Evaluation of ASCE 7‑22 Equivalent Lateral Force Procedures: Method 2 Versus Method 1
Here we examine the differences between the two methods and compare the resulting seismic response coefficient values across a range of site classes, structural periods, and geographic regions.
ASCE 7‑22 introduced Method 1 for determining the seismic base shear in the Equivalent Lateral Force (ELF) procedure, based directly on multi‑period design response spectra, while retaining the traditional method of base shear calculation based on two‑period design response spectra as Method 2.
This paper evaluates the commonly held perception that Method 1 generally produces higher seismic base shear demands than Method 2 at short periods. Seismic response coefficients (design base shear divided by seismic weigh) were computed using both methods for 56 locations across the Western United States (WUS) and Central and Eastern United States (CEUS) for Site Classes A, B, C, D, and E. The results demonstrate that neither method is uniformly more conservative.
Method 1 produces higher base shear values at very short periods when spectral peaks occur below 0.2 s, a period range not representative of most building structures, whereas Method 2 often yields significantly higher base shear values at intermediate periods. At longer periods, differences diminish, and the two methods typically converge as minimum design base shear requirements of ASCE 7 govern. This study identifies the conditions under which one method may produce larger seismic response coefficients than the other and clarifies the influence of the shape of the multi‑period response spectrum on the calculated base shear.
The paper also discusses a proposed change for the 2027 International Building Code®, which is intended to mitigate the effects of short‑period spectral spikes present in the ASCE 7‑22 multi‑period design response spectra at periods below 0.2 s. This code change will effectively result in Method 1 and Method 2 producing identical base shear values up to the period at which the design spectral response acceleration reaches its maximum value and then decreases to SDS.



