UV light. For example, workers using arc welding equipment must wear protective clothing to prevent skin or eye damage from the intense UV light created by the welding arc through air. In fact, at high current density, air is nearly as efficient at generating UV light as a xenon arc lamp. Because of the xenon line spectrum, xenon arc lamps produce some UV light efficiently when operated at low current density, but when operated at high current density the UV light output is primarily the result of the very high temperature gas acting as a black body radiator.

[0070] In some implementations the electric arc may be positioned so as to illuminate the entire combustion chamber, and timed to produce a flash of intense UV light 0 to 0.1 msec before fuel injection (e.g., within 0.05 msec, within 0.03 msec, within 0.01 msec, within 0.005 msec, within 0.001 msec of fuel injection), thus making a widespread distribution of monatomic oxygen available during the period leading up to auto-ignition. In some implementations the arc may be positioned near the point of fuel injection and fired near the time of injection, so as to produce a high concentration of monatomic oxygen in the immediate temporal and spatial vicinity of the vaporizing fuel.

[0071] FIG. 2 shows a schematic drawing of a diesel engine fuel delivery system 200 equipped for addition of N.sub.2O to the fuel. Fuel from tank 202 passes through an outlet tube 204 to a low pressure pump 206 which delivers it through a fuel filter 208. Simultaneously, liquid N.sub.2O from a pressurized tank 210 passes through a metering valve 212 where it merges with fuel before passing through a high, constant pressure, on-demand pump 214. The N.sub.2O-loaded fuel then enters high pressure manifold 216, called a common rail, where its pressure is monitored by a sensor 218 before it enters individual injectors 220 which spray it, with proper timing (for example within a crankshaft angle of 10 from top dead center, such as within 8, within 5, within 4, within 3, within 2, within 1) into the combustion zone of each cylinder. The desired fuel injection timing can be adjusted and controlled by an electronic engine control unit 222 similar to those commonly installed on conventional vehicular diesel engines. In some implementations, the fuel may be fed individually to each injector, or the injectors may be timed by cams, but such designs allow the use of N.sub.2O injection in much the same way as the common rail system shown in FIG. 2.

[0072] The metering valve 212 is under the control of an electronic system which adjusts the flow of N.sub.2O to maintain a desired concentration in the fuel. In some implementations, the N.sub.2O may pass through its own high pressure pump before being introduced into the high pressure fuel immediately before the fuel injectors 220, and the electronic control system may or may not include a processor coded to vary the N.sub.2O concentration in response changes in engine RPM and the air-to-fuel ratio.

[0073] FIG. 3 shows a schematic of another implementation of a diesel engine fuel delivery system 300 modified for addition of nitrous oxide to the fuel using an accumulator vessel to obviate the need for an on-demand constant pressure high pressure pump. Referring to FIG. 3, fuel is drawn from a fuel tank 302 by a low pressure pump 304 and delivered through a fuel filter 306 and check valve 308 to a mixing unit 310, which blends the fuel with a fixed proportion of liquid nitrous oxide from a pressurized tank 312 and N.sub.2O metering valve 314. The N.sub.2O-doped fuel then passes to an accumulator 316 which provides a feed stream to the high pressure pump 318, which in turn delivers N.sub.2O-doped fuel at high pressure to the common rail 320 and from there to the individual injectors 322. Excess fuel from the common rail escapes through a pressure relief valve 324 and recirculates through a return fuel line 326 to the high pressure pump 318, so only the small volume of fuel actually consumed need be replaced by the low pressure pump 304 and the accumulator 316. Check valve 308 acts as a safety to prevent N.sub.2O-doped fuel from ever returning to the fuel tank 302 to eliminate the possibility of N.sub.2O gas accumulating in the fuel tank 302.

[0074] FIG. 4 shows another implementation of a nitrous oxide delivery system 400 in which liquid N.sub.2O under autogenous pressure is delivered by a high pressure solenoid pump directly to each fuel line on its way from the common rail to a fuel injector. Referring to FIG. 4, fuel 402 from the fuel tank (not shown) is pressurized by a high pressure pump 404 and passed to a common rail 406 from which it passes through individual feed lines 408 to the fuel injectors 410. Concurrently, liquid N.sub.2O 412 from a pressurized holding tank (not shown) passes into a small, calibrated volume, high pressure solenoid pump 414 whose pulses are adjusted to produce the desired concentration of N.sub.2O. The pulse of high pressure nitrous oxide is then blended with the fuel en route to the fuel injector 410. Check valve 416 acts as a safety to prevent N.sub.2O-doped fuel from ever returning to the fuel tank to eliminate the possibility of N.sub.2O gas accumulating in the fuel tank.

