This application claims priority to EP application 14157239.6 filed Feb. 28, 2014, the contents of which are hereby incorporated in its entirety.
The invention relates to the acoustic damping of combustion dynamics. Combustion dynamics in the meaning of this application comprises pulsations, acoustic oscillations, pressure and velocity fluctuations and what is called in the everyday language “noise”.
Combustion dynamics occur in combustors of gas turbines, for example, as a consequence of changes in the fuel supply. Excessive pressure fluctuations may result in damage of machine components. For reasons of simplification subsequently the term “chamber” is used and comprises all locations where combustion dynamics occur. In these chambers a gas (for example a mixture of fuel and air or a hot combustion gas) flows with a high velocity.
To reduce these combustion dynamics it is well known in the art, to install acoustic damping devices like Helmholtz resonators, half-wave tubes, quarter-wave tubes or other types of damping devices with or without flow through of gas.
These acoustic damping devices may have one or more resonance frequencies. If under operation of the gas turbine the combustion dynamics stimulate the resonance frequencies of the acoustic damping devices, the combustion dynamics are reduced or damped.
The line 1 shows the theoretical reflection coefficient when using an acoustic damping device with a resonance frequency of approximately 300 Hertz. As can be seen, at a frequency of 300 Hertz the reflection coefficient has a relative minimum of approximately 0.5. At frequencies of approximately 225 Hertz and 375 Hertz, the reflection coefficient has a local maximum of about 0.75.
To give an example: a combustion chamber of a gas turbine is equipped with an acoustic damping absorber having a resonance frequency of 300 Hertz. Assuming that under operation in this combustion chamber fluctuations ensue comprising frequencies of 300 Hertz it can be expected that due to the local minimum of the reflection coefficient at 300 Hertz the fluctuations with a frequency of 300 Hertz are effectively damped and reduced.
In technical experiments the applicant made measurements and compared the theoretical reflection coefficient (line 1) with measurements taken at a frequency range between 50 Hertz and 400 Hertz.
The measured values are illustrated in
By comparing the measured values with the theoretical reflection coefficient (line 1) it can be seen that in the range between 250 Hertz and 350 Hertz the measured values 3 do not show a local minimum as should be expected. In other words: The acoustic damping device does not work sufficiently.
It is an object of the invention, to provide an acoustic damper that is capable of damping effectively in a gas turbine under operation and therefore effectively reduces combustion dynamics ensued from operation of the gas turbine at certain frequencies.
This objective has been achieved by using an acoustic damper comprising a neck and a damping volume, wherein the neck comprises a mouth being in fluid connection with a chamber that comprises adjacent to the mouth of the neck at least one opening for sealing gas.
The sealing gas, air or any other suitable gas that flows through the at least one opening into the chamber has the effect of a “fence” or a shield that protects the mouth of the damper from grazing flow. In conjunction with the claimed invention grazing flow is the flow of a gas more or less parallel to a wall that comprises the mouth of the damper. This grazing flow has a main or preferred direction more or less perpendicular to the neck of the damper and therefore may disturb the bias flow of gas through the neck and the mouth into the damping volume.
By means of the claimed opening or a number of openings located adjacent to the mouth of a damper the grazing flow is deflected and therefore does not disturb the bias flow through the neck and the mouth of the damper and as a result the performance of the damper is improved.
In a preferred embodiment of the claimed invention the at least one opening for sealing gas is located upstream of the mouth so as to deflect the grazing gas flow away from the mouth of the damper. If this opening is located upstream of the mouth it most efficiently protects the mouth from the grazing gas flow.
To even more efficiently deflect the grazing flow away from the mouth of the damper it may be advantageous to provide two or more openings upstream of the mouth. In embodiments where the preferred direction of the grazing flow may change it is preferred if three, four or even more openings are located around the mouth of the damper so as to deflect the grazing flow independent from its actual direction of flow and to protect the mouth of the damper from the grazing flow.
To optimize the effect of the claimed openings adjacent to the mouth the openings for sealing gas may have a circular, elliptic or square cross section. Of course, the selection of a specific cross section of the openings may be based on the efficiency, i.e. an optimal deflection of the grazing gas flow and little sealing gas consumption. Reducing the flow of sealing gas raises the overall efficiency of a gas turbine, since supplying a sealing gas with a higher pressure than the pressure inside the chamber requires energy.
In principle, any suitable source of a high pressure gas that is available may be used for the aerodynamic shielding of grazing flows according to the invention. In case the damper is a flow through damper the sealing gas that flows through the opening to the chamber may be the similar to that gas that flows through the damper into the chamber.
