Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis
This paper proposes a contact model between a rigid sphere and an elastic plane covered with a thin liquid film. The elastic contact is determined by Johnson–Kendall–Roberts theory, which deals with the energy equilibrium of elastic and interfacial energies. In elastic contact under presence of thin...
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Japanese Society of Tribologists
2020
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oai:doaj.org-article:316f09844e7049289914ade2bfbd22342021-11-05T09:12:03ZAdhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis1881-219810.2474/trol.15.1https://doaj.org/article/316f09844e7049289914ade2bfbd22342020-01-01T00:00:00Zhttps://www.jstage.jst.go.jp/article/trol/15/1/15_1/_pdf/-char/enhttps://doaj.org/toc/1881-2198This paper proposes a contact model between a rigid sphere and an elastic plane covered with a thin liquid film. The elastic contact is determined by Johnson–Kendall–Roberts theory, which deals with the energy equilibrium of elastic and interfacial energies. In elastic contact under presence of thin liquid film, the energy needed to separate the two bodies is defined as the summation of the interfacial energy among the sphere, liquid, and plane. Capillary force affects the two bodies because a liquid bridge is formed between them. Shape of the liquid bridge, assumed by the Clark’s toroidal approximation, determines the capillary force. The hysteresis of the liquid contact angles and that of the liquid volume between loading and unloading processes are considered. In loading process, the liquid film is squeezed out from the contact area and accumulates at the contact edge with increasing the liquid contact angles. In unloading process, the accumulated liquid is dragged to the contact edge, and the contact angles decrease. An irreversible force curve is obtained from these two hystereses, and the effect of liquid bridge is discussed based on the calculated results. In addition, the adhesion-hysteresis mechanisms caused by the capillary force are discussed.Yoji IguchiDooyoung BaekSatoshi MomozonoPasomphone HemthavyShigeki SaitoKunio TakahashiJapanese Society of Tribologistsarticleadhesion contactanalytical modelcapillary forceliquid contact anglesphereelastic half spacePhysicsQC1-999Engineering (General). Civil engineering (General)TA1-2040Mechanical engineering and machineryTJ1-1570ChemistryQD1-999ENTribology Online, Vol 15, Iss 1, Pp 1-8 (2020) |
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DOAJ |
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adhesion contact analytical model capillary force liquid contact angle sphere elastic half space Physics QC1-999 Engineering (General). Civil engineering (General) TA1-2040 Mechanical engineering and machinery TJ1-1570 Chemistry QD1-999 |
spellingShingle |
adhesion contact analytical model capillary force liquid contact angle sphere elastic half space Physics QC1-999 Engineering (General). Civil engineering (General) TA1-2040 Mechanical engineering and machinery TJ1-1570 Chemistry QD1-999 Yoji Iguchi Dooyoung Baek Satoshi Momozono Pasomphone Hemthavy Shigeki Saito Kunio Takahashi Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis |
description |
This paper proposes a contact model between a rigid sphere and an elastic plane covered with a thin liquid film. The elastic contact is determined by Johnson–Kendall–Roberts theory, which deals with the energy equilibrium of elastic and interfacial energies. In elastic contact under presence of thin liquid film, the energy needed to separate the two bodies is defined as the summation of the interfacial energy among the sphere, liquid, and plane. Capillary force affects the two bodies because a liquid bridge is formed between them. Shape of the liquid bridge, assumed by the Clark’s toroidal approximation, determines the capillary force. The hysteresis of the liquid contact angles and that of the liquid volume between loading and unloading processes are considered. In loading process, the liquid film is squeezed out from the contact area and accumulates at the contact edge with increasing the liquid contact angles. In unloading process, the accumulated liquid is dragged to the contact edge, and the contact angles decrease. An irreversible force curve is obtained from these two hystereses, and the effect of liquid bridge is discussed based on the calculated results. In addition, the adhesion-hysteresis mechanisms caused by the capillary force are discussed. |
format |
article |
author |
Yoji Iguchi Dooyoung Baek Satoshi Momozono Pasomphone Hemthavy Shigeki Saito Kunio Takahashi |
author_facet |
Yoji Iguchi Dooyoung Baek Satoshi Momozono Pasomphone Hemthavy Shigeki Saito Kunio Takahashi |
author_sort |
Yoji Iguchi |
title |
Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis |
title_short |
Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis |
title_full |
Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis |
title_fullStr |
Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis |
title_full_unstemmed |
Adhesional Contact between Rigid Sphere and Elastic Plane Covered with Thin Liquid Film Considering Contact-Angle Hysteresis |
title_sort |
adhesional contact between rigid sphere and elastic plane covered with thin liquid film considering contact-angle hysteresis |
publisher |
Japanese Society of Tribologists |
publishDate |
2020 |
url |
https://doaj.org/article/316f09844e7049289914ade2bfbd2234 |
work_keys_str_mv |
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_version_ |
1718444401260232704 |