[0075] In some implementations, an ultraviolet flash lamp can be used to introduce an intense flash of light, rich in short wavelength UV radiation, through a window directly into the combustion chamber near or shortly before the time of fuel ignition. FIG. 5 shows an example implementation of a UV light injector assembly 500 for supplying a pulse of intense UV-rich light to the interior of a diesel engine combustion chamber from a source external to the chamber. In this example implementation, the light is produced by a short-arc xenon flash lamp 502, though other light sources can be used. This flash lamp 502 includes an integral reflector (e.g., a parabolic reflector) to collimate the majority of its light into parallel rays. For practical considerations in the construction of many internal combustion engines, the window 504 passing UV light into the cylinder should be relatively small, for example 2 mm to 10 mm in diameter, and preferably 4 mm to 8 mm in diameter. To direct the collimated rays of light from the flash lamp 502 through the window 504, a UV-transparent condensing lens 506 is used to focus the light 508 from the flash lamp 502 onto the window 504. For transparency to short wavelength UV, the condensing lens 506, window 504, and window extension 510 can be made of synthetic fused silica, sapphire, or another UV transparent material that has sufficient strength and heat resistance. Likewise, the flash lamp 502 envelope uses one of these UV transparent materials to allow the UV light to exit. An alternative construction is to use a flash lamp 502 with an ellipsoidal reflector which provides focused rather than collimated light, thus eliminating the need for the condensing lens 506.

[0076] FIG. 5 also shows an alternate window shape 510 that includes a protrusion 512 into the engine cylinder. This protrusion 512 has a concave depression in the end, such as a conical indentation, to provide a reflective surface or total internal reflection surface to distribute the light inside the cylinder for more effective illumination of the combustion volume. The window extension 510 may be asymmetrical, particularly if the window 504 is not centered in the top of the cylinder head 514. The shape of the extension 510 can be used to distribute the light in an optimum pattern within the engine cylinder.

[0077] In addition to the optical components, this example configuration includes an electrical connector and trigger module 516 for the flash lamp 502. This module 516 has one or more wires 518 that connect to a power source and a flash timing controller (not shown) that assures that the flash of light occurs with the desired intensity and at the desired time.

[0078] A mechanical housing 520 holds all the optical and electrical components in the proper position and contains a UV-transparent atmosphere 522 such as a near vacuum, nitrogen gas, or another gas that does not significantly absorb the short wavelength UV. The mechanical housing 520 includes a threaded protrusion 524 that holds the window 504 and screws into the engine cylinder head 514 to direct the light 508 into the cylinder. A pressure seal 526 is included around the threaded protrusion 524 to contain the high pressure gases in the engine cylinder. The mechanical housing 520 may be hexagonal in cross-section for easy screwing and tightening into the cylinder head 514. This mechanical configuration can be easily attached to or detached from the engine for installation, repair or replacement.

[0079] FIG. 6 shows a simplified diagram of the top of a cylinder 600 of an internal combustion engine with the UV light injector assembly 500 installed so that the light distributor extension 510 of the window protrudes through the engine cylinder head 514 into the combustion space at the top of the engine cylinder. The UV light injector assembly 500 is positioned near the fuel injector 602 so the UV light 508 can illuminate the volume into which the fuel is injected. The light distributor 510 can be shaped such that the light from the flash lamp is primarily directed to the desired volume where the combustion will be initialized.

[0080] One or more wires 518 connect the UV light injector assembly 500 to a power source and flash timing controller (not shown) that cause the flash of light to occur at the desired time. The timing of the electric arc flash unit can be determined by a crankshaft angle sensor and control module already provided on diesel vehicles to time fuel injection. This time will typically be when the piston 604 is near the top of the compression stroke, for example between a crankshaft angle of 5 to 0 before fuel injection. At this time both the intake valve 606 and the exhaust valve 608 are closed so the hot air contained within the volume created by the cylinder walls 610, piston 604, and cylinder head 514 is compressed and ready to support combustion. The fuel injector 602 injects a fuel spray 612 into the combustion volume when the air has been compressed to near its minimum volume. The UV light dissociates oxygen in the air into oxygen atoms and thereby reduce heat loss to the walls by promoting a rapid and compact combustion zone which makes minimal contact with the metal walls. The energy from the flash of light can also promote more rapid burning by assisting in the evaporation of the fuel droplets.

