CyberShake Study 22.12: Difference between revisions
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| [[File:WNGC_8686_v_4293_scatter_colorbymag_3sec.png|thumb| | | [[File:WNGC_8686_v_4293_scatter_colorbymag_3sec.png|thumb|600px|Scatter plot comparing the mean 3sec RotD50 for each rupture, between v3.3.1 and v5.4.2]] | ||
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| [[File:WNGC_8686_v_4293_scatter_colorbymag_3sec_noSAFM8.png|thumb| | | [[File:WNGC_8686_v_4293_scatter_colorbymag_3sec_noSAFM8.png|thumb|600px|Scatter plot comparing the mean 3sec RotD50 for each rupture, between v3.3.1 and v5.4.2, SAF events>M8 excluded]] | ||
|- | |- | ||
| [[File:WNGC_8686_v_4293_scatter_colorbymag_3sec_noSAFM7_5.png|thumb| | | [[File:WNGC_8686_v_4293_scatter_colorbymag_3sec_noSAFM7_5.png|thumb|600px|Scatter plot comparing the mean 3sec RotD50 for each rupture, between v3.3.1 and v5.4.2, SAF events>M7.5 excluded]] | ||
|} | |} | ||
USC, PAS, and STNI also all see larger ground motions at 2-3 seconds from these same events, but the effect isn't as strong, so it only shows up in the tails of the hazard curves. | |||
We honed in on source 68, rupture 7, a M8.45 on the southern San Andreas which produced the largest WNGC ground motions at 3 seconds, up to 5.1g. We calculated spectral plots for v3.3.1 and v5.4.2 for all 4 sites: | |||
USC | {| | ||
! Site !! v3.3.1 !! v5.4.2 | |||
|- | |||
! WNGC | |||
| [[File:WNGC_3861_v3.3.1_spectral_s68_r7.png|thumb|300px]] | |||
| [[File:WNGC_8685_v5.4.2_spectral_s68_r7.png|thumb|300px]] | |||
|- | |||
! USC | |||
| [[File:USC_3970_v3.3.1_spectral_s68_r7.png|thumb|300px]] | |||
| [[File:USC_8691_v5.4.2_spectral_s68_r7.png|thumb|300px]] | |||
|- | |||
! PAS | |||
| [[File:PAS_3878_v3.3.1_spectral_s68_r7.png|thumb|300px]] | |||
| [[File:PAS_8687_v5.4.2_spectral_s68_r7.png|thumb|300px]] | |||
|- | |||
! STNI | |||
| [[File:STNI_3873_v3.3.1_spectral_s68_r7.png|thumb|300px]] | |||
| [[File:STNI_8689_v5.4.2_spectral_s68_r7.png|thumb|300px]] | |||
|[ | |||
== High-frequency codes == | == High-frequency codes == | ||
Revision as of 20:53, 2 November 2022
CyberShake Study 22.10 is a proposed study in Southern California which will include deterministic low-frequency (0-1 Hz) and stochastic high-frequency (1-50 Hz) simulations. We will use the Graves & Pitarka (2022) rupture generator and the high frequency modules from the SCEC Broadband Platform v22.4.
Status
This study is in the planning phase. We estimate calculations will begin in October 2022.
Data Products
Data products will be posted here when the study is completed.
Science Goals
The science goals for this study are:
- Calculate a regional CyberShake model for southern California using an updated rupture generator.
- Calculate an updated broadband CyberShake model.
- Sample variability in rupture velocity as part of the rupture generator.
Technical Goals
The technical goals for this study are:
- Use an optimized OpenMP version of the post-processing code.
- Bundle the SGT and post-processing jobs to run on large Condor glide-ins, taking advantage of queue policies favoring large jobs.
Sites
We will use the standard 335 southern California sites (same as Study 21.12). The order of execution will be:
- Sites of interest
- 20 km grid
- 10 km grid
- Selected 5 km grid sites
Velocity Model
We are planning to use CVM-S4.26 with a GTL applied, and the CVM-S4 1D background model outside of the region boundaries.
We are investigating applying the Ely-Jordan GTL down to 700 m instead of the default of 350m. We extracted profiles for a series of southern California CyberShake sites, with no GTL, a GTL applied down to 350m, and a GTL applied down to 700m.
Sites (the CVM-S4.26 basins are outlined in red):
These are for sites outside of the CVM-S4.26 basins:
| Site | No GTL | 700m GTL | Smaller value, extracted from mesh |
|---|---|---|---|
| LAPD | |||
| s764 | |||
| s568 | |||
| s035 | |||
| PERR | |||
| MRVY | |||
| s211 |
These are for sites inside of the CVM-S4.26 basins:
| Site | No GTL | 700m GTL | Smaller value |
|---|---|---|---|
| s117 | |||
| USC | |||
| WNGC | |||
| PEDL | |||
| SBSM | |||
| SVD |
Proposed Algorithm
Our proposed algorithm for generating the velocity model is as follows:
- Set the surface mesh point to a depth of 25m.
