Abstract:
A gas turbine has a compressor providing compressed air, a combustion chamber provided with a burner, and an expansion turbine, wherein a bypass flow channel is also provided designed to supply compressed air past the burner and to supply a hot gas flow generated in the combustion chamber during operation of the gas turbine. The opening cross section of the bypass flow channel can be adjusted, and an adjustment unit is designed to adjust the opening cross section of the bypass flow channel such that the modification speed of the opening cross section is selected such that the relative combustion chamber pressure drop or a material temperature of the combustion chamber is substantially constant, in particular that the relative combustion chamber pressure drop or the material temperature of the combustion chamber does not vary by more than 10%.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
       [0001]    This application is the US National Stage of International Application No. PCT/EP2014/072703 filed Oct. 23, 2014, and claims the benefit thereof. The International Application claims the benefit of European Application No. EP13190849 filed Oct. 30, 2013. All of the applications are incorporated by reference herein in their entirety. 
     
    
     FIELD OF INVENTION 
       [0002]    The present invention relates to a method for operating at partial load a gas turbine which comprises a compressor for providing compressor air, a combustion chamber provided with a burner, and an expansion turbine, a bypass flow channel furthermore being provided, which is configured in order to deliver compressor air past the burner and to a hot gas flow generated in the combustion chamber during gas turbine operation. The present invention also relates to such a gas turbine. 
       BACKGROUND OF INVENTION 
       [0003]    Gas turbines can typically be operated only in a restricted way in their power range toward the lower partial load ranges because of limit value requirements for the CO emission quantities. This is because, when the partial load operation is reduced to lower powers, the primary zone temperature of the combustion typically decreases continuously. When this primary zone temperature falls below a temperature limit value typical of a gas turbine, the amount of CO emission increases, sometimes exponentially, since the combustion of CO to form CO 2  can no longer take place to a sufficient extent. When predetermined limit values are reached, the partial load operation must therefore be restricted to lower powers in order not to violate the CO emission limit values. Such a restriction likewise has an effect on the operation of a steam turbine system coupled to such a gas turbine (in the sense of a Combined Cycle Power Plant, CCPP), since a power reduction possibly desired by the operator is not to be reached below a limit value. 
         [0004]    Because of compliance with predetermined CO emission limit values, a power plant operator is thus obliged to periodically turn off the gas turbine, or a steam power plant system coupled to this gas turbine, or remain in a partial load range which lies above the technically possible minimum power. 
         [0005]    There is consequently a technical requirement to provide a gas turbine, or a method for operating such a gas turbine, making it possible to reduce the partial load range further without simultaneously exceeding CO emission limit values. In other words, the partial load range of the gas turbine is intended in particular to be extended downward while complying with CO emission limit values. Above all, this partial load range should be provided below the otherwise technically available load range which can be achieved by suitable guide vane adjustment (so-called guide vane adjustment range). 
         [0006]    One solution approach for these technical requirements may be specified by the publications US 2010/0175387 A1 and U.S. Pat. No. 5,537,864. In these documents, it is proposed to adjust the amount of air blown out from the compressor by suitable control by means of a bypass flow channel, in such a way that the primary zone temperature does not change substantially. Since the primary zone temperature itself cannot be measured directly, however, these controls always rely on predetermined assumptions, or estimates. 
         [0007]    At this point, it should be pointed out that the primary zone temperature (TPZ) is an average temperature determined from the energy balance around the burner and flame, which describes the thermodynamic state of the hot gas after completed chemical reaction. The TPZ therefore correlates with the proportion of CO in the combustion gases. 
         [0008]    It is therefore desirable to provide a more highly developed method which can avoid the above-mentioned problems of the prior art, and at the same time can provide reference quantities that can be metrologically recorded better. 
       SUMMARY OF INVENTION 
       [0009]    Objects of the invention are achieved by a method as claimed , as described above and below, for operating such a gas turbine, and by a gas turbine as claimed as described below. 