[0081] In some implementations, atomic oxygen within the combustion chamber is generated by using an electric arc exposed directly inside the combustion chamber to produce an intense flash of light containing short wave UV radiation. The arc electrodes can be positioned so that all the light emitted from the arc permeates the cylinder volume. This eliminates the costs and losses associated with the optics necessary to direct light from an external source into the cylinder.

[0082] FIG. 7 shows an example configuration of an electric arc flash unit 700 useful for creating an intense flash of light, containing short wavelength UV radiation, directly inside a diesel engine combustion chamber. In this example configuration, the electric arc 702 is created between two arc electrodes 704a-b which extend through the cylinder head 514 into the internal volume of the engine cylinder. The arc electrodes 704a-b are connected to a source of electrical energy of sufficient voltage (typically 1,000 to 3,000V) to create a high energy electric arc 702 between the arc electrodes 704a-b. Because of the elevated air pressure in the cylinder, a third higher voltage trigger electrode 706 is used to initiate the arc 702 and control the precise timing.

[0083] The energy for the electric arc 702 is stored in one or more capacitors that are contained in the housing of the electric arc flash unit 700, or alternatively in a remote location dictated by available space or other considerations. Control wires 518 connect to the control electronics (not shown) to provide the energy to charge the capacitors, and to provide the trigger signal to initiate the electrical arc 702 at the desired time. If the energy storage capacitors are in a remote location, these wires 518 include the two conductors that connect directly to the arc electrodes 704a-b. In general, the control electronics can include standard and/or custom components, such as data storage media (e.g., a non-volatile memory chip) and an electronic processor (e.g., an ASIC).

[0084] The electric arc flash unit 700 includes a threaded protrusion 524 that is screwed into a hole in the cylinder head 514. The central portion of this protrusion is filled with a high temperature insulating material 708, such as a ceramic, to keep the electrodes (704a-b and 706) electrically isolated from each other and provide a gas-tight seal. A pressure seal 526 is also included around the threaded protrusion 524 to provide an additional seal against gas leakage.

[0085] FIG. 8 shows a schematic diagram of an electronic circuit 800 that can be used to create the electric arc 702. The circuit 800 includes of one or more energy storage capacitors 802 that hold energy for rapid electrical current delivery to the arc electrodes 704a-b. To obtain the highest efficiency of UV light production the energy storage capacitors 802 should generally be charged to a voltage greater than 1,000V. If other system constraints require a lower voltage, useful results can be achieved with voltages as low as a few hundred volts. The energy storage capacitors 802 are charged from an external high voltage power supply (not shown) which applies the charging current 804 to the energy storage capacitors 802 with a ground return connection 806. The energy storage capacitors 802 are charged during the interval of time between successive electrical arcs.

[0086] The value of the energy storage capacitors 802 is chosen to provide the desired amount of energy to the flash. Flash energy will typically be in the range of 0.5 to 5 joules per flash depending on the size of the engine and other operating characteristics. The energy in the energy storage capacitors 802, in joules, is defined by the expression 0.5CV.sup.2 where C is the total capacitor value in farads, and V is the voltage on the capacitor(s) in volts. For example, a 2 microfarad capacitor charged to 2 kV would store 4 joules of electrical energy. Because of the elevated air pressure in the cylinder, a higher voltage trigger electrode 706 may be needed to partially ionize the air between the arc electrodes 704a-b and initiate the electric arc 702 at the desired time. The trigger voltage is typically in the range from 5,000 to 50,000 volts. The trigger pulse can be very short, with a duration on the order of 1 microsecond. These pulses can be produced using a trigger transformer 808 designed for use with standard xenon flash lamps.