- Query the CVM-S4.26.M01 model ('cvmsi' string in UCVM) for each grid point.
- Calculate the Ely taper at that point using 700m as the transition depth.
- Compare the values before and after the taper modification; at each grid point down to the transition depth, use the value from the method with the lower Vs value.
- Check values for Vp/Vs ratio, minimum Vs, Inf/NaNs, etc.
Value constraints
We impose the following constraints on velocity mesh values:
- Vp >= 1700 m/s. If lower, Vp is set to 1700.
- Vs >= 500 m/s. If lower, Vs is set to 500.
- rho >= 1700 km/m3. If lower, rho is set to 1700.
- Vp/Vs >= 1.45. If not, Vs is set to Vp/1.45.
We will add the following additional constraints:
- If Vs<500 m/s, calculate the Vp/Vs ratio, set Vs=500, then set Vp=Vs*(Vp/Vs ratio).
- Apply Vp clamp after Vs check.
Cross-sections
Below are cross-sections of the TEST site velocity model at depths down to 600m for CVM-S4.26.M01, the taper to 700m, the lesser of the two values, and the % difference.
Note that the top two slices use a different color scale.
| Depth | CVM-S4.26.M01 | Ely taper to 700m | Selecting smaller value | % difference, smaller value vs S4.26.M01 |
|---|---|---|---|---|
| 0m (queried at 25m depth) | ||||
| 100m | ||||
| 200m | ||||
| 300m | ||||
| 400m | ||||
| 500m | ||||
| 600m |
Implementation details
To support the Ely taper approach where the smaller value is selected, the following algorithmic changes were made to the CyberShake mesh generation code. Since the UCVM C API doesn't support removing models, we couldn't just add the 'elygtl' model - it would then be included in every query, and we need to run queries with and without it to make the comparison. We also must include the Ely interpolator, since all that querying the elygtl model does is populates the gtl part of the properties with the Vs30 value, and it's the interpolator which takes this and the crustal model info and generates the taper.
- The decomposition is done by either X-parallel or Y-parallel stripes, which have a constant depth. Check the depth to see if it is shallower than the transition depth.
- If so, initialize the elygtl model using ucvm_elygtl_model_init(), if uninitialized. Set the id to UCVM_MAX_MODELS-1. There's no way to get model id info from UCVM, so we use UCVM_MAX_MODELS-1 as it is 29, we are very unlikely to load 29 models, and therefore unlikely to have an id conflict.
- Change the depth value of the points to query to the transition depth. This is because we need to know the crustal model Vs value at the transition depth, so that the Ely interpolator can match it.
- Query the crustal model again, with the modified depths.
- Modify the 'domain' parameter in the properties data structure to UCVM_DOMAIN_INTERP, to indicate that we will be using an interpolator.
- Change the depth value of the points to query back to the correct depth, so that the interpolator can work correctly on them.
- Query the elygtl using ucvm_elygtl_model_query() and the correct depth.
- Call the interpolator for each point independently, using the correct depth.
- For each point, choose to use either the original crustal data or the Ely taper data, depending on which has the lower Vs.
In the future we plan for this approach to be implemented in UCVM, and we can simplify the CyberShake query code.
Rupture Generator
In determining what rupture generator to use for this study, we performed tests with WNGC, USC, PAS, and STNI, and compared hazard curves generated with v5.4.2 to those from Study 15.4:
| Site | 2 sec | 3 sec | 5 sec | 10 sec |
|---|---|---|---|---|
| WNGC | ||||
| USC | ||||
| PAS | ||||
| STNI |
Digging in further, it appears the elevated hazard curves for WNGC at 2 and 3 seconds are predominately due to large-magnitude southern San Andreas events producing larger ground motions.
USC, PAS, and STNI also all see larger ground motions at 2-3 seconds from these same events, but the effect isn't as strong, so it only shows up in the tails of the hazard curves.
We honed in on source 68, rupture 7, a M8.45 on the southern San Andreas which produced the largest WNGC ground motions at 3 seconds, up to 5.1g. We calculated spectral plots for v3.3.1 and v5.4.2 for all 4 sites:










































































































