Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios
The average velocity field at the pump–turbine interface in a scaled version of a truck torque converter was studied. Seven different turbine-to-pump rotational-speed ratios were examined, ranging from near stall (0.065) to overspeed (1.050) so as to determine the effect of the speed ratio on the fl...
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| Format: | Article |
| Language: | English |
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Wiley
2003-01-01
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| Series: | International Journal of Rotating Machinery |
| Online Access: | http://dx.doi.org/10.1155/S1023621X0300040X |
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| author | A. Habsieger R. D. Flack |
| author_facet | A. Habsieger R. D. Flack |
| author_sort | A. Habsieger |
| collection | DOAJ |
| description | The average velocity field at the pump–turbine interface in a scaled version of a truck torque converter was studied. Seven different turbine-to-pump rotational-speed ratios were examined, ranging from near stall (0.065) to overspeed (1.050) so as to determine the effect of the speed ratio on the flow field and on the mass flow rate. Laser velocimetry was used to measure the flow velocity through the pump's exit and the turbine's inlet plane. At the pump's exit, as the speed ratio increases, the high velocities move to the pressure-shell corner and then to both the core-suction and the pressureshell corners. Concentrated velocity gradients are largest at the lowest speed ratio, but areas of velocity gradients are largest near the coupling point. Near the coupling point, the flow field is most nonuniform, which yields a highly periodic flow into the turbine inlet. Above the coupling point, the high velocity remains in the pressure-shell corner but separation is seen to develop at the highest speed ratio. At the turbine's inlet, reverse flow is seen at low speed ratios and is an indicator of flow leakage through the core. Velocity gradients are very large at low speed ratios. As the speed ratio increases to the coupling point, the high velocities remain on the shell side. Above the coupling point, the high-velocity flow migrates from the shell side to the core side. The mass flow rate decreases significantly and nonlinearly with the increase of the speed ratio, but for speed ratios greater than 1.000, the negative slope decreases. |
| format | Article |
| id | doaj-art-19e86bc120b3455d9b265c30294df4e0 |
| institution | OA Journals |
| issn | 1023-621X |
| language | English |
| publishDate | 2003-01-01 |
| publisher | Wiley |
| record_format | Article |
| series | International Journal of Rotating Machinery |
| spelling | doaj-art-19e86bc120b3455d9b265c30294df4e02025-08-20T02:01:58ZengWileyInternational Journal of Rotating Machinery1023-621X2003-01-019641942610.1155/S1023621X0300040XFlow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed RatiosA. Habsieger0R. D. Flack1Department of Mechanical and Aerospace Engineering, University of Virginia, Charlottesville, Virginia, USADepartment of Mechanical and Aerospace Engineering, University of Virginia, Charlottesville, Virginia, USAThe average velocity field at the pump–turbine interface in a scaled version of a truck torque converter was studied. Seven different turbine-to-pump rotational-speed ratios were examined, ranging from near stall (0.065) to overspeed (1.050) so as to determine the effect of the speed ratio on the flow field and on the mass flow rate. Laser velocimetry was used to measure the flow velocity through the pump's exit and the turbine's inlet plane. At the pump's exit, as the speed ratio increases, the high velocities move to the pressure-shell corner and then to both the core-suction and the pressureshell corners. Concentrated velocity gradients are largest at the lowest speed ratio, but areas of velocity gradients are largest near the coupling point. Near the coupling point, the flow field is most nonuniform, which yields a highly periodic flow into the turbine inlet. Above the coupling point, the high velocity remains in the pressure-shell corner but separation is seen to develop at the highest speed ratio. At the turbine's inlet, reverse flow is seen at low speed ratios and is an indicator of flow leakage through the core. Velocity gradients are very large at low speed ratios. As the speed ratio increases to the coupling point, the high velocities remain on the shell side. Above the coupling point, the high-velocity flow migrates from the shell side to the core side. The mass flow rate decreases significantly and nonlinearly with the increase of the speed ratio, but for speed ratios greater than 1.000, the negative slope decreases.http://dx.doi.org/10.1155/S1023621X0300040X |
| spellingShingle | A. Habsieger R. D. Flack Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios International Journal of Rotating Machinery |
| title | Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios |
| title_full | Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios |
| title_fullStr | Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios |
| title_full_unstemmed | Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios |
| title_short | Flow Characteristics at the Pump-Turbine Interface of a Torque Converter at Extreme Speed Ratios |
| title_sort | flow characteristics at the pump turbine interface of a torque converter at extreme speed ratios |
| url | http://dx.doi.org/10.1155/S1023621X0300040X |
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