This application is the US National Stage of International Application No. PCT/EP2007/059320, filed Sep. 6, 2007 and claims the benefit thereof The International Application claims the benefits of Great Britain application No. 0621798.8 GB filed Nov. 2, 2006, both of the applications are incorporated by reference herein in their entirety.
The invention relates to a nozzle for a fuel injector, and to a nozzle for a fuel injector supplying atomised liquid fuel to a device such as a gas-turbine engine.
Fuel-injector nozzles for supplying atomised droplets of liquid fuel to a combustion chamber in a gas-turbine engine are already known. One example is described in European patent application EP 1139021, which was published on 4 Oct. 2001 and involves the same inventor as the present application. FIGS. 1-3 of EP 1139021 are reproduced here as
A tubular, electrically conductive electrode 40 is provided near the outlet end of the nozzle 24. The electrode 40 has a sharp edge 42, which extends in the direction of travel of the fuel through the nozzle. Insulating layers 44, 46 are provided on respective sides of the electrode 40.
The fuel is subjected to an electrostatic charge at the point where the fuel stream, which keeps to the inside wall 38, starts to break up into droplets as it exits the outlet 36. A charge supply and control unit 48 (see
Electrostatic charging of the fuel is beneficial mainly when the engine is running at low loads, i.e. when less fuel is being delivered to the nozzles 24. Such charging then helps to control the atomisation and vaporisation of the fuel, the fuel placement and combustion intensity. By contrast, it may not be necessary to employ electrostatic charging when the engine is running at full load.
The fuel-injection nozzle disclosed in EP 1139021 has the drawback that it is complex and thereby costly to manufacture. In addition the volume occupied by the nozzle is quite large, especially in the axial direction.
The present invention seeks to mitigate these drawbacks.
In accordance with the invention there is provided a nozzle for a fuel injector for supplying atomised liquid fuel, the nozzle comprising: an electrode comprising a substantially planar electrically conductive member containing an aperture, the edge of the aperture being sharp to enable the electrode to impart charge; first and second insulating members disposed to respective sides of the plane of the electrically conductive member, the first insulating member being disposed on an outlet side of the nozzle, and swirler means for supplying a swirling flow of liquid fuel to the aperture, the axis about which the fuel swirls within the aperture being generally perpendicular to the plane of the electrode, wherein, in use of the nozzle, the electrode imparts charge to the swirling flow of liquid fuel within the aperture such that the nozzle supplies charged droplets of atomised fuel.
The first and second insulating members may have first and second apertures, respectively, which are substantially coaxial with the aperture of the conductive member. The second aperture may be larger than the first aperture. Furthermore, the aperture of the conductive member may be smaller than the first aperture.
The conductive member may have a thickness, which decreases in a radial direction between the second aperture and the aperture of the conductive member. The decrease in thickness of the conductive member may be substantially linear.
The nozzle may further comprise first and second substantially planar members disposed on outer planar sides of the first and second insulating members, respectively, the first substantially planar member comprising an outlet orifice for the supplying of the charged droplets of atomised fuel. The outlet orifice is preferably substantially the same size as the first aperture.
The swirler means may be a radial swirler means, which may comprise radial passages provided in the second insulating member and communicating with the second aperture.
Alternatively, the swirler means may be an axial swirler means. In this case passages may be provided in the second substantially planar member and communicating with the second aperture, said passages being oriented such as to impart an axial and a tangential component of flow to incoming fuel.
Embodiments of the invention will now be described, by way of example only, with reference to the accompanying drawings, of which:
a) is a sectional view through a generalised fuel-injection nozzle according to the present invention and
a) is a perspective view of a second embodiment of the nozzle shown in
b) and 8(c) are a sectional view and a plan view, respectively, of a lower substantially planar member forming part of the nozzle of
Referring now to
The planar members 100, 108 are preferably composed of metal, while the insulation layers are preferably composed of mica or a ceramic material. Silicon-based compounds are not suitable, since they are attacked by hydrocarbons. In order to resist erosion and maintain sharpness over a long period, the conductive member 104 is preferably composed of a hard, heat-resistant material, such as the high-speed tool steel or Stellite 6™ mentioned in EP 1139021.
