Development of large-scale journal bearing test setup
Abstract
Due to the rising demand for green energy, wind turbines are often installed in offshore locations where the wind is stronger. Floating platforms are secured to the seabed using mooring lines and anchors. Self-lubricating journal bearings are installed to accommodate the platform's oscillating movement caused by waves and wind and to mitigate the potential environmental impact of leaking lubricants. These compact bearings with high-load low-velocity characteristics, and maintenance-free operation, serve as a replacement for traditional roller bearings. Other offshore uses for these plain bearings include hydropower plants and the submerged stern tubes of cargo ships. To optimize the efficiency and reliability of these self-lubricating bearings, it is crucial to gain insight into their tribological characteristics. Small-scale testing may not provide representative results as the size effect is not taken into account. Due to the complex interactions, (running-in/out, sliding layer formation, edge effect, roughness changes, ...) large-scale tests are needed to accurately describe real-life behaviour as well as possible. Therefore, a full-scale test rig is designed to accurately replicate the enormous mooring line forces and the complex tribological interactions encountered in real-life applications. In the basic working principle of the developed machine, a shrink disc secures the lever arm, which transfers the displacement piston's motion to the shaft. During the test, the displacement of both pistons, the radial load, the load applied on the movement lever arm, and the resulted torque load are measured. Displacement laser sensors are used to measure the movement of the shaft with respect to the test bearing to qualitatively estimate the wear over time. The coefficient of friction (CoF) of these self-lubricating bearings could be obtained through two methods. The initial test results were evaluated and an asymmetric CoF behaviour was found. The static CoF was reported as the maximum value of friction during the first 25% of each stroke, and the average of the forward and backward stroke within each cycle. The dynamic CoF was reported as the average value of friction during the middle 33% of each stroke, and the average of the forward and backward stroke within each cycle