Published at : 06 Oct 2021
Volume : IJtech
Vol 12, No 4 (2021)
DOI : https://doi.org/10.14716/ijtech.v12i4.4674
Jhonni Rahman | Department of Mechanical Engineering, Faculty of Engineering, Universitas Islam Riau, Jl. Kaharuddin Nst. No. 113, Simpang Tiga, Kec. Bukit Raya, Kota Pekanbaru 28284, Riau, Indonesia |
Yutaka Shoukaku | Division of Mechanical Science and Engineering, Graduate School of Natural Science and Technology, Kanazawa University, Kakuma-machi, Kanazawa 920-1192, Ishikawa, Japan |
Tomoaki Iwai | Division of Mechanical Science and Engineering, Graduate School of Natural Science and Technology, Kanazawa University, Kakuma-machi, Kanazawa 920-1192, Ishikawa, Japan |
An experimental study was conducted to evaluate the
effect of the applied load and moving speed on the free rotating rubber
specimen contact area on a smooth-surfaced glass plate. The contact area of the
rubber specimen and flat surface was observed using fluorescence microscopy by
utilizing ultraviolet as an excitation light source and pyranine as a dye
substance. The apparent contact area between the rubber specimen and the flat
surface was measured using image processing software based on the Otsu
thresholding method. The result reveals an increasing
trend line due to applied normal load dependency, which agreed with the Hertz
theory. On moving-speed influence, the trend line of rubber contact increased
at a lower speed, reaching the highest value at a moving speed of 8 mm/s, and decreased
as the moving speed increased further.
Apparent contact area; Fluorescence; Free rotating; Rubber
Since the past few decades,
many scientists have been conducting several experiments related to the contact
mechanics of soft materials due to their significant applications in many
industries (Nakajima and Takahashi, 2002; Fujii, 2008; Bódai and
Goda, 2012; Fowell et al., 2014). One of them is the research about rubber tires of
vehicles. The important role of a tire in the vehicle system can be
comprehended as its function in transmitting forces on the vehicle through tire
rubber to the road surface in a safe and comfortable manner. Therefore,
traction force or grip between the tire and road surface becomes one of the
most important performance characteristics needed to understand in the
automotive industry (Liang et al., 2020). For example, it helps us to understand what range of
friction is needed to keep the vehicles safe when braking or cornering or how
fast the vehicle can be utilized to maintain the vehicle under control. If the
frictional characteristics fail to satisfy the required tractional force, then
the entire system of the vehicle will be out of control, leading to a car
accident.
In
general, the grip performance of rubber tires is affected by both internal and
external factors. One internal factor is the filler inside the tire, which
greatly affects its performance. Thus, enhancing the quality of the filler
enables the tire to increase its grip performance. This result was reported by Hasan et al. (2020) in their study about the
properties of tire rubber by modifying the clay filler of tires.
Similarly, external factors such as moving
speed and loads on vehicles also have a significant impact on vehicle
performance. The more weight is loaded on the vehicle, the faster the tire wears
down. Faster vehicle runs cause the driver to lose control easily. Therefore,
studying these two factors is vital to maintain the tire life and also for driving
safety. Although the importance of tire grip performance is applied on both dry
and wet surface conditions, its influence is much more reduced on wet surfaces.
This phenomenon was shown in a report from Micheline Corporation (Michelin, 2001). Zheng et al. also reported
similar results, as the adhesion coefficient reduced when the tire ran on a wet
surface, and it reduced further as the water thickness increased (Zheng et al., 2018). Due to its significant
impact on the grip performance of tires, we decided to observe and measure the
contact condition of tire rubber on wet surfaces.
Tire grip performance or the
coefficient of friction is generally calculated based on frictional force, as
stated in “laws of friction.” It was reported that the friction force (F?)
of elastomer contact is generally produced by two types of forces: adhesion
force (Fa) and hysteresis force (Fh) (Tabor, 1960). Thus, frictional force can be
expressed as follows:
However, in rough surface
contacts such as between the tire and road surface, the most dominant factor on
the friction force is hysteresis force; in contrast, the effect of adhesion
force is very minimal (Persson, 2001). On
the other hand, when the surface of rubber contact is very smooth, the adhesion
force makes the biggest contribution to the friction force (Persson and Volokitin, 2006). As the current
study utilized a smooth surface of both the rubber wheel and glass plate, the
frictional force solely depends on the adhesion force. Thus, the coefficient of
friction can be expressed as follows:
Maegawa et al.
