Remarks on Modeling the Oil Film Generation of Rod Seals
The oil film generation of a U-cup rod seal and the oil film thickness on the rod after outstroke were analyzed analytically, numerically, and experimentally. The analyzed sealing system consists of an unmodified, commercially available U-cup, a polished rod, and mineral oil. The inverse theory of h...
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doaj-b41ab65785c442379992cee18a8676572021-09-26T00:34:57ZengMDPI AGLubricants2075-44422021-09-019959510.3390/lubricants9090095Remarks on Modeling the Oil Film Generation of Rod SealsOliver Feuchtmüller0Nino Dakov1Lothar Hörl2Frank Bauer3Institute of Machine Components, Sealing Technology, University of Stuttgart, 70569 Stuttgart, GermanyInstitute of Machine Components, Sealing Technology, University of Stuttgart, 70569 Stuttgart, GermanyInstitute of Machine Components, Sealing Technology, University of Stuttgart, 70569 Stuttgart, GermanyInstitute of Machine Components, Sealing Technology, University of Stuttgart, 70569 Stuttgart, GermanyThe oil film generation of a U-cup rod seal and the oil film thickness on the rod after outstroke were analyzed analytically, numerically, and experimentally. The analyzed sealing system consists of an unmodified, commercially available U-cup, a polished rod, and mineral oil. The inverse theory of hydrodynamic lubrication (IHL) and an elastohydrodynamic lubrication (EHL) model—both based on the Reynolds equation for thin lubricating films—were utilized to simulate the oil film generation. In the EHL analysis, physical parameters and numerical EHL parameters were varied. Both the analytical and numerical results for the varied parameters show that the film thickness follows a square-root function (i.e., with a function exponent of 0.5) with respect to the product of dynamic viscosity and rod speed, also referred to as the duty parameter. In comparison to the analytical and numerical results, the film thickness obtained via ellipsometry measurements is a function of the duty parameter with an exponent of approximately 0.85. Possible causes for the discrepancy between theory and experiments are discussed. A potential remedy for the modeling gap is proposed.https://www.mdpi.com/2075-4442/9/9/95hydraulic rod sealfilm thickness measurementelastohydrodynamic simulationReynolds equation |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Oliver Feuchtmüller Nino Dakov Lothar Hörl Frank Bauer |
spellingShingle |
Oliver Feuchtmüller Nino Dakov Lothar Hörl Frank Bauer Remarks on Modeling the Oil Film Generation of Rod Seals Lubricants hydraulic rod seal film thickness measurement elastohydrodynamic simulation Reynolds equation |
author_facet |
Oliver Feuchtmüller Nino Dakov Lothar Hörl Frank Bauer |
author_sort |
Oliver Feuchtmüller |
title |
Remarks on Modeling the Oil Film Generation of Rod Seals |
title_short |
Remarks on Modeling the Oil Film Generation of Rod Seals |
title_full |
Remarks on Modeling the Oil Film Generation of Rod Seals |
title_fullStr |
Remarks on Modeling the Oil Film Generation of Rod Seals |
title_full_unstemmed |
Remarks on Modeling the Oil Film Generation of Rod Seals |
title_sort |
remarks on modeling the oil film generation of rod seals |
publisher |
MDPI AG |
series |
Lubricants |
issn |
2075-4442 |
publishDate |
2021-09-01 |
description |
The oil film generation of a U-cup rod seal and the oil film thickness on the rod after outstroke were analyzed analytically, numerically, and experimentally. The analyzed sealing system consists of an unmodified, commercially available U-cup, a polished rod, and mineral oil. The inverse theory of hydrodynamic lubrication (IHL) and an elastohydrodynamic lubrication (EHL) model—both based on the Reynolds equation for thin lubricating films—were utilized to simulate the oil film generation. In the EHL analysis, physical parameters and numerical EHL parameters were varied. Both the analytical and numerical results for the varied parameters show that the film thickness follows a square-root function (i.e., with a function exponent of 0.5) with respect to the product of dynamic viscosity and rod speed, also referred to as the duty parameter. In comparison to the analytical and numerical results, the film thickness obtained via ellipsometry measurements is a function of the duty parameter with an exponent of approximately 0.85. Possible causes for the discrepancy between theory and experiments are discussed. A potential remedy for the modeling gap is proposed. |
topic |
hydraulic rod seal film thickness measurement elastohydrodynamic simulation Reynolds equation |
url |
https://www.mdpi.com/2075-4442/9/9/95 |
work_keys_str_mv |
AT oliverfeuchtmuller remarksonmodelingtheoilfilmgenerationofrodseals AT ninodakov remarksonmodelingtheoilfilmgenerationofrodseals AT lotharhorl remarksonmodelingtheoilfilmgenerationofrodseals AT frankbauer remarksonmodelingtheoilfilmgenerationofrodseals |
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