There are provided in one of the lower components, e.g. the lower planar member 108, a series of holes 112, which are disposed such as to impart a rotational component of flow to liquid fuel flowing through these holes. The swirling fuel enters the space defined by lines 110, flows past the conductive member 104 and out through the outlet orifice 114, emerging as droplets of fuel. Along the way, the fuel picks up electronic charge produced by the application of a suitably high voltage between the conductive member 104 and a reference-potential point (e.g. earth). Since the planar members 100 and 108 are made of metal, it is assumed that they will likewise be held at a reference-potential point, e.g. earth.
A first, more practical, nozzle arrangement corresponding to a first embodiment of the invention is shown in
The operation of the nozzle is seen in greater detail in
The detail of the construction and action of the conductive member 104 is illustrated in
The conductive member 104 has a thickness, which decreases substantially linearly between the annulus forming the aperture of the lower insulation layer 106 and the annulus forming the aperture of the upper insulation layer 102. This assists the flow of the liquid fuel from the spin chamber 122 into the passage formed by the apertures of the upper insulation layer 102 and upper planar member 100.
A second embodiment of a nozzle in accordance with the invention is illustrated in
When the edge 140 of the electrode 104 is referred to as sharp, this means sufficiently sharp to effectively impart charge to the fuel droplets as they rapidly leave the outlet 114 of the nozzle. Purely as an example, it is considered that this requirement could be met with an edge 140 having an included angle of about one half of a degree, and a radius of not more than about one micron, though these are not hard and fast figures.
Although it has been assumed that the electrode 104 will have a bevelled profile at its radially inner extremity, this is not absolutely necessary. It is, however, preferred, as mentioned earlier, in order to improve the flow characteristics of the fuel as it passes from the inlet passages into the aperture region of the electrode 104 and first planar layer 102.
In order to ensure that the electrons discharged from the conductive member can reliably charge the passing fuel, account is ideally taken of the tendency of the electrons to flow to ground through the hydrocarbon fuel, which is usually electrically conductive. This is achieved by arranging for a suitable rate of flow of the liquid fuel past the conductive member.
Details on how to determine a suitable flow rate through the nozzle are contained in, for example, the paper “The Electrostatic Atomization of Hydrocarbons” by A. J. Kelly, Journal of the Institute of Energy, June 1984, pp 312-320. According to this paper, most commercial hydrocarbons have an electrical breakdown strength in the region of 2×107 V/m. Once charge has been injected into the fuel stream by the charging electrode, it stagnates in the fluid. Subsequently, the charge is acted upon by the fluid flow and the electrical forces which act to attract the charge to the orifice electrode. As mentioned earlier, this orifice electrode (the planar member 100 in the present invention) will be held at a reference potential relative to the potential on the charging electrode (the electrode 104 in the present invention). For commercial oxygenated hydrocarbons, the electrical mobility is commonly in the range of 10−7-10−8 m2/V·sec. (The electrical mobility is the ratio of the limiting velocity, to which a particle is accelerated in the presence of an electric field, to the magnitude of that field). Therefore, for a maximum electrical field of 2×10−7 V/m, the mobility of the charge will be approximately 2 m/s. This means that the fluid should ideally be flushed through the nozzle at a speed >2 m/s in order to reliably retain charge and provide good atomization.
It should be noted that the dielectric constant (electrical breakdown strength) for biofuels is approximately 50% higher than that for standard fuels. Consequently, if most commercial fuels have a dielectric constant of 2×107 V/m, as mentioned above, then most biofuels will have a dielectric constant of around 3×107 V/m. Since it is assumed that the electrical mobility for biofuels is roughly the same as for standard fuels—i.e. approximately 10−7-10−8 m2/Vs—then a nozzle flow speed of ˜3 m/s would be required, if the same charging efficiency were to be maintained.
In an analogous manner, if a silicone oil were to be employed as the fuel passing through the nozzle, this would have a dielectric constant of about 1.5×107 V/m. Again, on the assumption that the electrical mobility for biofuels is of the same order as that for standard fuels, a nozzle flow speed of 1.5 m/s would be suitable.
Number | Date | Country | Kind |
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0621798.8 | Nov 2006 | GB | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2007/059320 | 9/6/2007 | WO | 00 | 4/30/2009 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2008/052830 | 5/8/2008 | WO | A |
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Entry |
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A.J. Kelly, “The Electrostatic Atomization of Hydrocarbons”, Journal of the Institute of Energy, Jun. 1984, pp. 312-320. |
Number | Date | Country | |
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20100065663 A1 | Mar 2010 | US |