The claimed invention may be based on any type of acoustic damper, for example a resonator with one or more damping volumes, a half-wave tube a quarter-wave tube, a multi-volume damper, a liner or any kind of acoustic flow-through damper.
The claimed invention also may be applied to dampers with no flow through of the acoustic damper type.
The claimed invention may preferably be applied if the mouth of the damper opens into a combustor chamber, a mixing chamber a plenum and/or an air channel of a gas turbine.
Further advantages and details of the claimed invention are subsequently described in conjunction with the drawings and their description.
The figures show:
The damping device 11 in this exemplary embodiment may be a Helmholtz resonator, but the claimed invention is not limited to this type of acoustic damping device. The claimed invention may be used in conjunction with any type of acoustic damping device like a half-wave tube, a quarter-wave tube and the like. The claimed invention may be used in conjunction with flow through acoustic damping devices and acoustic damping devices without flow through.
As can be seen from
In the chamber 5 more or less parallel to the inner surface 9 a gas flows. This gas has a preferred direction of flow (illustrated by the arrow 19) and is also referred to as grazing flow 19. The preferred direction of this grazing flow 19 is essentially perpendicular to a bias flow 21 between the damping volume 15 and the combustion chamber 5 and disturbs the bias flow 21 through the neck 13. This negative effect of the grazing flow 19 on the bias flow 21 reduces the performance of the damper 11 as has been explained in conjunction with
In
In this embodiment the damper 11 is a flow through damper which means that the damping volume 15 is connected via the neck 13 with the combustion chamber 5. At the opposite end of the damping volume 15 the damping volume 15 is connected via a small bore 23 to a further chamber R1.
As can be seen from
Since the pressure pR1 in the chamber R1 is higher than the pressure p5 in the chamber 5 sealing air flows through the bore 25 and the opening 27 from chamber R1 into chamber 5. Since the bore 23 has a rather small diameter its flow resistance is great and consequently the bore 23 restricts the bias flow 21 through the damper 11.
The resulting pressure difference Δp (=pR1−p5) causes not only the bias flow 21 through damper 11, but a flow 29 of sealing gas through bore 25 and opening 27.
The flow resistance of the tube 23 is greater than the flow resistance of the neck 13. This means that the pressure reduction Δp23 at the bore 23 is greater than the pressure reduction Δp13 at the neck 13 of the damper. In other words: Δp23>Δp13.
This means that the tube 23 due to its small diameter and/or its length acts as a flow restrictor reducing the bias flow 21 through the neck 13.
The chamber R1 may be any high pressure environment, for example the hood or the liner pressure or a reservoir for cooling air. In most appliances of the claimed invention the chamber 5 is the combustion chamber of a gas turbine, but the claimed invention is not restricted to that.
The sealing gas flowing through bore 25 and entering the chamber 5 via opening 27 in a direction more or less perpendicular to the grazing flow 19 it deflects the grazing flow away from the mouth 17 of the damper 11.
As described in conjunction with
The flow resistance of the bore 25 is smaller than the flow resistance of the bore 23. This can be achieved by providing a larger diameter to bore 25 than to bore 23.
Consequently, a gas flow 29, illustrated by an arrow through the bore 25, is far greater than the bias flow 21 although the damper 11 and the bore 25 are supplied from the same chamber R1 with air or gas and open into the same chamber 5.
As can be seen by comparison of the arrows 29 and 19, the velocity of the sealing gas flow through the bore 25 is even higher than the velocity of the grazing flow 19.
The great velocity of the air or gas flow 29 through the bore 25 deflects the grazing flow 19 away from the inner surface 9 and away from the mouth 17 of the damper 11, as is illustrated by the arrow 19.2 in
Doing so, the grazing flow 19 does not reach the mouth 17 of the damper 11 and therefore the bias flow 21 is not disturbed by the grazing flow 19 anymore. Consequently, the efficiency and effectiveness of the damper 11 is high and independent from the grazing flow 19.
Going back to
In
In other words: The mouth 17 is on the leeward side of the “windshield 31” that generated by the flow 29 of air or gas through the bore 25. Since the mouth 17 should be on the leeward side of the windshield 31 in most cases it is preferred that the at least one opening 27 is located upstream of the mouth 17.
On the left side of
Therefore, the bias flow 21 through the mouth 17 is even better protected from the grazing flow.
In
The embodiment 7a) has already been described in conjunction with
In the embodiment illustrated in
In the embodiment illustrated in
According to the embodiment, illustrated in
In
g) illustrates an embodiment with one opening 12 and 27 with a bent cross section.
The embodiment illustrated in
Number | Date | Country | Kind |
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14157239.6 | Feb 2014 | EP | regional |