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Liquefaction Model — Geospatial GLM Surrogate

1. What the model computes (and what it does not)

The product is the probability and areal extent of liquefaction and its surface manifestation severity, served in three framings (§4): conditional on a ground motion, unconditional over a return period, and for a specific event. A geospatial model trades per-site borehole data for spatially continuous proxies — predicting liquefaction from PGV/PGA, Vs30V_{s30}, water-table depth, precipitation, and distance to water Zhu et al., 2015Zhu et al., 2017 — so it covers regions where site investigations do not exist.

What the model does not do: it does not replace site-specific CPT/SPT triggering analysis at an engineered site; it does not solve transient 3-D groundwater flow (it consumes a water-table field, §6); and it does not by itself produce ground motion — that comes from a ShakeMap (event) or the NSHM (probabilistic), §4–§5.

2. The physics — the equations we solve

The simplified procedure Seed & Idriss, 1971Idriss & Boulanger, 2006 compares seismic demand to soil capacity. The cyclic stress ratio (demand) is

CSR=0.65amaxgσv0σv0rd,\mathrm{CSR} = 0.65\,\frac{a_{max}}{g}\,\frac{\sigma_{v0}}{\sigma'_{v0}}\,r_d ,

the cyclic resistance ratio CRR\mathrm{CRR} is the capacity, and triggering is expected when the factor of safety

FSliq=CRRCSR1.\mathrm{FS}_{liq} = \frac{\mathrm{CRR}}{\mathrm{CSR}} \le 1 .

Surface severity is summarized by manifestation indices — the Liquefaction Potential Index Iwasaki et al., 1978 and the Liquefaction Severity Number Ballegooy et al., 2014. Two Pillar-1 state variables enter directly:

3. The geospatial surrogate — what is solved vs. assumed

Classical triggering (§2) is evaluated per soil column. The geospatial model regresses the outcome (liquefaction occurrence / manifestation) on spatially available proxies, and GAIA’s GLM uses the mechanics-informed ML surrogate of Sanger et al., 2025, which emulates physics-based triggering at national scale and in near-real time, demonstrated for the PNW in Sanger & Maurer, 2026.

ElementWhat it solvesWhat it assumes
Geospatial predictors → P(liq)P(\text{liq})logistic / ML mapping from PGV, Vs30V_{s30}, water table, precip, distance-to-water Zhu et al., 2017proxies stand in for unmeasured geotechnical state; training-region transferability Rashidian & Baise, 2020
Mechanics-informed surrogatefast emulation of the simplified-procedure FS over a region Sanger et al., 2025the surrogate is trained on / constrained by the mechanics; valid within its training envelope
Manifestation modelfragility from FS / LPI to damage state Geyin & Maurer, 2020Geyin et al., 2020Maurer et al., 2015surface manifestation is a function of integrated triggering + site
VsV_s fieldparametric CONUS VsV_s profiles Sanger & Maurer, 2025functional form + geospatial ML capture the near-surface profile

The surrogate’s value is speed and coverage: it runs the conditional model everywhere, fast enough for the unconditional integral (§4) and for Earth2Studio ensembles (§7).

4. The three hazard framings

A GLM digital twin must serve three distinct questions, each with different ground-motion input and data/model need:

FramingQuestionGround-motion inputOutputData / model need
Conditional (national)P(liqIM)P(\text{liq}\mid IM) — given shakinga specified IM (PGA/PGV)probability / extent given that IMthe national GLM surrogate Sanger et al., 2025; high-res Vs30V_{s30}, water table, geology
Unconditional (return period)total liquefaction hazard in TT yearsintegrated over the NSHM hazard curvereturn-period liquefaction hazardλliq=P(liqIM)dλ(IM)\lambda_{liq}=\int P(\text{liq}\mid IM)\,\lvert d\lambda(IM)\rvert; NSHM curves Petersen et al., 2024 via gaia-nhsm-deagg
Event-based (scenario)liquefaction footprint of this quakea ShakeMap IM fielddeterministic spatial maprupture → ShakeMap → GLM; the nowcasting mode

The unconditional product is the “total risk for a return period” baseline; the event-based product is the real-time nowcast for a specific rupture (e.g. a Cascadia or Nisqually scenario). All three call the same conditional surrogate — they differ only in how the ground motion is supplied and integrated.

5. Attenuation, κ0\kappa_0, and the NSHM

High-frequency ground motion — and therefore amaxa_{max} — is controlled by attenuation, parameterized by the site spectral-decay term κ0\kappa_0 Anderson & Hough, 1984. Two questions the GAIA seismic networks help answer:

Open integration question. The NSHM embeds a fixed reference-rock κ0\kappa_0 and Vs30V_{s30} site term Petersen et al., 2024; how to feed a time-varying site term (κ0(t)\kappa_0(t), Vs(t)V_s(t)) back into the hazard input for the unconditional product (§4) is unresolved and a GAIA research target.

6. Coupling map — where the other GAIA projects plug in

(a) Soil reanalysis (Pillar 1, Soil Hydromechanical Memory). The water-table depth dwt(x,t)d_{wt}(x,t) and saturation SwS_w are the dynamic liquefaction controls (§2); the seismic dv/vdv/v inversion also delivers a time-varying VsV_s for both the capacity term and the site amplification. This is the direct line from the reanalysis to liquefaction susceptibility, and the route by which sea-level rise and seasonal water-table change modulate hazard (via the groundwater modeling).