         [0010]    In particular, these objects of the invention are achieved by a method for operating at partial load a gas turbine which comprises a compressor for providing compressor air, a combustion chamber provided with a burner, and an expansion turbine, a bypass flow channel furthermore being provided, which is configured in order to deliver compressor air past the burner and to a hot gas flow generated in the combustion chamber during gas turbine operation, and the opening cross section of the bypass flow channel furthermore being adjustable by a setting means, which comprises the following steps:—operating the gas turbine at partial load;—adjusting the opening cross section of the bypass flow channel so that the variation rate of the opening cross section is selected in such a way that the relative combustion chamber pressure loss or a material temperature of the combustion chamber is essentially constant, in particular that the relative combustion chamber pressure loss or the material temperature of the combustion chamber does not vary by more than 10%. 
         [0011]    Objects of the invention are furthermore achieved by a gas turbine suitable for carrying out a method as presented above and below, which comprises a compressor for providing compressor air, a combustion chamber provided with a burner, and an expansion turbine, a bypass flow channel furthermore being provided, which is configured in order to deliver compressor air past the burner and to a hot gas flow generated in the combustion chamber during gas turbine operation, and the opening cross section of the bypass flow channel furthermore being adjustable by a setting means, which furthermore comprises an adjustment unit, which is configured in order to adjust the opening cross section of the bypass flow channel in such a way that the variation rate of the opening cross section is selected in such a way that the relative combustion chamber pressure loss or a material temperature of the combustion chamber is essentially constant, in particular that the relative combustion chamber pressure loss does not vary by more than 10%. 
         [0012]    The adjustment unit is in this case advantageously configured as a regulating unit, although it may also be configured as a control unit. The adjustment unit in this case allows automatic adjustment of the variation rate of the opening cross section, or of the opening cross section. 
         [0013]    It should be pointed out that the relative combustion chamber pressure loss can be determined as the ratio of the combustion chamber differential pressure and the compressor final pressure. In this case, the combustion chamber differential pressure is given by a difference of two static pressures, which are determined at different measurement positions on or in the combustion chamber. Typically, one pressure determination is determined before the burner, or in the region of the burner, and one pressure value inside the combustion chamber, for instance at the end of the combustion zone. The pressure difference of the two pressure values determined is related by taking the ratio to the compressor final pressure, which, as the name already says, describes the static pressure at the end of the compressor and can likewise be recorded metrologically. 
         [0014]    It should likewise be pointed out that that the combustion chamber material temperature according to the invention relates to a material temperature which can be recorded metrologically directly or indirectly. Such a temperature is, in particular, a temperature of the combustion chamber wall, a temperature of the combustion chamber tiles, or for instance a temperature of a flame tube component which the combustion chamber also comprises. 
         [0015]    The provision of a bypass flow channel as described above in a gas turbine is already known from the prior art. For example, DE 43 39 724 C1 describes a gas fitting which has a common wall between a compressor outlet and a turbine outlet. This wall has a slider which covers corresponding slots in this wall. The slots are in this case to be understood in the sense of a bypass flow channel. The slots can be adjusted variably in terms of their opening cross section by actuating the slider. According to the teaching of DE 43 39 724 C1, provision is made to adjust the slots according to the gas turbine power, so as to keep the mass flow rate in the turbine at a suitable order of magnitude. In the event of load shedding, in order to avoid automatic acceleration of the gas turbine, the slots can be moved approximately immediately into a final position, for instance by suitable actuation, so as to avoid bypassing of the burner by the compressor air. The operating mode described in DE 43 39 724 C1, however, is intended exclusively for power regulation and therefore does not allow operation which is carried out in accordance with CO emission limit values. 
         [0016]    At this point, it should be pointed out that the disclosure of DE 43 39 724 C1 is incorporated into the present application by explicit reference. 
         [0017]    Adjustment of the opening cross section of the bypass flow channel can now ensure that an operating mode complying with CO emission limit values can be achieved in the event of partial load operation. In this case, for instance, the opening cross section of the bypass flow channel may be varied as a function of time so that the variation rate of the opening cross section is selected in such a way that the primary zone temperature is essentially constant. Advantageously, the primary zone temperature in this case remains essentially constant below the gas turbine power range determined by the guide vane adjustment range. When the minimum guide vane adjustment range is reached, the primary zone temperature thus typically still lies above a temperature below which a significant increase in the CO emission values is to be expected. Suitable estimates of this temperature are known from the prior art. 
