Isothermal Elastohydrodynamic Lubrication of Point Contacts: Part IV—Starvation ResultsSource: Journal of Tribology:;1977:;volume( 099 ):;issue: 001::page 15DOI: 10.1115/1.3452973Publisher: The American Society of Mechanical Engineers (ASME)
Abstract: Utilizing the theory and numerical procedure developed by the authors in an earlier publication the influence of lubricant starvation on minimum film thickness was investigated. This study of lubricant starvation was performed simply by moving the inlet boundary closer to the contact center. From the results it was found that for the range of conditions considered the value of dimensionless inlet distance at the boundary between fully flooded and starved conditions (m*) can be expressed simply as m*=1+3.06Rxb2Hc,F0.58 or m*=1+3.34Rxb2Hmin,F0.56 that is, for a dimensionless inlet distance (m) less than m*, starvation occurs, and for m ≥ m*, a fully flooded condition exists. Furthermore, it has been possible to express the central and minimum film thickness for a starved condition as Hc,S=Hc,Fm−1m*−10.29Hmin,S=Hmin,Fm−1m*−10.25 Contour plots of the pressure and film thickness in and around the contact are shown for the fully flooded and starved lubricant condition. From these contour plots it was observed that the pressure spike becomes suppressed and the film thickness decreases substantially as starvation increases.
keyword(s): Pressure , Lubricants , Elastohydrodynamic lubrication AND Film thickness ,
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| contributor author | B. J. Hamrock | |
| contributor author | D. Dowson | |
| date accessioned | 2017-05-08T23:03:57Z | |
| date available | 2017-05-08T23:03:57Z | |
| date copyright | January, 1977 | |
| date issued | 1977 | |
| identifier issn | 0742-4787 | |
| identifier other | JOTRE9-28605#15_1.pdf | |
| identifier uri | http://yetl.yabesh.ir/yetl/handle/yetl/90519 | |
| description abstract | Utilizing the theory and numerical procedure developed by the authors in an earlier publication the influence of lubricant starvation on minimum film thickness was investigated. This study of lubricant starvation was performed simply by moving the inlet boundary closer to the contact center. From the results it was found that for the range of conditions considered the value of dimensionless inlet distance at the boundary between fully flooded and starved conditions (m*) can be expressed simply as m*=1+3.06Rxb2Hc,F0.58 or m*=1+3.34Rxb2Hmin,F0.56 that is, for a dimensionless inlet distance (m) less than m*, starvation occurs, and for m ≥ m*, a fully flooded condition exists. Furthermore, it has been possible to express the central and minimum film thickness for a starved condition as Hc,S=Hc,Fm−1m*−10.29Hmin,S=Hmin,Fm−1m*−10.25 Contour plots of the pressure and film thickness in and around the contact are shown for the fully flooded and starved lubricant condition. From these contour plots it was observed that the pressure spike becomes suppressed and the film thickness decreases substantially as starvation increases. | |
| publisher | The American Society of Mechanical Engineers (ASME) | |
| title | Isothermal Elastohydrodynamic Lubrication of Point Contacts: Part IV—Starvation Results | |
| type | Journal Paper | |
| journal volume | 99 | |
| journal issue | 1 | |
| journal title | Journal of Tribology | |
| identifier doi | 10.1115/1.3452973 | |
| journal fristpage | 15 | |
| journal lastpage | 23 | |
| identifier eissn | 1528-8897 | |
| keywords | Pressure | |
| keywords | Lubricants | |
| keywords | Elastohydrodynamic lubrication AND Film thickness | |
| tree | Journal of Tribology:;1977:;volume( 099 ):;issue: 001 | |
| contenttype | Fulltext |