[0087] Standard flash trigger transformers 808 are typically designed to be powered from a voltage of approximately 200V to 300V, so this circuit includes a voltage divider made up of resistors 810 and 812 to provide the appropriate voltage from the higher voltage energy storage capacitors 802. An additional, much smaller trigger energy storage capacitor 814 holds energy for the trigger transformer 808 to produce the high voltage trigger pulse. The trigger pulse is produced when the flash trigger silicon-controlled rectifier (SRC) 816 is turned on with a flash trigger signal 818 from the control electronics (not shown). When the flash trigger SCR 816 is turned on, current flows from the trigger energy storage capacitor 814 through the flash trigger transformer 808 to electrical ground 806. The windings in the flash trigger transformer 808 have a high ratio (e.g., 20 to 100 as needed) between the secondary and primary to produce the high voltage trigger pulse to the trigger electrode 706. Resistor 820 is included to reduce the likelihood of triggers to the flash trigger SCR 816 due to spurious electrical noise on the flash trigger signal line 818.

[0088] In an example implementation, resistors 810, 812, and 820 are 1M ohm, 100K ohm, and 1K ohm resistors, respectively, trigger energy storage capacitor 814 is a 0.47 F capacitor, trigger electrode 706 delivers a 25 KV pulse, and the voltage differential between arc electrodes 704a-b is 1 to 3 KV. These component parameters are given as an example. Components having different parameters may be used, depending on the implementation.

[0089] The components, steps, features, objects, benefits and advantages that have been disclosed above are merely illustrative. Neither they, nor the discussions relating to them, are intended to limit the scope of protection in any way. Numerous other embodiments can be envisioned, including embodiments that have fewer, additional, and/or different components, steps, features, objects, benefits and advantages. Nothing that has been stated or illustrated is intended to cause a dedication of any component, step, feature, object, benefit, advantage, or equivalent to the public. While particular embodiments of the present application have been described, variations of the present application can be devised without departing from the inventive concepts disclosed in the disclosure.

EXAMPLES

[0090] Example implementations are described below.

[0091] Example 1. In one example, over the course of 15 minutes, 100 grams of nitrous oxide is bubbled through 3000 grams of CN 45 diesel fuel, causing a weight gain of 10 grams, equivalent to 0.33%. A similar quantity of unmodified fuel is reserved in an identical container, and both containers are weighed. A John Deere M4024T four cylinder diesel engine mounted on a test rack and governed at 1800 RPM is rigidly connected to a 60 cycle AC Dynamo which in turn is connected to a set of four individually switchable 5 kW electrical heaters. A control panel is provided to allow RPM, current and voltage to be read in real time. Fuel consumption is monitored by weight.

[0092] The engine is started on standard diesel fuel from its own tank and allowed to reach steady state operating conditions for 15 minutes under a 5 kW load. Fuel flow is then switched to the graduated container of unmodified fuel and the engine is operated with a 5 kW load for 5 minutes, at which time flow is switched to the N.sub.2O doped fuel for the same length of time. At the beginning and end of these operating intervals the containers are weighed. Fuel flow is then switched back to fuel from the main tank, and the engine is allowed to equilibrate for 15 minutes with a 10 kW load. The same procedure is then followed with the two containers of unmodified and modified fuel, and this sequence is again followed with 15 kW and 20 kW loads. In all cases the actual load is determined by current and voltage readings.

[0093] Table 1 shows the results of these tests:

TABLE-US-00001 TABLE 1 Unmodified Fuel N.sub.20-Doped Fuel Load Consumption Consumption 0 kW 18 gm/min 14 gm/min 5 kW 30 gm/min 24 gm/min 10 kW 60 gm/min 49 gm/min 15 kW 90 gm/min 70 gm/min 20 kW 120 gm/min 98 gm/min

[0094] Over this range of loads, the consumption of fuel is reduced between 18% and 23% when the engine is operating on fuel containing 0.33% N.sub.2O by weight.

[0095] Example 2. In another example, a Ford F250 truck powered by a 6.0 liter V8 Power Stroke diesel is modified as shown schematically in FIG. 9.

[0096] An experiment is conducted as follows to determine the improvement in mileage of a diesel vehicle produced by a small concentration of N.sub.2O in the fuel. Referring to system 902 of FIG. 9, at the beginning of the experiment, tank 902, the truck's original fuel tank, is filled with conventional fuel having a cetane number of 45; tank 904 is filled with 60.0 kg of the same fuel; and tank 906 is filled with 59.79 kg of the same fuel in which 0.21 kg of N.sub.2O (0.35% by weight) has been dissolved in a manner similar to that of Example 1.

