Hydrodynamic Lubrication

Hydrodynamic Lubrication
Hydrodynamic Lubrication. Edited from http://pdf.directindustry.com

Revision for “Hydrodynamic Lubrication” created on April 27, 2017 @ 13:12:34 [Autosave]

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Hydrodynamic Lubrication
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<h2>Definition</h2> Hydrodynamic lubrication theory is a theory used to reduce friction and/or wear of rubbing solids with the aid of liquid lubricant. For a vast majority of the surfaces encountered in nature and used in industry, the source of friction is the imperfections of the surfaces. Even mirror shining surfaces are composed of hills and valleys - surface roughness. The goal of hydrodynamic lubrication is to add a proper lubricant, so that it penetrates into the contact zone between rubbing solids and creates a thin liquid film. This film separates the surfaces from direct contact and it in general reduces friction and consequently wear (but not always), since friction within the lubricant is less than between the directly contacting solids. &nbsp; History of lubrication theory goes more than a century back to 1886 when O. Reynolds published famous equation of thin fluid film flow in the narrow gap between two solids (<a href="http://discovery.nationalarchives.gov.uk/details/rd/9c1e8ebb-baae-41b2-8c13-799b8ea03dcf" target="_blank" rel="noopener noreferrer">Reynolds 1886</a>). This equation carries his name and forms a foundation of the lubrication theory. Derivation of Reynolds equation and possible solution methods are given <a href="http://www.tribonet.org/wiki/reynolds-equation/" target="_blank" rel="noopener noreferrer">here</a>. It differs from <a href="http://www.tribonet.org/wiki/elastohydrodynamic-lubrication-ehl/" target="_blank" rel="noopener noreferrer">elastohydrodynamic lubrication theory (EHL)</a> due to negligible elastic deformation of the surfaces. Absence of the elastic deformations simplifies the problem as compared to EHL theory, but allows one to construct some important analytical solutions as will be shown further. <h2>Solution</h2> First solutions of lubrication theory were obtained by Reynolds himself and can be found in the <a href="http://discovery.nationalarchives.gov.uk/details/rd/9c1e8ebb-baae-41b2-8c13-799b8ea03dcf">original work</a>. One of the most important analytical solutions of the hydrodynamic theory (of the most interest in tribology field) was obtained by Martin in 1916. The solution considers a relative motion of cylinder on flat plane, as shown in figure below. <img class="wp-image-1944 aligncenter" src="http://www.tribonet.org/wp-content/uploads/2017/02/Hydrodynamic-Solution.jpg" alt="hydrodynamic solution" width="362" height="182" data-wp-pid="1944" /> Following system of equations is considered: [math] \begin{eqnarray} \label{complete_sys1} \frac{\partial}{\partial x}(\frac{h^3}{\mu}\frac{\partial p}{\partial x}) = 6U_m\frac{\partial h}{\partial x} \\ \label{complete_sys2} h(x) = h_0 + \frac{x^2}{2R} \\ \label{complete_sys3} F_l = \int_{-\infty}^{\infty} pdx \\ \end{eqnarray} [/math] where [math] h, p, \mu, \alpha, U_m [/math] are hydrodynamic film thickness, pressure, viscosity and average sliding speed correspondingly ([math] U_m = \frac{U_1+U_2}{2} [/math]). [math] F_l [/math] here is the normal load (per unit length). There are two unknowns, pressure and the approach [math] h_0 [/math] with two equations to determine them. Martin's solution states following: [math] \begin{eqnarray} \label{complete_sys1} h_0 = 4.9\frac{\mu U_m R}{F_l} \\ \end{eqnarray} [/math] This solution immediately shows the major relations within the hydrodynamic theory (but they also remain qualitatively true in elastohydrodynamic theory as well). The sliding speed has to be higher to generate a thicker film. The same is true for viscosity: higher viscosity leads to a thicker lubricant film. It should be noted, that it is typically desired to have a sufficiently thick lubricant film, so that the surface are completely separated to reduce wear. At the same time, it is clear, that the friction (hydrodynamic) will increase with the increase of both, sliding speed and viscosity. This in turn leads to energy losses. Therefore, there will be a trade-off between the wear performance and the optimization of energy losses. Currently, continuous efforts are undertaken to reduce the energy losses and to move towards a sustainable society and at the same time increase the reliability of tribological devices. According to the discussion above it is clear that there is a contradiction between the wear performance and the energetical performance. Therefore, classical lubrication theory has reached its fundamental limit in the energy losses reduction and new theories have to be developed. From that standpoint, solid lubricants, such as <a href="http://www.tribonet.org/reduce-the-friction-with-graphene-balls/" target="_blank" rel="noopener noreferrer">graphene</a> or <a href="http://www.tribonet.org/macroscale-superlubricity/">diamond like carbon</a> are promising materials to reduce friction further. See this video for further information regarding hydrodynamic lubrication principles: [embed]https://www.youtube.com/watch?v=WwvLvgwSpT4[/embed] <span style="border-radius: 2px; text-indent: 20px; width: auto; padding: 0px 4px 0px 0px; text-align: center; font: bold 11px/20px 'Helvetica Neue',Helvetica,sans-serif; color: #ffffff; background: no-repeat scroll 3px 50% / 14px 14px #bd081c; position: absolute; opacity: 1; z-index: 8675309; display: none; cursor: pointer;">Save</span> <span style="border-radius: 2px; text-indent: 20px; width: auto; padding: 0px 4px 0px 0px; text-align: center; font: bold 11px/20px 'Helvetica Neue',Helvetica,sans-serif; color: #ffffff; background: no-repeat scroll 3px 50% / 14px 14px #bd081c; position: absolute; opacity: 1; z-index: 8675309; display: none; cursor: pointer;">Save</span> <span style="border-radius: 2px; text-indent: 20px; width: auto; padding: 0px 4px 0px 0px; text-align: center; font: bold 11px/20px 'Helvetica Neue',Helvetica,sans-serif; color: #ffffff; background: no-repeat scroll 3px 50% / 14px 14px #bd081c; position: absolute; opacity: 1; z-index: 8675309; display: none; cursor: pointer;">Save</span> <span style="border-radius: 2px; text-indent: 20px; width: auto; padding: 0px 4px 0px 0px; text-align: center; font: bold 11px/20px 'Helvetica Neue',Helvetica,sans-serif; color: #ffffff; background: no-repeat scroll 3px 50% / 14px 14px #bd081c; position: absolute; opacity: 1; z-index: 8675309; display: none; cursor: pointer;">Save</span> <span style="border-radius: 2px; text-indent: 20px; width: auto; padding: 0px 4px 0px 0px; text-align: center; font: bold 11px/20px 'Helvetica Neue',Helvetica,sans-serif; color: #ffffff; background: #bd081c no-repeat scroll 3px 50% / 14px 14px; position: absolute; opacity: 1; z-index: 8675309; display: none; cursor: pointer; top: 580px; left: 337px;">Save</span> <span style="border-radius: 2px; text-indent: 20px; width: auto; padding: 0px 4px 0px 0px; text-align: center; font: bold 11px/20px 'Helvetica Neue',Helvetica,sans-serif; color: #ffffff; background: #bd081c no-repeat scroll 3px 50% / 14px 14px; position: absolute; opacity: 1; z-index: 8675309; display: none; cursor: pointer;">Save</span>
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