Centrifugal compressors are commonly used for fluid compression in rotating machines such as, for example, a gas turbine engine. Gas turbine engines typically include at least a compressor section, a combustor section, and a turbine section. In general, during operation, air is pressurized in the compressor section and is mixed with fuel and burned in the combustor section to generate hot combustion gases. The hot combustion gases flow through the turbine section, which extracts energy from the hot combustion gases to power the compressor section and other gas turbine engine loads.
A centrifugal compressor is a device in which a rotating rotor or impeller delivers air at relatively high velocity by the effect of centrifugal force on the gas within the impeller. The impeller typically comprises a plurality of vanes circumferentially spaced about a hub. Centrifugal impellers have complex three-dimensional flow structures due to turning of the flow in both the tangential and radial dimensions. Improvements to impeller geometries are desirable to increase impeller efficiency and uniformity of the gas flow exiting the impeller.
According to some aspects of the present disclosure, a centrifugal impeller comprises a hub and a plurality of circumferentially spaced vanes. The hub has a flowpath surface and an axis of rotation. The plurality of circumferentially spaced vanes extend from the flowpath surface, each of the vanes having a pressure-side fillet and a suction-side fillet extending from a leading edge to a trailing edge of the vane. Each of the pressure-side fillet and suction-side fillet intersect the flowpath surface at a runout. The runout of the pressure-side fillet of a first vane is asymmetric to the runout of the suction-side fillet of the first vane.
In some embodiments the runout of the pressure-side fillet of a first vane is asymmetric to the runout of the suction-side fillet of an adjacent second vane. In some embodiments the runout of the pressure-side fillet of a first vane is asymmetric to the runout of the pressure-side fillet of an adjacent second vane. In some embodiments the runout of the pressure-side fillet of a first vane is asymmetric to the runout of the suction-side fillet of an adjacent second vane.
In some embodiments the runout of the pressure-side fillet of a first vane is asymmetric to the runout of the suction-side fillet of the first vane for a first portion of the length of the first vane, and wherein the runout of the pressure-side fillet of a first vane is symmetric to the runout of the suction-side fillet of the first vane for a second portion of the length of the first vane. In some embodiments the first portion is proximate an impeller discharge. In some embodiments a maximum asymmetry between the runout of the pressure-side fillet and the runout of the suction-side fillet is proximate the impeller discharge. In some embodiments a maximum asymmetry between the runout of the pressure-side fillet and the runout of the suction-side fillet is at a meridional position of 1.0.
In some embodiments the first portion is proximate a knee of the impeller. In some embodiments a maximum asymmetry between the runout of the pressure-side fillet and the runout of the suction-side fillet is proximate the knee. In some embodiments a maximum asymmetry between the runout of the pressure-side fillet and the runout of the suction-side fillet is at a meridional position of 0.5.
In some embodiments the centrifugal impeller further comprises a splitter vane disposed between the first vane and the second vane, the splitter vane extending from a knee of the impeller to a discharge of the impeller, the splitter vane having a pressure-side fillet and a suction-side fillet extending from a leading edge to a trailing edge of the splitter vane. In some embodiments the runout of the pressure-side fillet of the first vane is asymmetric the runout of the pressure-side fillet of the splitter vane. In some embodiments the runout of the pressure-side fillet of the first vane from the knee to the discharge of the impeller is symmetric to the runout of the pressure-side fillet of the splitter vane.
According to aspects of the present disclosures, a centrifugal impeller comprises a hub having a flowpath surface and an axis of rotation; and a plurality of circumferentially spaced vanes extending from the flowpath surface. Each of the vanes have a pressure-side fillet and a suction-side fillet extending from a leading edge to a trailing edge of the vane. A line at an intersection of the flowpath surface and the fillet along either the pressure side or the suction side of a first vane is non-parabolic.
In some embodiments the line at the intersection of the flowpath surface and the fillet along either the pressure side or the suction side of a first vane comprises a plurality of curves having differing foci.
According to further aspects of the present disclosure, a centrifugal impeller comprises a hub having a flowpath surface and an axis of rotation; and a plurality of circumferentially spaced vanes extending from the flowpath surface. A meridional cross-section of the hub comprises a flowpath surface that is non-axisymmetric about the axis of rotation of the hub.
In some embodiments the meridional cross-section is taken at a meridional position of 0.3. In some embodiments the meridional cross-section is taken at a meridional position of 0.5. In some embodiments the meridional cross-section is taken at a meridional position of 1.0.
The following will be apparent from elements of the figures, which are provided for illustrative purposes.
While the present disclosure is susceptible to various modifications and alternative forms, specific embodiments have been shown by way of example in the drawings and will be described in detail herein. It should be understood, however, that the present disclosure is not intended to be limited to the particular forms disclosed. Rather, the present disclosure is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the disclosure as defined by the appended claims.
For the purposes of promoting an understanding of the principles of the disclosure, reference will now be made to a number of illustrative embodiments in the drawings and specific language will be used to describe the same.
