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Proceedings of SerbiaTrib '13

Proceedings of SerbiaTrib '13

Proceedings of SerbiaTrib '13

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comes to the sharp increase <strong>of</strong> wear rate and toreduction <strong>of</strong> pressure. Lubrication with synthetic oilhas a smaller increase <strong>of</strong> wear rate and smallerreduction <strong>of</strong> pressure.Based on the foregoing analysis, it can beconcluded that the Hertzian contact stress dependson the choice <strong>of</strong> lubricant. Synthetic lubricating oilis the most favourable from the aspect <strong>of</strong> wear, andin terms <strong>of</strong> achieving hydrodynamic lubrication.Optimal lubrication conditions were obtained forthe rotation speed <strong>of</strong> n 1 = 5000 min -1 or slidingvelocity v gs = 2.53 m/s.6. DAMAGE TYPES6.1. WearFigure 4. Wear on wheel tooth surface withoutadditional treatment for T 2 = 36 Nm; t = 260 h;n 1 = 5000 min -1tribological system are: the gear wheel (basicbody), the worm (opposed body) and the lubricant(intermediate component).Experiments with wheels with differentadditional treatments provide basic knowledge <strong>of</strong>sintered gears load capacity. Worm and wheel arein contact in a point. During operation, a change inthe tooth flank <strong>of</strong> the wheel appears due to wear.The worm forms on the tooth flank <strong>of</strong> the wheel, awear surface that has a shape that is identical toworm gear flank. Wear progress widens the wearsurface, which leads to a lower Hertzian pressure inthe tooth contact. After a certain period <strong>of</strong> operationunder intensive wear progress, the steady stateoccurs, where a necessary oil layer exists, so thatthe wear progress is minimal. Figure 4 shows theform <strong>of</strong> wear damage on tooth surface <strong>of</strong> wheelmade from material without additional treatment.Figure 5 compares all experiments with wheels<strong>of</strong> different material variants after a trial <strong>of</strong> 100 hand an output torque <strong>of</strong> 20 Nm. The maximumwear, δ wn = 115 m, occurred on material S2 –material with case hardening. The minimum wear,δ wn = 7.8 m, occurred on S5 – sinter-hardening.Figure 4 shows the wear width <strong>of</strong> the wear surfaceon wheel from material S4 - “pyrohydrolysis” andS5 sinter-hardening for different speeds. TheFigure 5. Wear δ wn for all trials with different material variants [6]The wear describes the continuous loss <strong>of</strong>material from the surface <strong>of</strong> the basic body whichhas a relative movement with respect to a solid,liquid or gaseous mating with which it is in contact[7]. Wear has exclusively mechanical causes.Different from hardness or tensile strength, wear isnot a specific material property but a systemproperty which depends on the particulartribological system. In our case, the elements <strong>of</strong> thesmallest wear width occurred at input speedn 1 = 5000 min -1 . The reason for this is that the bestexperimental conditions, with regard to lubricationand wear, are at this input speed.6.2. WearA large pressure on surface does not lead to asudden failure <strong>of</strong> drive, but over the time, small324 13 th International Conference on Tribology – Serbiatrib’13

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