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🏢 Base Isolation Explorer

Instead of making a building strong enough to survive the shaking, disconnect it from the ground. Lead-rubber bearings lengthen the period far past the spectrum's dangerous plateau and dissipate energy in a fat hysteresis loop. The catch: the building now moves nearly a metre, and something has to accommodate that gap.

Isolation System

Building & Site

Live Result

—
Design displacement D—
Effective isolated period Teff—
Equivalent damping βeq—
Damping reduction η—
Base shear (isolated)—
Base shear if fixed-base at plateau—
Powered by bilinear isolator theory with the equivalent-linear (secant stiffness + equivalent viscous damping) method (engine/base-isolation.js). Verified before publishing: the equivalent damping computed from the hysteresis loop area matches the independently-stated closed form β = 2Qd(D−Dy)/(πKeffD²) to machine precision, η returns exactly 1.000 at the 5% reference damping, and the design displacement is solved by iteration then verified to satisfy its own defining equation — a genuine fixed point, not merely the last iterate. Keff is confirmed to always lie strictly between the post-yield and initial stiffness.

Method

Naeim & KellyBilinear lead-rubber bearing model; Keff = Kd + Qd/D, Wd = 4Qd(D−Dy).
EN 1998-1 §10Damping reduction η = √(0.10/(0.05+ξ)) ≥ 0.55.
Scope: equivalent-linear analysis of the isolation system only. Does NOT model superstructure flexibility, bidirectional interaction, velocity dependence, lead-core heating, bearing stability/buckling, or uplift — all of which matter in real isolation design. A teaching tool, not a bearing specification.
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Visual explanation

Vibration isolation at bridge bearings. Isolation lengthens the period into r > √2; acceleration transmitted to the superstructure falls
Figure 41. Vibration isolation at bridge bearingsSource: Kelly (1997), Earthquake-Resistant Design with Rubber; AASHTO / TBDY isolation provisions.