The present disclosure is directed to improvements in the three-dimensional structure of a centrifugal impeller to increase impeller efficiency and uniformity of the gas flow exiting the impeller. Although the bulk flow of gas within the impeller largely follows the contours of the impeller vanes, many centrifugal impellers have significant secondary flow (such as cross-flow) due to high streamwise curvature in multiple planes and a long running length of the impeller. Reducing secondary flows may reduce losses in the impeller owed to such secondary flows and also improve uniformity of flow exiting the impeller. More specifically, the present disclosure is directed to a centrifugal impeller having a non-axisymmetric flowpath surface tailored to reduce vane-to-vane secondary flows in the impeller.
Each vane 102 extends from a leading edge 147 (shown on
A fillet 119 is provided on both the pressure side 111 and suction side 113 to smoothly transition between the vane 102 and hub 104. The fillet 119 of the pressure side 111 (i.e. the pressure-side fillet) and the fillet 119 of the suction side 113 (i.e. the suction-side fillet) may each extend from the leading edge 147 to the trailing edge 148 of the vane. Each fillet 119 has a runout 120 defined at the intersection of the fillet 119 and the flowpath surface 115. The runout 120 thus comprises a line extending along the length of the fillet 119.
The hub 104 comprises an outwardly facing surface referred to as the flowpath surface 115. The flowpath surface 115 may face predominantly radially outward proximate an impeller inlet 122 (shown in
As shown in
During operation, the impeller 100 is rotated at relatively high speeds about the axis of rotation. A fluid, typically air, is supplied at the impeller inlet 122 and flows through the fluid flowpath 108 to the impeller discharge 124.
Bulk flow of the fluid through the fluid flowpath 108 is, in
The predominant secondary flow 125 is shown flowing from the lower pressure side 111 of a vane 102 toward the lower suction side 113 of an adjacent vane 102, along the flowpath surface 115. The predominant secondary flow 125 is then directed by the adjacent vane 102 in a radially outward direction and flows along the adjacent vane 102 toward the shroud 106. The predominant secondary flow 125 is then directed circumferentially along the shroud 106. This pattern of predominant secondary flow 125 may create substantially cross flow between the vanes 102 of an impeller 100.
As shown in
Similarly,
An axisymmetric flowpath surface 115 such as that described with respect to
In the illustrated embodiment, the flowpath surface 731 extends linearly from the runout 120 of a fillet 119 on the pressure side 111 of a vane 102 to the runout 120 of a fillet 119 on the suction side 113 of an adjacent vane 102. The flowpath surface 731 may extend between the runouts 120 in a curvilinear or parabolic shape when viewed as a cross-section taken normal to the axis of rotation.
The runout 120 of the fillet 119 on the pressure side 111 is higher, or further from the axis of rotation, than the runout 120 of the fillet 119 on the suction side 113 of the adjacent vane 102. The runout 120 of the fillet 119 may be higher, or further from the axis of rotation, than an axisymmetric flowpath surface 115 proximate the pressure side 111 of a vane. Proximate the suction side 113 of a vane the runout 120 of the fillet 119 may be lower, or closer to the axis of rotation, than an axisymmetric flowpath surface 115. However, in some embodiments the runout 120 may be higher, or further from the axis of rotation, than an axisymmetric flowpath surface 115 proximate the suction side 113 of a vane while the runout 120 may be lower, or closer to the axis of rotation, than an axisymmetric flowpath surface 115 proximate the pressure side 111 of a vane.
The altered flowpath geometry presented in
The divergence between non-axisymmetric flowpath surface 731 and axisymmetric flowpath surface 115 may be measured by an angle θ between the surfaces. In some embodiments, angle θ may be between 0 and 10 degrees.
The runout 120 along the fillet 119 of the pressure side 111 of a vane 102 may be asymmetric to the runout 120 along the fillet 119 of the suction side 113 of the same vane 102. The runout 120 along the fillet 119 of the pressure side 111 of a vane 102 may be asymmetric to the runout 120 along the fillet 119 of the suction side 113 of an adjacent vane 102.
Departures from an axisymmetric flowpath surface 115 such as those depicted in
In the embodiment of
The flowpath surface 731 taken at the runout 120 on the pressure side 111 may be higher (further from the axis of rotation) than an axisymmetric flowpath surface 115. The flowpath surface 731 taken at the runout 120 on the suction side 113 may be lower (closer to the axis of rotation) than an axisymmetric flowpath surface 115. The flowpath surface 731 taken both proximate to the pressure side 111 and the suction side 113 may be non-parabolic.
The runout 120 may return to an axisymmetric and/or parabolic flowpath surface 115 proximate the impeller inlet 122 and/or impeller discharge 124. In the illustrated embodiment, the runouts 120 proximate the pressure side 111 and suction side 113 each return to an axisymmetric and parabolic flowpath surface 115 at a meridional position of approximately 0.2 and 0.8. In some embodiments, the runout 120 may return to an axisymmetric and/or parabolic flowpath surface 115 at a first meridional position proximate the pressure side 111 and at a second meridional position proximate the suction side 113.