         [0018]    On the basis of such thermal estimates, or suitable calculation methods, the opening cross section of the bypass flow channel can also be calculated in the event of partial load powers which lie in particular below the gas turbine power range determined by the guide vane adjustment range, in which case an essentially constant primary zone temperature may for instance be ensured as a boundary condition. Such estimates or calculation methods may sometimes also be based on test measurements. If partial load operation is now reduced to lower values, according to the invention a continuous adjustment of the opening cross section of the bypass flow channel to larger values is carried out, so that an increasing pressure equalization between the downstream region of the bypass flow channel (combustion chamber) and the upstream region of the bypass flow channel (compressor air plenum) results. 
         [0019]    As a consequence of this, the pressure difference which determines the flow rate of the compressor air through the burner is also reduced. At the same time—varying depending on the embodiment of the gas turbine—it is also possible to modify the cooling power for the combustion chamber cooling, which results for instance because of the flow of compressor air into cooling channels of the combustion chamber for cooling hot gas parts in the combustion chamber. At this point, the gas turbine of the type SGT X-200E of the Applicant is to be mentioned in particular, in which such cooling channels are provided as cooling air bores for cooling the flame tube bottoms by impact cooling (see also, for instance, DE 43 39 724 C1). 
         [0020]    Because of the reduction of the pressure of the compressor air flow delivered to the combustion chamber, there is also a reduction in the cooling power of the hot gas parts in the combustion chamber. If the thermal loads for the hot gas parts of the combustion chamber now become too great because of the reduced cooling, material damage and failure of individual components is to be expected. In order to anticipate such a development, it is now proposed according to the invention to carry out an adaptation of the variation rate of the opening cross section of the bypass flow channel, specifically in such a way that the relative combustion chamber pressure loss or a material temperature of the combustion chamber is used as an adjustment quantity. By an essentially constant relative combustion chamber pressure loss, the flow rate of the compressor air for cooling the hot gas parts in the combustion chamber is likewise kept essentially constant. This results in an essentially constant cooling rate, so that it is possible to avoid an increase of the temperatures to which the hot gas parts in the combustion chamber are exposed. 
         [0021]    According to one embodiment, it is proposed to operate a gas turbine by a method for operating the gas turbine at partial load with the following steps:—operating the gas turbine ( 100 ) at partial load;—adjusting the opening cross section (Q) of the bypass flow channel ( 10 ) so that the variation rate (V) of the opening cross section (Q) is selected in such a way that the primary zone temperature (TPZ) is essentially constant, and in particular does not vary by more than 10%. This is intended in particular to be carried out in the event of a reduction of the partial load, and specifically initially until the thermal loads for the hot gas parts of the combustion chamber become too great. Subsequently, provision may be made to operate the gas turbine by a method as claimed, so that the resulting cooling power in the combustion chamber, or at the hot gas parts in the combustion chamber, is essentially constant. According to this embodiment, the primary zone temperature is thus initially used as a suitable adjustment quantity, the relative combustion chamber pressure loss or the material temperature of the combustion chamber being used as a further adjustment quantity after reaching a temperature limit value not further to be exceeded. By the combined mode of operation, or the respective individual modes of operation, it is ensured that the CO emission values can be kept essentially constant, or lie below predetermined CO limit values. 
         [0022]    The variation rate of the opening cross section of the bypass flow channel is thus adapted in the course of the partial load operation in such a way that a reduction of the partial load below system-specific limit values (for instance determined by the guide vane adjustment range) can be made possible. 
         [0023]    According to the invention, it is possible to carry out the variation of the opening cross section of the bypass flow channel as a continuous and/or stepwise variation over time, the respective variations being carried out in such a way that the underlying adjustment quantities (for instance relative combustion chamber pressure loss) remain essentially constant, but in particular do not vary by more than 10%. The respective variations to be carried out may, in the case of a discrete variation, be stored in the scope of interpolation points in an adjustment unit, which then if need be cause a suitable variation of the opening cross section. The variation rate of the opening cross section is in this case to be understood as a time average over the individual discrete interpolation points. 
