Source code for openquake.hazardlib.gsim.bozorgnia_campbell_2016

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"""
Module exports :class:`BozorgniaCampbell2016`
               :class:`BozorgniaCampbell2016HighQ`
               :class:`BozorgniaCampbell2016LowQ`
               :class:`BozorgniaCampbell2016AveQJapanSite`
               :class:`BozorgniaCampbell2016HighQJapanSite`
               :class:`BozorgniaCampbell2016LowQJapanSite`
"""
import numpy as np
from openquake.hazardlib.gsim.base import GMPE, CoeffsTable
from openquake.hazardlib.gsim.campbell_bozorgnia_2014 import \
                                          CampbellBozorgnia2014 as CB14
from openquake.hazardlib import const
from openquake.hazardlib.imt import PGA, PGV, SA


[docs]class BozorgniaCampbell2016(GMPE): """ Implements the BC15 GMPE by Bozorgnia & Campbell (2016) for vertical-component ground motions from the PEER NGA-West2 Project This model follows the same functional form as in CB14 by Campbell & Bozorgnia (2014) with minor modifications to the underlying parameters. Note that this is a more updated version than the GMPE described in the original PEER Report 2013/24. **Reference:** Bozorgnia, Y. & Campbell, K. (2016). Vertical Ground Motion Model for PGA, PGV, and Linear Response Spectra Using the NGA-West2 Database. *Earthquake Spectra*, 32(2), 979-1004. Implements the global model that uses datasets from California, Taiwan, the Middle East, and other similar active tectonic regions to represent a typical or average Q region. Applies the average attenuation case (Dc20=0) """ #: Supported tectonic region type is active shallow crust DEFINED_FOR_TECTONIC_REGION_TYPE = const.TRT.ACTIVE_SHALLOW_CRUST #: Supported intensity measure types are spectral acceleration, peak #: ground velocity and peak ground acceleration DEFINED_FOR_INTENSITY_MEASURE_TYPES = set([ PGA, PGV, SA ]) #: Supported intensity measure component is the #: :attr:`~openquake.hazardlib.const.IMC.Vertical` direction component DEFINED_FOR_INTENSITY_MEASURE_COMPONENT = const.IMC.VERTICAL #: Supported standard deviation types are inter-event, intra-event #: and total; see the section for "Aleatory Variability Model". DEFINED_FOR_STANDARD_DEVIATION_TYPES = set([ const.StdDev.TOTAL, const.StdDev.INTER_EVENT, const.StdDev.INTRA_EVENT ]) #: Required site parameters are Vs30, Vs30 type (measured or inferred), #: and depth (km) to the 2.5 km/s shear wave velocity layer (z2pt5) REQUIRES_SITES_PARAMETERS = {'vs30', 'z2pt5'} #: Required rupture parameters are magnitude, rake, dip, ztor, rupture #: width and hypocentral depth REQUIRES_RUPTURE_PARAMETERS = { 'mag', 'rake', 'dip', 'ztor', 'width', 'hypo_depth'} #: Required distance measures are Rrup, Rjb and Rx REQUIRES_DISTANCES = {'rrup', 'rjb', 'rx'}
[docs] def get_mean_and_stddevs(self, sites, rup, dists, imt, stddev_types): """ See :meth:`superclass method <.base.GroundShakingIntensityModel.get_mean_and_stddevs>` for spec of input and result values. """ # Extract dictionary of coefficients specific to required IMT and PGA C = self.COEFFS[imt] C_PGA = self.COEFFS[PGA()] # Get mean and standard deviations for IMT mean = self.get_mean_values(C, sites, rup, dists) if imt.name == "SA" and imt.period < 0.25: # If Sa (T) < PGA for T < 0.25 then set mean Sa(T) to mean PGA # Get PGA on given sites pga = self.get_mean_values(C_PGA, sites, rup, dists) idx = mean < pga mean[idx] = pga[idx] # Get standard deviations stddevs = self._get_stddevs(C, rup, sites, stddev_types) return mean, stddevs
