1. Field of the Invention
Embodiments of the present invention relate generally to thermal control of gas turbine engine turbine disks and, more specifically, controlling heat transfer rate at the turbine disk bore.
2. Description of Related Art
Several types of gas turbine engines include a high pressure rotor having an axial high pressure turbine (HPT) joined to a high pressure compressor (HPC) to form a high pressure rotor. The HPT typically includes one or more connected stages. Each stage includes a row of turbine blades or airfoils extending radially outwardly from an annular outer rim of a turbine disk. A disk web extends radially outwardly from a disk bore to the outer rim of the disk. A single tie bolt or tie rod through a high pressure bore of the high pressure rotor is tightened and secured by a lock-nut used to clamp together and place the high pressure rotor in compression. The disk bore is spaced apart from and circumscribes the tie rod. Such rotors are well known and an example of one is disclosed in U.S. Pat. No. 5,537,814, entitled “High pressure gas generator rotor tie rod system for gas turbine engine”, which issued Jul. 23, 1996, is assigned to the present assignee the General Electric Company, and which is incorporated herein by reference.
During engine acceleration, the outer rim of the second stage turbine disk heats up very rapidly as it is closest to the hot flowpath. The disk bore is much larger and does not heat up as quickly. This difference in temperature from the rim to the bore causes thermally induced stress in the second stage turbine disk. During engine deceleration, the outer rim of the second stage turbine disk cools down rapidly because the air flowing over the disk cools down. During this period, the disk bore remains at a much higher temperature until the entire turbine disk reaches thermal equilibrium. The disk bore is much larger and does not cool down or heat up as quickly as the disk rim. This difference in temperature from the rim to the bore causes thermally induced stress in the second stage turbine disk. Thermal control air is flowed through an annular passage between disk bore and the tie rod.
Thus, there continues to be a need to reduce thermally induced stresses in second stage turbine disks caused by differences in temperature and thermal conditions between the outer rim of the second stage turbine disk and the bore during engine acceleration and deceleration. There continues to be a need to reduce the thermal response time of second stage turbine disk bores relative to the outer rims of the second stage turbine disk during engine acceleration and deceleration.
A gas turbine engine high pressure rotor (12) includes first and second high pressure turbine stages (55, 56) with first and second stage disks (60, 62) having first and second stage disk hubs (154, 156) with first and second stage disk bores (164, 166) therethrough respectively. A single tie rod (170) disposed through the first and second stage disk bores (164, 166). First and second bore annular flowpaths (184, 186) are radially located between the first and second stage disk hubs (154, 156) and the tie rod (170) and a means for increased cooling and/or heating in the second stage disk bore (166) is axially located within the second stage disk bore (166). The first stage bore annular flowpath (184) may include a substantially constant first cross-sectional flow area (200) between the first stage disk hub (154) and the tie rod (170).
The means may include an airflow accelerator (188) axially located within the second stage disk bore (166) such as one or more annular ribs (190) on the tie rod (170). A bore annular cross-sectional flow area (200) between the second stage disk hub (156) and the ribs (190) may be substantially smaller than between the second stage disk hub (156) and the tie rod (170).
An axially unobstructed inlet (206) into the second bore annular flowpath (186) may be used for fully axially flowing and axially unobstructed flowing second stage bore cooling air (180) into the inlet (206). An axially unobstructed outlet (208) out of the second bore annular flowpath (186) may be used for fully axially flowing and axially unobstructed flowing of second stage bore cooling air (180) out of the outlet (208). A converging section (207) of the second bore annular flowpath (186) may be in the inlet (206) and converge in the inlet (206) to a forwardmost plateau (210) of a forwardmost one of the ribs (190). A diverging section (209) of the second bore annular flowpath (186) may be in the outlet (208) and diverge in the outlet (208) aftwardly from an aftwardmost plateau (210) of an aftwardmost one of the ribs (190).
One particular embodiment of the airflow accelerator (188) includes only two of the annular ribs (190) and the two annular ribs (190) being axially unevenly distributed along the tie rod (170) within the second stage disk bore (166). The two annular ribs (190) may be axially located in about a first or upstream half of a bore axial length (218) of the second stage disk bore (166).
Illustrated in
Referring to
Referring to
In the exemplary embodiment of the engine depicted herein, the high pressure turbine 22 includes, in downstream serial flow relationship, first and second high pressure turbine stages 55, 56 having first and second stage disks 60, 62. A first stage nozzle 66 is directly upstream of the first high pressure turbine stage 55 and a second stage nozzle 68 is directly upstream of the second high pressure turbine stage 56. The compressor discharge pressure (CDP) air 76 discharged from the diffuser 42 is used for combustion and to cool components of turbine subjected to the hot combustion gases 28.
Referring to
Referring to
Cooling air apertures 157 in the inner combustor casing 47 allows turbine blade cooling air 80 from the compressor discharge pressure air 76 to flow into an annular cooling air plenum 163 within a plenum casing 158. The blade cooling air 80 is accelerated by a one or more accelerators 165 attached to the plenum casing 158 at an aft end of the cooling air plenum 163. The accelerators 165 inject the blade cooling air 80 into a stage one disk forward cavity 168 through cooling holes 169 in the retainer plate 109. The stage one disk forward cavity 168 is positioned axially between the retainer plate 109 and the disk web 162 of the first stage disk 60. The accelerators 165 inject the blade cooling air 80 at a high tangential speed approaching wheel speed of the first stage disk 60 at a radial position of the accelerator 165. The blade cooling air 80 then flows through the stage one disk forward cavity 168 and cools the first stage disk 60 and the first stage blades 91.