(2015) reported that the correlation
between kinetic friction force and the contact area of the elastomer was
linear. Therefore, the frictional force of the elastomer can also be measured based
on the contact area between the rubber tire and the mating surface. The
coefficient of friction of adhesion force can be expressed as follows:
where ? is the shear strength and A is
the contact area between the elastomer and the mating surface. As the shear
strength does not change, the only factor affecting the adhesion force is the elastomer
contact area. This means that the contact area of tire rubber determines the
amount of frictional force of the vehicles in a certain manner.
The only way to directly observe
the contact condition in situ is by using visualization methods such as fluorescence
microscopy. Fluorescence microscopy is the best method for observing and
measuring the contact area of elastomer material. Fluorescence microscopy provides
detailed information based on the amount of fluorescence dye that exists within
the contacting parts. Therefore, the intensity produced in fluorescence microscopy
represents the gap within mating contact. Moreover, differentiating the contact
region and noncontact region is becoming easier and more accurate. There are
several samples of fluorescence microscopy applications in the field of
tribology. For example, Fowell et al. (2014)
used fluorescence microscopy on elastomeric seal material to measure the lubricant
film thickness of contact area at several entrainment speeds. Petrova et al. (2019) utilized fluorescence
microscopy to visualize solid-to-solid contact regimes. As it is a very
sensitive observation method, the fluorescence technique is also used more
frequently in other fields of studies, such as chemistry (Rozaini
et al., 2012), biology (Hötzer et al., 2012), and medicine (Marcu, 2012).
As the contact condition of tires is closely related to the coefficient of friction and the grid performance of tires, a lot of data is required to design and produce better performing tires. The information about the contact condition of tires can also be used to analyze the condition of tire wear, to predict the lifetime of tires, and for some other purposes. However, the currently existing reports and data are still far from enough to satisfy the needs of data on many circumstances of tire contact conditions. One of them is the contact condition of rubber tires due to the influence of moving speeds and applied loads on wet surfaces.
Therefore, to contribute to providing data for these purposes, this study conducted an experiment to investigate how the applied loads and moving speeds affect the contact condition of rubber tires. As a fundamental study, the experiment was carried out as a rubber tire wheel running on the top of the flat surface of a glass plate under several applied loads and moving speeds. The contact condition of the tire and mating surface was observed using the ultraviolet-induced fluorescence technique. The moving speed in this study indicates free rotation, which is a mixed movement of rolling and sliding. The rubber wheel had the same material as the tire rubber of regular vehicles, and the mating surface was a smooth glass plate (BK7). During the experiment, the fluorescence liquid made of the pyranine-dyed solution was covered on the top of the mating surface, simulating the condition of wet surfaces.
The
effect of the applied load and moving speed on the free rotating rubber
specimen contact area on a smooth-surfaced glass plate was studied. The results
indicate different tendencies between applied-load and moving-speed
dependencies. Regarding applied-load dependency, the plot distribution of the rubber
specimen apparent contact area was within the 20 mm2 range for each
applied load from three tests. Overall, the apparent contact area increased linearly
as the applied load increased in the graph with the log–log axis. This result
fits the function of the Hertz theory, as the half-width of the contact area is
proportional to the applied load in the power of ½. Regarding moving-speed
influences, some information can be obtained from the results. First, the applied
load also increased the apparent contact area of the rubber specimen. Second,
the moving speed of the rubber specimen increased the rubber apparent contact
area at a lower speed up to 8 mm/s, and then it decreased as the moving speed
increased further.
This work was supported by the Indonesia Endowment Fund for Education
(LPDP), the Ministry of Finance of Republic Indonesia (KEMENKEU), the Ministry
of Research and Technology of Republic Indonesia (KEMENRISTEK), and the
Ministry of Education and Culture of Republic Indonesia (KEMENDIKBUD) in the
form of a scholarship for a doctoral degree at Kanazawa University with the
grand contract number PJR-1570/LPDP.4/2019. Also, thanks to TOYO TIRE for the financial
support and being a collaboration partner with the Tribology Laboratory of
Kanazawa University.
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