[0097] During travel to a test route, valves 910 and 912 are set so as to deliver fuel from tank 902 through the low pressure pump 914, the filter 916, and the high pressure pump 918 to the common rail 920, from which it is distributed to the individual injectors 922, with excess fuel escaping through pressure relief valve 924 and then flowing through two way valve 912, return line 926, and routing valve 928 back to fuel tank 902.

[0098] Upon the truck arriving at the starting site three way valve 910 is set so as to draw fuel from tank number 904, and two way valve 928 is set to return excess fuel back to tank 904. The truck is immediately driven on a round trip over the 50 km test course, adhering as closely as possible to a predetermined sequence of speeds not exceeding 80 km/hr.

[0099] When once again at the starting point, valve 910 is set so as to draw N.sub.2O-containing fuel from tank 906, valves 912 and 928 are set so as to deliver excess fuel from the pressure relief valve 924 to waste tank 908, and the truck is driven on a round trip over the same course adhering as nearly as possible to the same sequence of speeds.

[0100] During this part of the test run, tanks 906 and 908 automatically adjust their volume so as to minimize head space over the N.sub.2O-containing fuel, thus mitigating any slight risk of exothermic decomposition of N.sub.2O vapor and allowing and little or no N.sub.2O (a known greenhouse gas) to be released into the atmosphere.

[0101] At the conclusion of the experiment valves 910, 912 and 928 are returned to their initial settings so as to draw fuel from, and return fuel to, tank 902; after which the truck is driven back to its base of operations and the weight of fuel remaining in tanks 904, 906, and 908 is accurately determined.

[0102] The mileage obtained using the two fuels is then calculated based on the 100 km total length of the course and the weight of fuel consumed, (60 kg minus the weight of fuel in tank 904) for regular fuel and (60 kg minus the weight of fuel in tank 906 plus the weight of fuel in tank 908) for the N.sub.2O-containing fuel. The results of three repetitions of this experiment show the average mileage on conventional fuel to be 17.1 mpg and the average mileage on N.sub.2O-containing fuel to be 21.4 mpg. Thus under the conditions described here the improvement achieved by the addition of 0.35% N.sub.2O to the fuel is 25.1%.

[0103] Example 3. In another example, a flash lamp and power assembly similar to that shown in FIG. 6 is mounted on each of the four cylinders of a John Deere M40241 diesel engine, and is provided with a timing circuit keyed to the crankshaft angle. The engine is operated at a governed speed of 1800 RPM while driving a 60 hertz AC generator connected to a variable load. When in use the UV flash lamps are triggered to produce monatomic oxygen by means of an arc delivering 1 joule of energy 2 of crankshaft angle before fuel injection.

[0104] The engine is allowed to equilibrate under each set of test conditions for 5 minutes and is then operated for an accurately timed 15 minute test period. Fuel consumption is obtained by weighing the fuel container before and after the test period.

[0105] Table 2 shows the total fuel consumed under different test conditions:

TABLE-US-00002 TABLE 2 External UV Source Load Fuel Consumed Off 5 kW 450 gm On 5 kW 360 gm Off 10 kW 900 gm On 10 kW 720 gm Off 15 kW 1350 gm On 15 kW 1080 gm Off 20 kW 1800 gm On 20 kW 1440 gm

[0106] As shown above, over this range of loads a consistent 20% reduction in fuel consumption is provided by a pulsed external UV source.

[0107] Example 4. In another example, the experiment of Example 3 was repeated with an electric arc flash unit similar to that shown schematically in FIG. 7 replacing the external flash lamp.

[0108] Table 3 shows the total fuel consumed under these various test conditions:

TABLE-US-00003 TABLE 3 Internal Arc UV Source Load Fuel Consumed Off 5 kW 450 gm On 5 kW 348 gm Off 10 kW 900 gm On 10 kW 696 gm Off 15 kW 1350 gm On 15 kW 996 gm Off 20 kW 1800 gm On 20 kW 1395 gm

[0109] As shown above, the reduction in fuel consumption achieved by internally generated short wavelength ultraviolet light ranges from 22% to 26%.

[0110] While several example implementations are described, these are merely examples to demonstrate various benefits of the disclosed systems and techniques. Other embodiments are in the following claims.