The runout 120 may have a maximum departure from an axisymmetric flowpath surface 115 at knee 833. The runout 120 may have a maximum departure from an axisymmetric flowpath surface 115 at a meridional position of 0.5. In some embodiments, the runout 120 may have a maximum departure from an axisymmetric flowpath surface 115 at a meridional position of between 0.2 and 0.8.
The axisymmetric flowpath surface 115 of
When the meridional position is considered in quartiles, the embodiment of
In the embodiment of
In some embodiments, such as that presented in
The flowpath surface 731 taken at the runout 120 on the suction side 113 may be higher than and/or axially forward from an axisymmetric flowpath surface 115. The flowpath surface 731 taken at the runout 120 on the pressure side 111 may be lower than and/or axially aft of an axisymmetric flowpath surface 115. The flowpath surface 731 taken both proximate to the pressure side 111 and the suction side 113 may be non-parabolic.
The flowpath surface 731 may diverge from an axisymmetric and/or parabolic flowpath surface 115 proximate the knee 833 and/or a meridional position of 0.5. The flowpath surface 731 may begin to diverge from an axisymmetric and/or parabolic flowpath surface 115 at a point between a meridional position of 0.4 and 0.6. In some embodiments, the flowpath surface 731 may begin to diverge from an axisymmetric and/or parabolic flowpath surface 115 at a first meridional position proximate the pressure side 111 and at a second meridional position proximate the suction side 113. The flowpath surface 731 may be axisymmetric and/or parabolic between the leading edge of a vane 102 and the leading edge of the splitter vane 127, and then begin to diverge from an axisymmetric and/or parabolic flowpath surface 115 at the leading edge of the splitter vane 127.
The flowpath surface 731 of
The axisymmetric flowpath surface 115 of
When the meridional position is considered in quartiles, the embodiment of
In the embodiment of
The divergence from an axisymmetric flowpath surface 115, such as that shown by flowpath surface 731 of
A flowpath surface 1036 extends generally from a runout 120 on the pressure side 111 of a vane 102 to the runout 120 on the suction side 113 of an adjacent vane 102 and is intersected by a splitter vane 127. The flowpath surface 1036 is thus defined as a first portion 1038 extending between the runout 120 on the pressure side 102 of a vane 102 and the runout 120 on the suction side 113 of a splitter vane 127, and a second portion 1039 extending between the runout 120 on the pressure side 102 of a splitter vane 127 and the runout 120 on the suction side 113 of a vane 102.
The divergence between non-axisymmetric flowpath surface 1036 and axisymmetric flowpath surface 115 may be measured by an angle θ between the surfaces. In some embodiments, angle θ may be between 0 and 10 degrees.
As shown in
In still further embodiments, the runout 120 at a fillet 119 of the pressure side 111 of a vane 102 may be asymmetric the runout 120 at a fillet 119 of the pressure side 111 of an adjacent vane 102.
The divergence from an axisymmetric flowpath surface 115 such as that shown by flowpath surface 731 of
In
The runout 120 on the pressure side 111 of vane 102 and the runout 120 on the pressure side 111 of splitter vane 127 may have a common divergence from an axisymmetric flowpath surface 115 (i.e. may be equally distant from the axis of rotation). Similarly, the runout 120 on the suction side 113 of a splitter vane 127 and the runout 120 on the suction side 113 of a vane 102 may have a common divergence from an axisymmetric flowpath surface 115 (i.e. may be equally distant from the axis of rotation). However in some embodiments the runouts 120 on a common side of adjacent vanes and/or splitter vanes may have varying divergences from an axisymmetric flowpath surface 115.
As shown in
In still further embodiments, the runout 120 at a fillet 119 of the pressure side 111 of a vane 102 may be asymmetric the runout 120 at a fillet 119 of the pressure side 111 of an adjacent vane 102.
In some embodiments the divergence between non-axisymmetric flowpath surface 1137 and axisymmetric flowpath surface 115 may be measured by an angle θ between the surfaces. In some embodiments, angle θ may be between 0 and 10 degrees. In some embodiments the divergence as measured by an angle θ may be different between the first flowpath surface segment 1143 and the second flowpath surface segment 1144.
As described above with reference to
The present disclosure provides many advantages over existing centrifugal impellers. The disclosed centrifugal impeller may obtain an improved efficiency and uniformity of gas discharge by adjusting the flowpath surface of the hub to more evenly distribute flow Mach numbers between the impeller vanes. More evenly distributed flow Mach numbers may reduce the tendency of cross flow to form from regions of relative low flow Mach number to regions of relatively high flow Mach number.
The present disclosure also provides for influencing cross flow and secondary flows of an impeller without altering or substantially altering the geometry of an impeller shroud and/or the impeller vanes. Thus a consistent vane profile is presented to the shroud, and the present disclosure does not increase the risk of impingement of the vanes against the shroud.
Although examples are illustrated and described herein, embodiments are nevertheless not limited to the details shown, since various modifications and structural changes may be made therein by those of ordinary skill within the scope and range of equivalents of the claims.
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