[docs] def get_mean_values(self, C, sites, rup, dists): """ Returns the mean values for a specific IMT """ if isinstance(sites.z2pt5, np.ndarray): # Site model defined temp_z2pt5 = sites.z2pt5 else: # Estimate unspecified sediment depth according to # equations 33 and 34 of CB14 temp_z2pt5 = self._select_basin_model(sites.vs30) return (self._get_magnitude_term(C, rup.mag) + self._get_geometric_attenuation_term(C, rup.mag, dists.rrup) + self._get_style_of_faulting_term(C, rup) + self._get_hanging_wall_term(C, rup, dists) + self._get_shallow_site_response_term(C, sites.vs30) + self._get_basin_response_term(C, temp_z2pt5) + self._get_hypocentral_depth_term(C, rup) + self._get_fault_dip_term(C, rup) + self._get_anelastic_attenuation_term(C, dists.rrup))
def _get_magnitude_term(self, C, mag): """ Returns the magnitude scaling term, f_mag, defined in equation 2 """ return CB14._get_magnitude_term(self, C, mag) def _get_geometric_attenuation_term(self, C, mag, rrup): """ Returns the geometric attenuation term, f_dis, defined in equation 3 """ return CB14._get_geometric_attenuation_term(self, C, mag, rrup) def _get_style_of_faulting_term(self, C, rup): """ Returns the style-of-faulting scaling term, f_flt, defined in equations 4 to 6 """ if (rup.rake > 30.0) and (rup.rake < 150.): frv = 1.0 fnm = 0.0 elif (rup.rake > -150.0) and (rup.rake < -30.0): fnm = 1.0 frv = 0.0 else: fnm = 0.0 frv = 0.0 # Re-defined this method to replace c8, which is now # IMT-dependent in BC15 fflt_f = (C["c8"] * frv) + (C["c9"] * fnm) if rup.mag <= 4.5: fflt_m = 0.0 elif rup.mag > 5.5: fflt_m = 1.0 else: fflt_m = rup.mag - 4.5 return fflt_f * fflt_m def _get_hanging_wall_term(self, C, rup, dists): """ Returns the hanging wall scaling term, f_hng, defined in equation 7 """ return CB14._get_hanging_wall_term(self, C, rup, dists) def _get_hanging_wall_coeffs_rx(self, C, rup, r_x): """ Returns the hanging wall r-x scaling term, f_hng_Rx defined in equation 8 """ return CB14._get_hanging_wall_coeffs_rx(self, C, rup, r_x) def _get_f1rx(self, C, r_x, r_1): """ Defines the f1 scaling coefficient defined in equation 9 """ return CB14._get_f1rx(self, C, r_x, r_1) def _get_f2rx(self, C, r_x, r_1, r_2): """ Defines the f2 scaling coefficient defined in equation 10 """ return CB14._get_f2rx(self, C, r_x, r_1, r_2) def _get_hanging_wall_coeffs_rrup(self, dists): """ Returns the hanging wall rrup term, f_hng_Rrup, defined in equation 13 """ return CB14._get_hanging_wall_coeffs_rrup(self, dists) def _get_hanging_wall_coeffs_mag(self, C, mag): """ Returns the hanging wall magnitude term, f_hng_M defined in equation 14 """ return CB14._get_hanging_wall_coeffs_mag(self, C, mag) def _get_hanging_wall_coeffs_ztor(self, ztor): """ Returns the hanging wall ztor term, f_hng_Z, defined in equation 15 """ return CB14._get_hanging_wall_coeffs_ztor(self, ztor) def _get_hanging_wall_coeffs_dip(self, dip): """ Returns the hanging wall dip term, f_hng_delta, defined in equation 16 """ return CB14._get_hanging_wall_coeffs_dip(self, dip) def _get_shallow_site_response_term(self, C, vs30): """ Returns the shallow site response term, f_site, defined in equations 17, 18, and 19 Note that the effects of nonlinear soil response for the vertical component were not included in this model """ vs_mod = vs30 / C["k1"] # Get linear global site response term f_site_g = C["c11"] * np.log(vs_mod) # For Japan sites (SJ = 1) further scaling is needed (equation 19) if self.CONSTS["SJ"]: fsite_j = C["c13"] * np.log(vs_mod) # additional term activated for soft sites (Vs30 <= 200m/s) # in Japan data idx = vs30 <= 200.0 add_soft = C["c12"] * (np.log(vs_mod) - np.log(200.0 / C["k1"])) # combine terms fsite_j[idx] += add_soft[idx] return f_site_g + fsite_j else: return f_site_g def _select_basin_model(self, vs30): """ Select the preferred basin model (California or Japan) to scale basin depth with respect to Vs30 """ return CB14._select_basin_model(self, vs30) def _get_basin_response_term(self, C, z2pt5): """ Returns the basin response term, f_sed, defined in equation 20 The deep basin response (z2.5 > 1km) is not included in this model """ f_sed = np.zeros(len(z2pt5)) idx = z2pt5 < 1.0 f_sed[idx] = (C["c14"] + C["c15"] * float(self.CONSTS["SJ"])) *\ (z2pt5[idx] - 1.0) return f_sed def _get_hypocentral_depth_term(self, C, rup): """ Returns the hypocentral depth scaling term, f_hyp, defined in equations 21 to 23 """ return CB14._get_hypocentral_depth_term(self, C, rup) def _get_fault_dip_term(self, C, rup): """ Returns the fault dip term, f_dip, defined in equation 24 """ return CB14._get_fault_dip_term(self, C, rup) def _get_anelastic_attenuation_term(self, C, rrup): """ Returns the anelastic attenuation term, f_atn, defined in equation 25 """ Dc20 = self._get_delta_c20(C) f_atn = np.zeros(len(rrup)) idx = rrup > 80.0 f_atn[idx] = (C["c20"] + Dc20) * (rrup[idx] - 80.0) return f_atn def _get_delta_c20(self, C): """ Retrieve regional-dependent coefficient accounting for differences in anelastic attenuation in path scaling This is to derive a reference/base-case c20 that includes California, Taiwan, the Middle East, and other similar active tectonic regions to represent a typical or average Q region. """ return 0. def _get_stddevs(self, C, rup, sites, stddev_types): """ Returns the inter-event, intra-event, and total standard deviations Note that it is assumed here that the soil response of the vertical component is linear (i.e. nonlinear site response effects not included). Thus, the expressions for the aleatory std devs for the vertical component is much simpler than in the horizontal component, since the site response- and IMT-correlation functions are neglected. """ num_sites = len(sites.vs30) # Evaluate tau according to equation 27 tau = self._get_taulny(C, rup.mag) # Evaluate phi according to equation 28 phi = self._get_philny(C, rup.mag) stddevs = [] for stddev_type in stddev_types: assert stddev_type in self.DEFINED_FOR_STANDARD_DEVIATION_TYPES if stddev_type == const.StdDev.TOTAL: stddevs.append(np.sqrt((tau ** 2.) + (phi ** 2.)) + np.zeros(num_sites)) elif stddev_type == const.StdDev.INTRA_EVENT: stddevs.append(phi + np.zeros(num_sites)) elif stddev_type == const.StdDev.INTER_EVENT: stddevs.append(tau + np.zeros(num_sites)) # return std dev values for each stddev type in site collection return stddevs def _get_taulny(self, C, mag): """ Returns the inter-event random effects coefficient (tau) defined in Equation 29. """ return CB14._get_taulny(self, C, mag) def _get_philny(self, C, mag): """ Returns the intra-event random effects coefficient (phi) defined in Equation 30. """ return CB14._get_philny(self, C, mag) #: Table of regression coefficients obtained from supplementary material #: published together with the EQS paper COEFFS = CoeffsTable(sa_damping=5, table="""\ IMT c0 c1 c2 c3 c4 c5 c6 c7 c8 c9 c10 c11 c12 c13 c14 c15 c17 c18 c19 c20 Dc20_JP Dc20_CH a2 h1 h2 h3 h5 h6 k1 phi1 phi2 tau1 tau2 pgv -3.86 1.51 0.27 -1.299 -0.379 -2.383 0.196 