12.07.2015 Views

Report - PEER - University of California, Berkeley

Report - PEER - University of California, Berkeley

Report - PEER - University of California, Berkeley

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

instantaneous period <strong>of</strong> vibration and receives the energy from a set <strong>of</strong> wavecomponents which correspond to a set <strong>of</strong> instantaneous period <strong>of</strong> structure. As aresult, the energy spectrum is obtained from the energy spectrum <strong>of</strong> the purely elasticsystem through an averaging (smoothing) process. The period which represents a set<strong>of</strong> instantaneous period is termed to be the effective period. The effective period <strong>of</strong>the damped elastic system is equal to the natural period, since the instantaneousperiod spreads around the natural period. The effective period <strong>of</strong> the inelastic systembecomes longer than the initial natural period, since the inelastic system is s<strong>of</strong>tenedby the plastification. The energy spectrum for design use must reflect the influence <strong>of</strong>the nonlinearity. The nonlinearity which corresponds to the 10% <strong>of</strong> the fraction <strong>of</strong> thecritical damping was found to represent the averaging effect met in the practicalstructures.Thus, the energy spectrum <strong>of</strong> the elastic system with 10% <strong>of</strong> fraction <strong>of</strong> criticaldamping is referred to be the energy spectrum for design use. The effective period isinfluenced by the type <strong>of</strong> restoring force characteristic and the level <strong>of</strong> nonlinearity.In this paper, the effective period is derived theoretically and the effectiveness <strong>of</strong>the effective period is verified by comparing the result <strong>of</strong> the direct response analysesand the energy spectra for design use (Akiyama, 1985).2. ENERGY SPECTRUMThe energy input into a single degree <strong>of</strong> freedom system subjected to a horizontalground motion is written as−∫tE000= Mz && dy(1)where E is the total energy input, M the total mass <strong>of</strong> the system, & z& 0 the horizontalground acceleration, y the horizontal displacement <strong>of</strong> the mass relative to the groundand t 0 the duration time <strong>of</strong> the ground motion. The energy spectrum is defined by thefollowing functions.E(Te)Es (Te) = , (2)M2E(Te)Es (Te) = VE(Te) =(3)Mwhere E s is the energy spectrum and T e the effective period.Eq. (2) is the direct expression <strong>of</strong> the total energy input per unit mass versus theeffective period. Eq (3) is the equivalent velocity expression <strong>of</strong> the direct energyspectrum.The energy spectrum <strong>of</strong> the purely elastic system is denoted by 0 E s . The energyspectra <strong>of</strong> the damped elastic system and the inelastic system can be described asfollows, based on the energy spectrum <strong>of</strong> the purely elastic system.For the damped elastic system,386

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!