         [0024]    According to a first embodiment of the invention, a first method for operating the gas turbine at partial load with the following steps is carried out during a first time period:—operating the gas turbine ( 100 ) at partial load;—adjusting the opening cross section (Q) of the bypass flow channel ( 10 ) so that the variation rate (V) of the opening cross section (Q) is selected in such a way that the primary zone temperature (TPZ) is essentially constant, and in particular does not vary by more than 10%. The method as claimed is carried out during a second time period, in particular with the second time period directly following the first time period. As already explained above in detail, in this way it is possible to achieve a particularly efficient operating mode of the gas turbine at partial load, which allows CO-compliant operation even in very low partial load ranges. According to one embodiment, it is particularly advantageous for the partial load to be reduced in this case over the time periods, and in particular reduced over the two time periods. 
         [0025]    According to another embodiment of the method according to the invention, the method for operating the gas turbine at partial load with the following steps:—operating the gas turbine ( 100 ) at partial load;—adjusting the opening cross section (Q) of the bypass flow channel ( 10 ) so that the variation rate (V) of the opening cross section (Q) is selected in such a way that the primary zone temperature (TPZ) is essentially constant, and in particular does not vary by more than 10%, is carried out during a first time period until a first thermal characteristic reaches a predetermined first limit value, in particular with this being followed by a second time period during which a method as claimed is carried out. The first thermal characteristic is in this case, in particular, a measure of the cooling power at hot gas parts of the combustion chamber. To this extent, when a thermal limit value (first limit value) is exceeded, more reliable operation of the gas turbine is achieved even with still low partial load powers than during the first time period, without exceeding CO emission limit values. 
         [0026]    According to another method, the method as claimed is carried out with a partial load reduction until a second thermal characteristic reaches a predetermined second limit value, in particular with the variation of the opening cross section then being selected in such a way that the opening cross section is reduced, in particular reduced stepwise. Such a method-technology precaution may sometimes be necessary since the relative combustion chamber pressure loss is dependent on the ambient conditions, and a sufficient cooling power of the hot gas parts of the combustion chamber cannot therefore always be ensured, for instance when the ambient temperatures are very high. If a sufficient cooling power is not then provided despite a continuous or stepwise increase of the opening cross section of the bypass flow channel, a second limit value of a second thermal characteristic may be exceeded. The thermal characteristic is in particular a suitable adjustment quantity which records the thermal loading the combustion chamber, and therefore ensures thermally reliable operation of the gas turbine. A suitable characteristic quantity for this thermal load may, for example, be a measured material temperature (advantageously in the combustion chamber), which has been recorded directly or indirectly by means of a thermocouple, or a substitute characteristic, for example the relative combustion chamber pressure loss or another suitable thermal quantity. 
         [0027]    If the second limit value is now reached by the second thermal characteristic, the opening cross section of the bypass flow channel is reduced. This reduction is advantageously carried out in steps of about 10% of the overall range. As a result of this, the cooling air flow rate increases again and the hot gas parts of the combustion chamber are supplied with more cooling power. According to one embodiment, this process with a stepwise variation may in particular be repeated until the second thermal characteristic reaches a value above a further third thermal limit value. 
         [0028]    According to one refinement of the method according to this embodiment, in the event of a reduction of the opening cross section and when a third thermal predetermined limit value is reached by the second thermal characteristic, the variation of the opening cross section is selected in such a way that the opening cross section is increased again, in particular increased again stepwise. A stepwise increase may in this case advantageously be carried out in steps of about 10% of the overall range. Owing to the hysteresis thus carried out of initially a reduction and then subsequently an increase of the opening cross section of the bypass flow channel again, stable regulation of the gas turbine operation can be achieved. 
         [0029]    According to one embodiment of the method according to the invention, the method is carried out below the guide vane adjustment range. As a result of this, as explained above, the partial load power range can be reduced further, but without the risk of exceeding CO limit values. In this way, the flexibilizaton of the gas turbine operation can be improved significantly. 
