Introduced nearly 50 years ago, pot bearings are now in service in thousands of structures throughout the USA and the world. There are good reasons for this popularity, all stemming from the confined elastomer principle.
A rubber pad, when tightly confined within a steel “pot,” will support an almost limitless stress. Tests to 57,000 psi show absolutely no change in the structure of the material.
Because rubber undergoes no change in its volume when loaded (Poisson’s ratio = 0.5), there is virtually no compression under load.
If a freely loaded plate, bearing on such a pad, is tilted, the rubber flows within the confined space with almost no resistance to the rotation. Since the rubber reacts like a viscous fluid, pressure is uniformly distributed within the closed system. Figure 1 illustrates the complete system.
Practical bearings using this principle can be designed for any combination of loads (including uplift), angle of rotation, or horizontal load found in today’s bridges. Only pot bearings have all the following performance advantages:
Also note that spherical bearings are sensitive to large horizontal loads, which can cause the convex part of the bearing to “ride up” out of its socket and, in extreme cases, pop out.
Expansion pot bearings feature slide interfaces of PTFE/stainless steel. The pot bearing works particularly well with a PTFE slide surface for several reasons. Many factors affect the coefficient of friction, but it has been found to decrease with increasing pressure.
However, excessive pressures would cause the PTFE to cold flow. An ideal balance is struck at about the same pressure at which a pot bearing operates. Also, the very small load eccentricity under rotation of the pot bearing provides the lowest possible edge loading. Finally, the even pressure distribution inherent in the hydraulic principle of the pot ensures the lowest peak pressures on the PTFE.
Pot bearings have the additional advantages of compact size, low overall height, and efficient use of materials.