(b) The landslide model (Landslide Model — Landlab Implementation). Liquefaction and landslides share the same antecedent hydromechanical state — saturation and water table — but couple it to a seismic trigger (PGA/PGV) rather than rainfall recharge. The landslide engine’s Monte-Carlo-over-uncertain-strength structure is the template the liquefaction surrogate mirrors: both are “soil state + trigger → probability of failure.”

(c) Earthquake wavefields & the NSHM. The ground-motion field comes from ShakeMap (event) or the NSHM (probabilistic, via gaia-nhsm-deagg); GAIA’s wavefield reconstruction/forecasting work is the natural source of refined, possibly time-varying, site ground motion.

7. Interoperability with Earth2Studio

The dynamic half of the GLM twin needs forecast forcing, routed through Earth2Studio — the same AI weather/climate stack the landslide model and Pillar 3 forecasting use:

8. Evaluation & metrics

As for the landslide model, separate calibration of intermediate states from validation of the prediction; full metric definitions live in HazEvalHub.

9. Repositories (placeholders — for Morgan to confirm)

Proposed repositories do not exist yet — the names are placeholders for the team to create/confirm.

References

References
  1. Sanger, M. D., Geyin, M., & Maurer, B. W. (2025). Mechanics-Informed Machine Learning for Geospatial Modeling of Soil Liquefaction: Global and National Surrogate Models for Simulation and Near-Real-Time Response. Journal of Geotechnical and Geoenvironmental Engineering, 151(11), 04025126. 10.1061/JGGEFK.GTENG-13737
  2. Sanger, M. D., & Maurer, B. W. (2026). Geospatial AI for liquefaction hazard and impact forecasting: A demonstrative study in the U.S. Pacific Northwest. Geodata and AI, 7, 100069. 10.1016/j.geoai.2026.100069
  3. Zhu, J., Daley, D., Baise, L. G., Thompson, E. M., Wald, D. J., & Knudsen, K. L. (2015). A Geospatial Liquefaction Model for Rapid Response and Loss Estimation. Earthquake Spectra, 31(3), 1813–1837. 10.1193/121912EQS353M
  4. Zhu, J., Baise, L. G., & Thompson, E. M. (2017). An Updated Geospatial Liquefaction Model for Global Application. Bulletin of the Seismological Society of America, 107(3), 1365–1385. 10.1785/0120160198
  5. Seed, H. B., & Idriss, I. M. (1971). Simplified Procedure for Evaluating Soil Liquefaction Potential. Journal of the Soil Mechanics and Foundations Division, 97(9), 1249–1273. 10.1061/JSFEAQ.0001662
  6. Idriss, I. M., & Boulanger, R. W. (2006). Semi-empirical procedures for evaluating liquefaction potential during earthquakes. Soil Dynamics and Earthquake Engineering, 26(2–4), 115–130. 10.1016/j.soildyn.2004.11.023
  7. Iwasaki, T., Tatsuoka, F., Tokida, K., & Yasuda, S. (1978). A Practical Method for Assessing Soil Liquefaction Potential Based on Case Studies at Various Sites in Japan. Proc. 2nd Int. Conf. on Microzonation for Safer Construction, 2, 885–896.
  8. van Ballegooy, S., Malan, P., Lacrosse, V., Jacka, M. E., Cubrinovski, M., Bray, J. D., O’Rourke, T. D., Crawford, S. A., & Cowan, H. (2014). Assessment of Liquefaction-Induced Land Damage for Residential Christchurch. Earthquake Spectra, 30(1), 31–55. 10.1193/031813EQS070M
  9. Andrus, R. D., & Stokoe, K. H. (2000). Liquefaction Resistance of Soils from Shear-Wave Velocity. Journal of Geotechnical and Geoenvironmental Engineering, 126(11), 1015–1025. 10.1061/(ASCE)1090-0241(2000)126:11(1015)
  10. Rashidian, V., & Baise, L. G. (2020). Regional efficacy of a global geospatial liquefaction model. Engineering Geology, 272, 105644. 10.1016/j.enggeo.2020.105644
  11. Geyin, M., & Maurer, B. W. (2020). Fragility Functions for Liquefaction-Induced Ground Failure. Journal of Geotechnical and Geoenvironmental Engineering, 146(12), 04020142. 10.1061/(ASCE)GT.1943-5606.0002416
  12. Geyin, M., Baird, A. J., & Maurer, B. W. (2020). Field assessment of liquefaction prediction models based on geotechnical versus geospatial data, with lessons for each. Earthquake Spectra, 36(3), 1386–1411. 10.1177/8755293019899951
  13. Maurer, B. W., Green, R. A., & Taylor, O.-D. S. (2015). Moving towards an improved index for assessing liquefaction hazard: Lessons from historical data. Soils and Foundations, 55(4), 778–787. 10.1016/j.sandf.2015.06.010
  14. Sanger, M. D., & Maurer, B. W. (2025). Parametric modeling of shear wave velocity profiles for the conterminous U.S. 10.48550/arXiv.2510.00372
  15. Petersen, M. D., Shumway, A. M., Powers, P. M., Field, E. H., Moschetti, M. P., Jaiswal, K. S., & others. (2024). The 2023 US 50-State National Seismic Hazard Model: Overview and implications. Earthquake Spectra, 40(1), 5–88. 10.1177/87552930231215428