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Tribo-dynamics analysis of engine small-end bearing under real temperature boundary conditions by a wireless in-situ measuring technology

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... Firstly, a more comprehensive tribo-dynamics and bearing temperature prediction model was established with taking into account the impacts of elastic deformation and lubricant rheology for engine big-end bearing system. Secondly, the wireless in-situ temperature measurement equipment developed in our previous work [40] is modified based on the big-end bearing system features. Then, full-size engine tests were performed to measure the internal bearing temperature under actual engine operating conditions. ...
... This hinders the validation of numerical models' accuracy and could be a reason why many researchers' models do not consider bearing temperature behavior. Notably, This study benefits from the author's prior research [40], where a wireless temperature measurement device was developed specifically for small-end bearings. After some modification, this device can now be used to measure the big-end bearing temperature during ignition conditions. ...
... Notably, traditional wired or indirect measurements of bearing temperature have significant limitations. In our previous study, we successfully developed an in-situ wireless temperature measurement device for engine components [40]. In this experiment, it was successfully employed to wirelessly measure the big-end bearing temperature. ...
... Rights reserved. R. Li et al. become an academic term [12,26,37,63,69]. Building a tribo-dynamics model often starts with building a dynamics model. ...
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Piston assembly friction measurement has been carried out on a single cylinder gasoline engine using the IMEP (indicated mean effective pressure) method at realistic engine speeds and loads without any major engine modifications. Instantaneous and mean piston assembly friction were measured under motored and fired conditions at different lubricant temperatures. The forces acting on the piston assembly were carefully determinated by measuring the cylinder pressure, crankshaft angular velocity and strain in the connecting rod. The difference between the resulting gas pressure, inertia and connecting rod axial forces acting on the piston yields the piston assembly friction. To achieve this with confidence, an advanced instrumentation, telemetry and data acquisition system was designed and developed, giving special attention to the synchronisation and simultaneous sampling of analogue and digital channels. Experiments are reported for piston assembly friction at a range of engine operating conditions with different lubricant formulations, with and without a friction modifier.
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The effect of roughness on lubrication is considered. The research outlined in this paper was motivated by the need to find directly simple relationships between ∂h/∂x and ∂h̄T/ ∂x, ∂h/∂t and ∂h̄T/∂t instead of h and h̄T, where h = nominal film thickness (compliance); h̄T = average gap (separation). A dimensionless parameter called the contact factor is derived from the roughness deformation and probability theory. The introduction of the contact factor makes the average Reynolds equation not only much simplified but also more suitable for studying partial hydrodynamic lubrication and elastohydrodynamic lubrication. The contact factor is the probability that the surfaces are really lubricated, and this makes the physical meaning of the average Reynolds equation clearer.
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Experimental results of steady dimples measured in elliptical glass-steel contact under pure sliding conditions are presented. It is found that two dimples connected with a shallower furrow are generated, each near an end of the major radius of the contact ellipse. The complete solution of the corresponding thermal elastohydrodynamic lubrication (TEHL) problem is calculated numerically. Good agreement is obtained between the experimental and theoretical results. This agreement can be explained by the temperature-viscosity wedge mechanism. Correctness of this mechanism is demonstrated using additional experiments with ceramic balls in contact with glass and sapphire disks.
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Surfaces and subsurfaces of test specimens that failed in scuffing were examined. A scuffing criterion is developed stating that scuffing failure would occur when the maximum surface tangential traction is larger than the modified shear strength. A scuffing uncertainty factor is introduced to reflect the influence of factors that affect wear and scuffing and the inaccuracy in modeling.
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Performance analysis of a piston ring pack is presented in this investigation with the objective of studying the behavior and interrelationships of key engine parameters such as oil consumption, blow-by/blow-back, power loss and wear loads for typical operating conditions. The analysis is based on an integrated methodology addressing the various physical phenomena associated with ring packs including (a) ring dynamics for axial and twist motions within the grooves to determine flow paths for gases, (b) inter-ring gas dynamics for blow-by and blow-back behavior, (c) mixed lubrication at the ring face-liner conjunction for friction considerations and radial ring dynamics, and (d) oil transport for distribution of lubricant along the liner. Relevant output from each of these phenomenological models such as instantaneous values of (i) inter-ring flow areas, (ii) gas blow-back, (Hi) volume of oil within inter-ring regions, (iv) oil accumulation at top ring's leading edge and (v) liner oil film distribution are utilized by the oil consumption models which enable the calculations from the various consumption mechanisms (due to throw-off, entrainment and evaporation). Additionally, wear loads on the ring faces and liner are calculated based on contact pressures due to mixed lubrication at the ring face-liner interface. Included in this investigation are results from a series of studies undertaken to analyze the behavior of the aforementioned engine parameters over a range of speed and load conditions.
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The interpretation of certain phenomena occuring at nominally flat surfaces in stationary or sliding contact is dependent on the assumed distribution of the real area of contact between the surfaces. Since there is little direct evidence on which to base an estimate of this distribution, the approach used is to set up a simple model and compare the deduced theory (e.g., the deduced dependence of the experimental observables on the load) with the experimental evidence. The main conclusions are as follows. (a) The electrical contact resistance depends on the model used to represent the surfaces; the most realistic model is one in which increasing the load increases both the number and size of the contact areas. (b) In general, mechanical wear should also depend on the model. However, in wear experiments showing the simplest behavior, the wear rate is proportional to the load, and these results can be explained by assuming removal of lumps at contact areas formed by plastic deformation; moreover, this particular deduction is independent of the assumed model. This suggests that a basic assumption of previous theories, that increasing the load increases the number of contacts without affecting their average size, is redundant.