         [0030]    According to a first embodiment of the gas turbine according to the invention, it furthermore comprises a regulating circuit and a measurement probe, the measurement probe being configured in order to record a thermal characteristic and the regulating circuit being configured in order, in the event of a partial load reduction and when a predetermined limit value (second limit value) of the thermal characteristic (second thermal characteristic) is reached, the variation of the opening cross section is selected in such a way that the opening cross section is reduced again, in particular reduced stepwise. 
         [0031]    As already mentioned above, stable regulation of the gas turbine can be achieved in this way, and at the same time the dependency of the relative combustion chamber pressure loss on the ambient conditions can be taken into account. Likewise, protection of hot gas parts of the combustion chamber by sufficient cooling can be ensured at the same time. 
         [0032]    According to another embodiment of the gas turbine according to the invention, the gas turbine is configured in such a way that the compressor air delivered to the burner is provided at least partially in order to cool hot gas parts of the combustion chamber, in particular flame tube bottoms, by means of feeding through cooling channels in the combustion chamber. By the provision of cooling channels in the combustion chamber, particularly when carrying out the method as claimed, a sufficient cooling power can be ensured. Overheating and consequent damage to hot parts of the combustion chamber can therefore be prevented. 
         [0033]    The invention will be described in detail below with the aid of individual figures. In this case, technical features which have the same references have the same technical effects. 
         [0034]    It should likewise be pointed out that the following figures are to be interpreted merely schematically, and no restriction in respect of the implementability of the invention may be based thereon. 
         [0035]    It should likewise be pointed out that the technical features explained below are claimed in any combination with one another so long as the combination can achieve the object of the invention. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0036]      FIG. 1  shows a schematic representation of the variation of the primary zone temperature (TPZ) as a function of the relative gas turbine power (AGTP) with a fully closed and open opening cross section of the bypass flow channel; 
           [0037]      FIG. 2  shows a diagrammatic representation of the relative opening cross section (RQ) as a function of the corrected turbine output temperature (OTC) below the guide vane adjustment range (LSVB) corresponding to suitable embodiments of the operating mode according to the invention at partial load; 
           [0038]      FIG. 3  shows a functional profile of the second thermal characteristic (TK 2 ) as a function of time (t) during operation to reduce the partial load power when reaching a second limit value (GW 2 ) and a third limit value (GW 3 ); 
           [0039]      FIG. 4  shows an embodiment of the method according to the invention as claimed in a flowchart representation; 
           [0040]      FIG. 5  shows an embodiment of a gas turbine according to the invention in perspective lateral sectional view; 
           [0041]      FIG. 6  shows a simplified schematic partial sectional view of the gas turbine shown in  FIG. 5 . 
       
    
    
     DETAILED DESCRIPTION OF INVENTION 
       [0042]      FIG. 1  shows a diagrammatic representation of the profile of the primary zone temperature TPZ (in ° C.) as a function of the relative gas turbine power AGTP (in %). In this case, two fundamentally different modes of operation of the gas turbine are represented, namely one with a fully closed bypass flow channel (operating mode  200 ) and one with a fully open bypass flow channel (operating mode  210 ). A flatter profile in the region of the guide vane adjustment range LSVB over which the gas turbine can be operated with conventional partial load operation by suitable adjustment of the guide vanes in the guide vane adjustment range LSVB at different partial load powers, can be seen clearly for the two operating modes  200  and  210 . Support of the partial load operation below this guide vane adjustment range LSVB by adjusting the guide vanes is, however, no longer possible. The ranges available to the invention preferably relate to these ranges lying below. They consequently lie between the range  200  with a closed bypass flow channel and the range  210  which represents an operating mode with an open bypass flow channel. 
         [0043]    For example,  FIG. 1  represents two points  220 ,  230  which are used to illustrate further operating points. The operating point  220  represents an operating state with a minimum guide vane guide vane adjustment range, which, with a partially open bypass flow channel, reaches the primary zone temperature TPZ as exists for instance with a basic load. In contrast thereto, the operating point  230  represents an operating state which likewise reaches the primary zone temperature TPZ for a basic load, but does so with a fully open bypass flow channel. The operating point  230  is, however, significantly below the technically possible minimum guide vane adjustment range LSVB in terms of the relative gas turbine power. 
