The present invention relates to fluidic apparatus, and in particular to fluidic apparatus for use in controlling fuel flow to the combustor of a gas turbine engine.
All gas turbine engines include a combustor in which a mixture of fuel and air is burnt to produce exhaust gases that drive a turbine. To reduce the amount of harmful emissions such as nitrogen oxides (NOx) that are produced during combustion, most modern gas turbine engines burn a lean pre-mixture of fuel and air, without suppression of NOx by injection of water or steam into the combustion process. However, these sorts of dry low emission (DLE) gas turbine engines are particularly prone to acoustic vibrations and noise caused by variations in the gas pressure within the combustor. These pressure variations can have a frequency of 200 Hz or more, and in larger gas turbine engines the acoustic vibrations and noise can be so severe that the combustor is literally shaken to pieces.
One way of minimizing these pressure variations is to modulate the rate of delivery of the fuel flow into the combustor in a controlled manner such that the coupling mechanism which is responsible for the instability is disrupted. The present assignee has successfully modulated the fuel flow using a high bandwidth modulation valve that can operate at the necessary frequencies. The valve can be controlled to modulate a portion of the fuel flow into the combustor using a complex mathematical algorithm. However, such valves are very expensive and potentially unreliable. They also have a limited lifespan.
The purpose of the present invention is therefore to provide an alternative fluidic apparatus for modulating the rate of delivery of fuel flow into the combustor that is cheap to manufacture and very reliable.
Fluidic devices are well known to the skilled person and include bistable fluidic devices and astable (or “flip-flop”) fluidic oscillators. The general principle of operation of bistable fluidic devices and astable fluidic oscillators is explained in The Analysis and Design of Pneumatic Systems, Blaine W. Anderson, John Wiley & Sons, Inc, 1967. In bistable fluidic devices a supply jet of liquid or gas can be made to exit from either of two outlets due to the Coanda effect. The Coanda effect is the tendency of a fluid jet to attach itself to, and flow along, a wall. In bistable fluidic devices the supply jet can be made to switch from one outlet to the other by the application of a relatively small control pressure. In astable fluidic oscillators the supply jet can be made to switch from one outlet to the other continuously.
An astable (or “flip-flop”) fluid oscillator can be made by connecting at least one of the diverging outlets to the control inlet on the same side. Thus, the left-hand outlet 4 can be connected to the left-hand control inlet 8, and/or the right-hand outlet 6 can be connected to the right-hand control inlet 10. The supply jet 12 can then be made to oscillate continuously so that it exits first from the left-hand outlet 4 and then from the right-hand outlet 6. The frequency of oscillation (i.e., the rate at which the supply jet oscillates between the pair of diverging outlets) depends on the length and capacity of the feedback path connecting the diverging outlets to the control inlets. Other factors that also influence the oscillation frequency include the width of the supply inlet 2, the pressure of the supply jet 12 and the angle between the pair of diverging outlets 4, 6.
The present invention provides a fluidic apparatus for modulating the rate of fluid fuel flow into a gas turbine engine combustor, the apparatus comprising a fluidic oscillator device having first and second outlet passages, a supply inlet passage and a junction at which the outlet and inlet passages meet, the inlet passage being connected to a fuel supply line, the first outlet passage being connected to a fuel discharge line for connection to the combustor, whereby in use the fluidic oscillator device outputs fuel from the first and second outlet passages alternately.
By modulating the rate of fuel flow into the combustor it is possible to disrupt a coupling mechanism which is responsible for combustion instability, thereby attenuating the variations in the gas pressure which cause the acoustic vibrations and noise. In practice, the introduction of modulated fuel flow into the combustor effectively prevents the variations in the gas pressure from latching on to certain resonance frequencies at which the acoustic variations and noise are amplified to reach dangerous levels.
The fluidic oscillator device is preferably an astable (or “flip-flop”) fluidic oscillator. It will be readily appreciated by the skilled person that the astable fluidic oscillator can be of any suitable configuration. As described above, astable fluidic oscillators have no moving parts which means that they are cheap to manufacture and very reliable.
In a preferred arrangement, the first and second outlet passages diverge from each other in a direction away from the junction and a control inlet communicates with the junction to effect diversion of fuel flow between the outlet passages. The second diverging outlet may be connected to the control inlet by a feedback line that introduces a time delay. The time delay may be increased by means such as a restrictor and/or a volume in the feedback line. The restrictor and/or the volume is/are preferably variable so that the time delay introduced by the feedback line can be varied.
The time delay introduced by the feedback line determines the oscillation frequency of the fluidic oscillator device.
The fluidic oscillator device can have a pair of oppositely facing control inlets communicating with the junction. In this arrangement each of the diverging outlets can be connected to one of the control inlets by a feedback line. As previously explained, each feedback line preferably includes a means such as a restrictor and/or a volume for introducing a time delay into communication between the second outlet and the control inlet, the restrictor and/or the volume preferably being variable so that the time delays can be varied. The time delays introduced by the feedback lines can be the same or different.
Alternatively, the second control inlet can be connected to the fuel supply line by a bypass line. The bypass line preferably includes a restrictor.