During engine acceleration, the outer rims 101 of the first and second stage disks 60, 62 tend to heat up very rapidly as they are closest to the hot flowpath 110. The cooling air 80 cools the first stage disk 60, the first outer rim 99 and the first stage blades 91 mounted thereupon. Rotor bore cooling air 176 from the rotor bore 172 provides first and second stage bore cooling air 178, 180, and second stage blade cooling air 182. Because rotor bore cooling air 176 is used to cool the first stage disk hub 154 and the second stage blades 92 before cooling the second stage disk hub 156, the rate of thermal response during engine transients such as acceleration and deceleration is faster for the first stage disk hub 154 than for the second stage disk hub 156. The second stage disk hub 156 is much larger and more massive than the second outer rim 101 of the second stage disk 62 and does not heat up or cool down as quickly. This difference in temperature from the rim to the bore causes thermally induced stress in the turbine second stage disk 62 not experienced to the same degree in the first stage disk hub 154. Note that the first and second stage bore cooling air 178, 180 is used to both cool and heat the first and second stage disk hubs 154, 156 respectively.
Referring to
The exemplary airflow accelerator 188 illustrated in
The ribs 190 are axially located well within the second stage disk bore 166 between bore leading and trailing edges 202, 204 of the second stage disk bore 166. This provides an axially unobstructed inlet 206 and an axially unobstructed outlet 208 to and from the second bore annular flowpath 186 respectively within the second stage disk bore 166. The second bore annular flowpath 186 includes a converging section 207 in the inlet 206 that converges in the inlet 206 until it reaches a plateau 210 of a forwardmost one of the rib 190. The second bore annular flowpath 186 includes a diverging section 209 in the outlet 208 that diverges in the outlet 208 from a plateau 210 of the aftwardmost of the ribs 190. The axially unobstructed inlet and outlet 206, 208 provides a fully axial and axially unobstructed flow of the second stage bore cooling air 180 into the inlet 206 and out of the outlet 208 which helps bore heating and cooling. A bore inner surface area 212 and a plateau surface area 214 are cylindrical concentric with respect to each other. The cross-sectional flow area 200 between the second stage disk hub 156 and the tie rod 170 (where there is no rib 190) is less than the cross-sectional flow area 200 between the first stage disk hub 154 and the tie rod 170. The cross-sectional flow area 200 between the first stage disk hub 154 and the tie rod 170 which has no ribs 190 is substantially constant.
During engine acceleration, the outer rim 101 of the second stage disk 62 heats up very rapidly as it is closest to the hot flowpath 110 of the high pressure turbine (HPT) 22. The second stage disk hub 156 of the second stage disk 62 is much larger and does not heat up as quickly. This difference in temperature from the rim to the hub causes thermal stress in the disk. The airflow accelerator 188 alleviates this thermal stress by heating up the second stage disk hub 156 faster by reducing the cross-sectional flow area 200 between the second stage disk hub 156 and the one or more ribs 190 on the tie rod 170. This causes the velocity of the second stage bore cooling air 180 in the second bore annular flowpath 186 to increase under the disk which causes a better heat transfer coefficient and an increased rate of heat transfer to the disk hub.
During engine deceleration, the outer rim 101 of the second stage disk 62 cools down rapidly and the second stage disk hub 156 of the second stage disk 62 remains at it's increased temperature. This difference in temperature from the rim to the hub causes thermal stress in the disk in the opposite direction to thermal stress caused by engine acceleration. During engine deceleration, the second stage bore cooling air 180 cools down from level before the engine deceleration. The airflow accelerator 188 alleviates this thermal stress by cooling down the second stage disk hub 156 faster by reducing the cross-sectional flow area 200 between the second stage disk hub 156 and the one or more ribs 190 on the tie rod 170. This causes the velocity of the second stage bore cooling air 180 to increase under the second stage disk hub 156 producing a better heat transfer coefficient and an increased rate of heat transfer from the disk hub to the second stage bore cooling air 180.
While there have been described herein what are considered to be preferred and exemplary embodiments of the present invention, other modifications of the invention shall be apparent to those skilled in the art from the teachings herein and, it is therefore, desired to be secured in the appended claims all such modifications as fall within the true spirit and scope of the invention. Accordingly, what is desired to be secured by Letters Patent of the United States is the invention as defined and differentiated in the following claims.
The present application claims priority to U.S. Provisional Patent Application Ser. No. 61/639,429, entitled “AIR ACCELERATOR ON TIE ROD WITHIN TURBINE DISK BORE”, filed Apr. 27, 2012, the disclosure of which is hereby incorporated by reference.
Filing Document | Filing Date | Country | Kind |
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PCT/US13/38330 | 4/26/2013 | WO | 00 |
Number | Date | Country | |
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61639429 | Apr 2012 | US |