BearingLab rolling bearing life
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1. A bearing does not break — it wears out statistically

Almost every other component in this collection has a strength you check against: a stress, a limit, a safety factor. A rolling bearing does not work that way. Under a load it can perfectly well carry, it will still eventually fail by rolling contact fatigue — and two identical bearings, in identical machines, will fail at wildly different times.

So the rating is not "will it hold" but "how long". L₁₀ is the life that 90 % of a population reaches: one in ten will have spalled before it, and the median life is roughly five times longer.

L10 = ( CP )p   [million revolutions]ISO 281
  • C — the basic dynamic load rating, off the catalogue page. It is defined as the load that gives exactly one million revolutions of L₁₀ life, so the equation is really just a scaling from that definition.
  • P — the equivalent dynamic load, which is chapter 3.
  • p — 3 for ball bearings, 10/3 for roller bearings.
2468101101001000 roller, p = 10/3 ball, p = 3 load ratio C / P L₁₀ [million revolutions]
The life curve is brutally steep — the vertical axis is logarithmic. Doubling the load ratio multiplies the life by eight for a ball bearing. Which is the same statement read backwards: a 25 % load increase costs half the life.

Why the exponent differs

A ball touches its race at a point, a roller along a line. The line spreads the same force over more material, so the stress rises more slowly with load — which comes out as the gentler exponent. It is the same reason a roller bearing of the same size carries more.

Read the curve backwards. The interesting direction is not "how much life do I gain by oversizing" but "how much do I lose by underestimating the load". A load 25 % above what you assumed halves the life of a ball bearing. Load estimation is where bearing calculations actually go wrong.

Formulas in this chapter

L₁₀ — basic rating life
L₁₀ = (C/P)^p; p = 3 ball, 10/3 roller [Mrev] ISO 281