Some of the fuel is preferably supplied from the fuel supply line direct to the fuel discharge line through a bypass line. Hence, a first proportion of fuel for delivery to the combustor bypasses the fluidic oscillator device and a second proportion of fuel for delivery to the combustor passes through the fluidic oscillator device. The bypass line can include means for controlling the proportion of fluid fuel that flows along the bypass line, such as a variable restrictor and/or an adjustable valve.
The fuel can be a liquid or a gas.
The present invention also provides a method of modulating a rate of fuel flow into the combustor of a gas turbine engine, the method comprising the steps of:
The oscillation frequency of the fluidic device is preferably adjustable.
The invention will now be described, by way of example only, with reference to the accompanying drawings, in which:
The present invention will now be explained with reference to
A fluid fuel supply line 14 is connected between the supply inlet 2 and a fluid (liquid or gas) fuel source in the form of a fuel tank 16 of a gas turbine engine (not shown). Supply line 14 includes a pump 15 that supplies fluid fuel at a predetermined pressure to the fluidic oscillator 1.
The left-hand outlet 4 is connected to the combustor 18 of a gas turbine engine (not shown) by means of a fluid fuel discharge line 20.
The right-hand outlet 6 is connected to the right-hand control inlet 10 by means of a feedback line 22. The feedback line 22 includes a variable restrictor 24 and a downstream volume 26.
The left-hand control inlet 8 is connected to the fluid fuel supply line 14 by means of a first bypass line 28 that includes a restrictor 30. However, it will be readily appreciated by the skilled person that the left-hand control outlet 8 could alternatively be connected to the left-hand outlet 4 by means of a feedback line 23, shown as a dashed line, which like feedback line 22 could also include a variable restrictor and a volume, though these are not shown.
A second bypass line 32 is connected between the fluid fuel supply line 14 and the fluid fuel discharge line 20. Fluid fuel from the tank 16 is able to flow along the second bypass line 32 so that only a portion of the fluid fuel is supplied to the supply inlet 2 of the fluidic oscillator. The second bypass line 32 includes a restrictor 34, which may be variable if desired.
The operation of the fluidic apparatus will now be explained.
Fluid fuel from the tank 16 of the gas turbine engine is supplied to the supply inlet 2 of the fluidic oscillator 1 along the fluid fuel supply line 14 at a predetermined pressure from the pump 15.
It will be assumed that the supply jet (not shown) of fluid fuel from the supply inlet 2 initially attaches itself to the side wall of the right-hand outlet 6. The fluid fuel exits from the right-hand outlet 6 and passes along the feedback line through the variable restrictor 24 and into the volume 26. Once the volume 26 has been completely pressurized the fluid fuel is applied to the right-hand control inlet 10. This causes the supply jet of fluid fuel to attach itself to the side wall of the left-hand outlet 4 and the fluid fuel exits from the left-hand outlet. If the left-hand outlet 4 is connected to the left-hand control inlet 8 by a feedback line 23 then the above process will be repeated and the supply jet of fluid fuel will again attach itself to the side wall of the right-hand outlet 6. However, in the case of the preferred fluidic apparatus shown in
The operation of the fluidic oscillator 1 means that fluid fuel is intermittently supplied to the fluid fuel discharge line 20 from the left-hand outlet 4. The rate of delivery of the fuel flow to the combustor 18 is therefore modulated in a controlled manner. However, only a proportion of the total fluid fuel supplied to the combustor 18 needs to be modulated. Most of the fluid fuel is therefore supplied directly to the combustor 18 from the fluid fuel source 16 along the second bypass line 32. The amount of fluid fuel supplied directly to the combustor 18 can be controlled either by restrictor 34 if it is made adjustable, or by an adjustable valve (not shown) in series with the restrictor.
It will be seen from the above description that the fluidic oscillator 1 or 1′ acts to modulate the pressure/rate of delivery of fuel flow into the combustor 18. This can be used to prevent combustion noise frequencies or gas pressure variations from reaching dangerous levels due to being amplified at certain resonance frequencies of the combustion system. The coupling mechanism which is responsible for combustion instability is disrupted, thereby attenuating the variations in the gas pressure which cause the vibration and noise.
It will be understood that each of the elements described above, or two or more together, also may find a useful application in other types of constructions differing from the types described above.
While the invention has been illustrated and described as embodied in a fluidic control of fuel flow, it is not intended to be limited to the details shown, since various modifications and structural changes may be made without departing in any way from the spirit of the present invention.
Without further analysis, the foregoing will so fully reveal the gist of the present invention that others can, by applying current knowledge, readily adapt it for various applications without omitting features that, from the standpoint of prior art, fairly constitute essential characteristics of the generic or specific aspects of this invention and, therefore, such adaptations should and are intended to be comprehended within the meaning and range of equivalence of the following claims.
What is claimed as new and desired to be protected by Letters Patent is set forth in the appended claims.
Number | Date | Country | Kind |
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0201414 | Jan 2002 | GB | national |
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Number | Date | Country | |
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20040020208 A1 | Feb 2004 | US |