         [0044]      FIG. 2  represents the functional profile of the relative opening cross section RQ as a function of the corrected turbine output temperature OTC. The relative opening cross section RQ relates to the ratio of the existing, i.e. adjusted, opening cross section Q to the maximum possible opening cross section. In this case, the operating mode represented has, below the guide vane adjustment range LSVB, a control curve which has a plurality of interpolation points. With a decreasing corrected turbine output pressure OTC, i.e. with a decreasing partial load power, during a first time period ZA 1  an operating mode is initially selected which requires the adjustment of the opening cross section Q of the bypass flow channel  10  to be carried out in such a way that the variation rate V of the opening cross section Q is selected so that the primary zone temperature TPZ is essentially constant, and in particular does not vary by more than 10%. During this first time period ZA 1 , an essentially constant primary zone temperature TPZ can therefore be ensured, so that the CO emission values can be kept above particular limit values not to be exceeded. 
         [0045]    During a second time period ZA 2 , which directly follows the first time period ZA 1 , the operating mode is modified in such a way that it is now carried out according to an embodiment as claimed. In this case, for the gas turbine, the adjustment of the opening cross section Q of the bypass flow channel  10  is carried out in such a way that the variation rate V of the opening cross section Q is selected so that the relative combustion chamber pressure loss ABDV or the material temperature MT of the combustion chamber  4  is essentially constant, and in particular so that the relative combustion chamber pressure loss ABDV or the material temperature MT does not vary by more than 10%. According to this operating mode, it is possible to ensure that a sufficient cooling power for hot gas parts in the combustion chamber is still available, and thermal damage to these components can thus be prevented, while complying with the CO emission limit values. 
         [0046]    The further interpolation points, or operating states, shown in the representation respectively relate to interpolation points, or operating states, respectively known from the prior art, and not to be explained further. 
         [0047]    The corrected turbine output temperature OTC given in  FIG. 2  corresponds to the turbine output temperature corrected in relation to the air temperature, as is explained in detail for example in EP 1 462 633 A1. 
         [0048]      FIG. 3  shows a variation, carried out in the event of partial load reduction, of the second thermal characteristic TK 2  as a function of time. In this case, it is shown that initially at small times the partial load reduction also entails a reduction of the second thermal characteristic TK 2 . When a predetermined second limit value GW 2  is exceeded, however, the variation of the cross section Q of the bypass flow channel  10  is selected in such a way that the opening cross section Q is now reduced, in particular reduced stepwise. The stepwise reduction is in this case indicated by the variation profile AQ of the opening cross section Q. Thus, a reduction of the opening cross section Q by two steps is initially carried out, so that the profile of the thermal characteristic TK 2  is again raised above the second limit value GW 2 . After two stepwise reductions of the opening cross section Q, the profile of the second thermal characteristic TW 2  reaches a third predetermined limit value GW 3 , which now requires the opening cross section Q to be increased again, in particular increased again stepwise. In the present case, the increase of the opening cross section Q again takes place in two steps of comparable size to the previous two steps, so that the resulting opening cross section Q corresponds to the opening cross section Q which there was before initiation of the stepwise variations. This leads to a stabilization of the strongly decreasing thermal characteristic and therefore a stabilization of the operation of the gas turbine  100  at partial load. The variations of the opening cross section Q according to the variation profile AQ are in this case carried out by an adjustment unit  20 , which instigates the corresponding adaptations. 
         [0049]      FIG. 4  shows an embodiment of the method according to the invention as claimed, which comprises the following steps:—operating the gas turbine  100  at partial load (first method step  400 );—adjusting the opening cross section Q of the bypass flow channel  10  so that the variation rate V of the opening cross section Q is selected in such a way that the relative combustion chamber pressure loss ABDV or the material temperature MT of the combustion chamber  4  is essentially constant, in particular that the relative combustion chamber pressure loss ABDV or the material temperature MT of the combustion chamber  4  does not vary by more than 10% (second method step  410 ). 
