Start from the soil, not the code
Before any partial factor or α-value, a bored pile is a load-transfer problem. Everything in the code is a calibrated proxy for the physics underneath.
The two load paths
- Shaft friction — shear mobilised at the pile–soil interface as the pile tries to move down relative to the clay.
- End bearing — compression under the base.
Shaft friction mobilises at small displacement (~1% of diameter); end bearing needs ~10%. So at working load a bored pile in London clay carries almost everything on its shaft — the base is barely engaged. That fact, which the α/Nc equations hide, is why slender friction piles work and why leaning on end bearing is a trap.
Why London clay behaves the way it does
London clay is heavily overconsolidated — buried far deeper in geological history than now. That gives high strength but also fissuring: relief cracks that admit water and drop the operative strength below an intact triaxial sample.
The code hands you . First principles tell you why: boring the hole remoulds and softens a thin annulus at the interface and water migrates in, cutting effective stress — so mobilised adhesion is roughly half the intact undrained strength. Understand that and you know when to push α up (dry, fast, low-fissure) and when to pull it down (bentonite, delays, fissured horizons) — instead of blindly taking the table.
The brave bit (where chartered judgement lives): the code is the floor. When first principles and a load test justify it, a chartered geotechnical engineer can defend an α above the tabulated value — or insist on one below it where the ground says so. That judgement, not the equation, is the value.