Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing
The dominant factors and processes for the rapid progression of scuffing from a partial area to an entire surface under lubricated, plane contact, and pure sliding conditions were studied by performing an in situ observation of the surface, and in situ measurements of the oil-film thickness and temp...
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Japanese Society of Tribologists
2021
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oai:doaj.org-article:abb1762dfd3d43f9835ba5eb917c649b2021-11-05T09:31:04ZProposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing1881-219810.2474/trol.16.89https://doaj.org/article/abb1762dfd3d43f9835ba5eb917c649b2021-04-01T00:00:00Zhttps://www.jstage.jst.go.jp/article/trol/16/2/16_89/_pdf/-char/enhttps://doaj.org/toc/1881-2198The dominant factors and processes for the rapid progression of scuffing from a partial area to an entire surface under lubricated, plane contact, and pure sliding conditions were studied by performing an in situ observation of the surface, and in situ measurements of the oil-film thickness and temperature distributions during scuffing. Transitions of the oil-film thickness were measured using three-wavelength optical interferometry, and the temperature distributions of the sliding surface were measured using thermography. It was observed that oil-film breakdown progressed from a partial area to an entire surface within several tens of milliseconds under high sliding speed and high-load conditions. The proposed process of the rapid progression of oil-film breakdown on the surface was described using the "thermal-diffusion-induced spiral model." The processes in the model are as follows: (I) the frictional heat generated in a solid contact area diffused into the adjacent region of the surface; (II) the oil-film temperature in the adjacent region increased within a short time, as the films were very thin (several tens of nanometers); (III) the viscosities of the oil-films decreased; (IV) the solid contact area grew larger, and these phenomena repeated continuously until the oil-film breakdown reached the entire surface.Mamoru TohyamaTakashi IzumiShuzo SandaJapanese Society of Tribologistsarticlescuffingoil-filmfilm thicknessin situ observationfrictional heatthermal diffusionPhysicsQC1-999Engineering (General). Civil engineering (General)TA1-2040Mechanical engineering and machineryTJ1-1570ChemistryQD1-999ENTribology Online, Vol 16, Iss 2, Pp 89-98 (2021) |
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DOAJ |
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scuffing oil-film film thickness in situ observation frictional heat thermal diffusion Physics QC1-999 Engineering (General). Civil engineering (General) TA1-2040 Mechanical engineering and machinery TJ1-1570 Chemistry QD1-999 |
spellingShingle |
scuffing oil-film film thickness in situ observation frictional heat thermal diffusion Physics QC1-999 Engineering (General). Civil engineering (General) TA1-2040 Mechanical engineering and machinery TJ1-1570 Chemistry QD1-999 Mamoru Tohyama Takashi Izumi Shuzo Sanda Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing |
description |
The dominant factors and processes for the rapid progression of scuffing from a partial area to an entire surface under lubricated, plane contact, and pure sliding conditions were studied by performing an in situ observation of the surface, and in situ measurements of the oil-film thickness and temperature distributions during scuffing. Transitions of the oil-film thickness were measured using three-wavelength optical interferometry, and the temperature distributions of the sliding surface were measured using thermography. It was observed that oil-film breakdown progressed from a partial area to an entire surface within several tens of milliseconds under high sliding speed and high-load conditions. The proposed process of the rapid progression of oil-film breakdown on the surface was described using the "thermal-diffusion-induced spiral model." The processes in the model are as follows: (I) the frictional heat generated in a solid contact area diffused into the adjacent region of the surface; (II) the oil-film temperature in the adjacent region increased within a short time, as the films were very thin (several tens of nanometers); (III) the viscosities of the oil-films decreased; (IV) the solid contact area grew larger, and these phenomena repeated continuously until the oil-film breakdown reached the entire surface. |
format |
article |
author |
Mamoru Tohyama Takashi Izumi Shuzo Sanda |
author_facet |
Mamoru Tohyama Takashi Izumi Shuzo Sanda |
author_sort |
Mamoru Tohyama |
title |
Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing |
title_short |
Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing |
title_full |
Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing |
title_fullStr |
Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing |
title_full_unstemmed |
Proposition of Thermal-Diffusion-Induced Spiral Model for the Rapid Oil-Film Breakdown Process during Scuffing |
title_sort |
proposition of thermal-diffusion-induced spiral model for the rapid oil-film breakdown process during scuffing |
publisher |
Japanese Society of Tribologists |
publishDate |
2021 |
url |
https://doaj.org/article/abb1762dfd3d43f9835ba5eb917c649b |
work_keys_str_mv |
AT mamorutohyama propositionofthermaldiffusioninducedspiralmodelfortherapidoilfilmbreakdownprocessduringscuffing AT takashiizumi propositionofthermaldiffusioninducedspiralmodelfortherapidoilfilmbreakdownprocessduringscuffing AT shuzosanda propositionofthermaldiffusioninducedspiralmodelfortherapidoilfilmbreakdownprocessduringscuffing |
_version_ |
1718444308680409088 |