         [0050]      FIG. 5  shows a perspective partial sectional view through a gas turbine  100  according to the invention, which essentially corresponds to the model SGT5-2000E sold by the Applicant. Besides a compressor  1  and an expansion turbine  5 , the gas turbine  100  in this case comprises a combustion chamber  4  provided with a plurality of burners  3 . During operation of the gas turbine  100 , compressor air  2  is delivered laterally from the compressor  1  on the outside of the combustion chamber  4  to the burners  3 . Because of the static pressure difference between the combustion chamber  4  and the pressure of the compressor air  2  fed to the outside of the combustion chamber  4 , cooling air taken from this compressor air  2  flows through cooling channels  7  into the combustion chamber  4 . The rest of the compressor air  2  is then fed to the burners  3  and burnt with a suitable fuel. The combustion products are discharged from the combustion chamber  4  as a hot gas flow  6  and fed to the expansion turbine  5  to perform mechanical work. 
         [0051]    The gas turbine  100  represented has a bypass flow channel  10  (not further shown in detail), which is configured in order, during operation of the gas turbine  100 , to deliver compressor air  2  past the burner  3  and to a hot gas flow  6  generated in the combustion chamber  4 , in which case the opening cross section Q of the bypass flow channel  10  can furthermore be adjusted by a setting means  11 . This setting means  11  is also not shown in detail here. 
         [0052]      FIG. 6  shows a schematic side view through the embodiment of the gas turbine  100  as shown in  FIG. 5 , which represents both the bypass flow channel  10  and the setting means  11  for adjusting the opening cross section Q of the bypass flow channel  10 . During operation of the gas turbine  100 , compressor air  2  is initially delivered from a compressor  1  (not further shown) to the combustion chamber  4 . The compressor air  2  is in this case fed to the burners  3  through a volume between the combustion chamber  4  and an outer wall  8 . In this case, the compressor air  2  flows past the bypass flow channel  10 , which has an opening cross section Q and fluidically connects the region between the combustion chamber  4  and the outer wall  8  to the combustion chamber  4  itself. The opening cross section Q can be adjusted by a slider configured as a setting means  11  (more detailed remarks about this technology may be found in DE 43 39 724 C1). The flow of the compressor air  2  is consequently divided at the opening cross section Q, one part flowing further to the burners  3  of the combustion chamber  4 , but another part flowing through the opening cross section Q into the combustion chamber  4  for pressure equalization. 
         [0053]    The flow of compressor air  2  fed to the burners  3  is furthermore reduced in that a part of this compressor air  2  can flow through cooling channels  7  (not further shown) into the combustion chamber  4  and in this case cool hot gas components (not further shown), in particular flame tube bottoms, of the combustion chamber  4 . The cooling power is in this case proportional to the static pressure difference existing at the cooling channels. 
         [0054]    The gas turbine  100  furthermore has an adjustment unit  20 , which comprises a regulating circuit  30  that is configured for suitable adjustment of the opening cross section Q of the bypass flow channel  10 . The gas turbine  100  likewise has a measurement probe  40 , which records a thermal characteristic (for example the turbine output temperature) and communicates the measurement value to the adjustment unit  20 , or the regulating circuit  30 . The gas turbine  100  likewise has a second measurement probe  50  arranged in the combustion chamber  4 , which is configured in order to metrologically record the material temperature MT of the combustion chamber  4  and to communicate the measurement value to the adjustment unit  20 , or the regulating circuit  30 . The adjustment unit  20  ensures that the opening cross section Q of the bypass flow channel  10  is adjusted in such a way that the variation rate V of the opening cross section Q is selected so that the primary zone temperature TPZ is essentially constant, and in particular does not vary by more than 10%, or that the variation rate V of the opening cross section Q is selected so that the relative combustion chamber pressure loss ABDV of the material temperature MT of the combustion chamber  4  is essentially constant, in particular so that the material temperature MT of the combustion chamber  4  does not vary by more than 10%. 
         [0055]    Further embodiments may be found in the dependent claims.