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Proceedings of SerbiaTrib '13

Proceedings of SerbiaTrib '13

Proceedings of SerbiaTrib '13

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The tribometer operates in principle <strong>of</strong> inclinedplane. Contact pair together with system for heatingand probe for temperature measurement is rotatedfrom horizontal to the desired angle α. The rotatedangle <strong>of</strong> inclined plane is measured with readingprecision <strong>of</strong> one minute, which for a wide interval<strong>of</strong> possible values <strong>of</strong> the coefficient <strong>of</strong> rollingfriction causes the measurement error less than 3%.Figure 1 – The balance <strong>of</strong> rolling body at inclined plateThe authors’ starting point was from theoreticalassumption that the contact between ball and flatsurface in laboratory conditions will be achieved onthe small number <strong>of</strong> unevenness in a regard anumber <strong>of</strong> unevenness at higher temperatures.Further, it is assumed that due to thermal expansion<strong>of</strong> material in the contact zone, will result asincreasing <strong>of</strong> value e (figure 1). This means that asa consequence we will have an increase <strong>of</strong> rollingmoment resistance and a parallel increase <strong>of</strong> thecoefficient <strong>of</strong> rolling friction. The authors believethat there is some correlation between staticcoefficient <strong>of</strong> rolling friction and the value <strong>of</strong>thermal dilatation <strong>of</strong> contact pair. If we have inmind the stochastic nature <strong>of</strong> real contact area andnonlinear temperature field, it is hard totheoretically quantify the influence <strong>of</strong> temperatureon coefficient <strong>of</strong> friction. Hence, in order toquantify the influence <strong>of</strong> various parameters oncoefficient <strong>of</strong> friction, authors will provide relativeextensive experimental research.3. EXPERIMENTAL TESTSExperimental tests were performed on a specialdesigned and constructed tribometer. The completemeasuring instrument is showed on figure 2. Also,all positions are marked with numbers anddescribed in following text. The tribometer consists<strong>of</strong> three bigger parts, as follows:1 – Thermoregulator. The main aim <strong>of</strong> this part is tovary a temperature (in our case is 200°C). There aretwo small screens; one is showing desiredtemperature and another current temperature.2 – Block with thermocouple. Inside <strong>of</strong> this block,beside thermocouple, there is a system for heatingand probe for temperature measurement. Also, inthis part <strong>of</strong> tribometer the contact between objectand block is made.3 – Counterweight. This part enables to makerotating <strong>of</strong> the block with thermocouple with verygood precision.Figure 2 – Measurement instrumentation(1-Thermoregulator, 2-Counterweight,3-Block with thermocouple)The tests were performed with rolling balls <strong>of</strong>different diameters over channels with differentradius bends. Balls weight and balls diameter werein a range from 0.04 to 0.08N and from 2.32 to13mm respectively. Bend radius <strong>of</strong> the blockcovered a range from 2.5 to 8 mm. Balls and blockwere heated on selected temperatures, 20, 100, 150and 200°C. Chosen material for balls and block wassteel DIN 17230 (100Cr6) with hardness 62-66HRC. Hardness is achieved by quenching andtempering process. Ball roughness is Ra=0.002µm.The roughness <strong>of</strong> the block channels surface was ina range between: Ra=0.8-1µm. The figure 3 is adiagrammatic representation coefficient <strong>of</strong> rollingfriction dependence regarding temperature andnormal load.Figure 3 – Coefficient <strong>of</strong> rolling friction dependenceregarding temperature and normal load398 13 th International Conference on Tribology – Serbiatrib’13

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