6.274 0.111 -0.128 0.14 -0.395 0.338 0.407 -0.0016 0.382 0.0581 0.0294 0.00761 -0.0019 0.0005 0.0019 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.608 0.442 0.334 0.24 pga -4.729 0.984 0.537 -1.499 -0.443 -2.666 0.214 7.166 0 -0.23 0.759 -0.356 1.019 0.373 -0.1172 -0.097 0.102 0.0442 0.00784 -0.0053 -0.0018 0.0039 0.167 0.241 1.474 -0.715 -0.337 -0.27 865 0.694 0.493 0.461 0.347 0.01 -4.674 0.977 0.533 -1.485 -0.445 -2.665 0.214 7.136 0 -0.229 0.759 -0.354 1.015 0.372 -0.1193 -0.094 0.1026 0.0452 0.00784 -0.0053 -0.0018 0.0039 0.168 0.242 1.471 -0.714 -0.336 -0.27 865 0.695 0.494 0.462 0.345 0.02 -4.548 0.976 0.549 -1.488 -0.453 -2.699 0.215 6.936 0 -0.27 0.768 -0.344 0.95 0.4 -0.1454 -0.081 0.1059 0.0427 0.00786 -0.0052 -0.0018 0.0036 0.166 0.244 1.467 -0.711 -0.339 -0.263 865 0.7 0.508 0.474 0.375 0.03 -4.05 0.931 0.628 -1.494 -0.464 -2.772 0.216 7.235 0 -0.315 0.766 -0.297 1.056 0.394 -0.1957 -0.091 0.1175 0.041 0.00815 -0.0052 -0.002 0.0033 0.167 0.246 1.467 -0.713 -0.338 -0.259 908 0.722 0.536 0.529 0.416 0.05 -3.435 0.887 0.674 -1.388 -0.552 -2.76 0.202 8.334 0 -0.329 0.764 -0.363 1.316 0.422 -0.187 -0.29 0.1238 0.0408 0.00783 -0.0062 -0.0026 0.0039 0.173 0.251 1.449 -0.701 -0.338 -0.263 1054 0.751 0.584 0.576 0.468 0.075 -3.435 0.902 0.726 -1.469 -0.543 -2.575 0.177 8.761 0 -0.29 0.795 -0.427 1.758 0.336 -0.095 -0.261 0.1088 0.0516 0.00726 -0.0072 -0.0021 0.0048 0.198 0.26 1.435 -0.695 -0.347 -0.219 1086 0.74 0.578 0.523 0.427 0.1 -3.93 0.993 0.698 -1.572 -0.47 -2.461 0.166 9.049 0 -0.203 0.842 -0.429 1.411 0.314 -0.0999 -0.091 0.0918 0.0559 0.00644 -0.0072 -0.0018 0.005 0.174 0.259 1.449 -0.708 -0.391 -0.201 1032 0.723 0.57 0.461 0.39 0.15 -5.505 1.267 0.51 -1.669 -0.452 -2.349 0.164 8.633 0 -0.203 0.736 -0.421 1.227 0.289 0.0017 -0.092 0.072 0.0447 0.00745 -0.0066 -0.0018 0.0048 0.198 0.254 1.461 -0.715 -0.449 -0.099 878 0.731 0.536 0.391 0.343 0.2 -6.28 1.366 0.447 -1.75 -0.435 -2.335 0.175 8.742 0 -0.203 0.801 -0.429 0.987 0.29 0.0402 -0.081 0.0602 0.0485 0.00789 -0.0056 -0.0022 0.0041 0.204 0.237 1.484 -0.721 -0.393 -0.198 748 0.701 0.51 0.363 0.308 0.25 -6.789 1.458 0.274 -1.711 -0.41 -2.332 0.183 8.4 0 -0.203 0.715 -0.438 0.577 0.303 0.0468 0.011 0.05 0.0416 0.00629 -0.0049 -0.0025 0.0034 0.185 0.206 1.581 -0.787 -0.339 -0.21 654 0.687 0.507 0.355 0.288 0.3 -7.4 1.528 0.193 -1.77 -0.305 -2.297 0.19 7.643 0 -0.203 0.708 -0.421 0.279 0.336 0.0255 0.092 0.0382 0.0438 0.00524 -0.0046 -0.0027 0.0031 0.164 0.21 1.586 -0.795 -0.447 -0.121 587 0.668 0.514 0.355 0.265 0.4 -8.75 1.739 -0.02 -1.594 -0.446 -2.219 0.185 7.059 0 -0.203 0.683 -0.401 0.358 0.358 0.0606 0.122 0.0264 0.0307 0.00522 -0.0037 -0.0024 0.0024 0.16 0.226 1.544 -0.77 -0.525 -0.086 503 0.628 0.521 0.36 0.28 0.5 -9.74 1.872 -0.121 -1.577 -0.489 -2.205 0.191 6.375 0 -0.203 0.704 -0.417 0.229 0.432 0.0904 0.287 0.0163 0.0287 0.00539 -0.0031 -0.0025 0.0021 0.184 0.217 1.554 -0.77 -0.407 -0.281 457 0.606 0.526 0.376 0.284 0.75 -11.05 2.021 -0.042 -1.757 -0.53 -2.143 0.188 5.166 0.016 -0.203 0.602 -0.49 0.574 0.459 0.1776 0.292 -0.0016 0.0277 0.00501 -0.0021 -0.0025 0.002 0.216 0.154 1.626 -0.78 -0.371 -0.285 410 0.568 0.536 0.416 0.322 1 -12.184 2.18 -0.069 -1.707 -0.624 -2.092 0.176 5.642 0.032 -0.115 0.394 -0.539 0.98 0.442 0.2389 0.316 -0.0072 0.0277 0.00506 -0.0012 -0.0023 0.0012 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.536 0.55 0.472 0.311 1.5 -13.451 2.27 0.047 -1.621 -0.686 -1.913 0.144 5.963 0.128 -0.005 0.328 -0.611 0.819 0.52 0.2758 0.45 -0.0262 0.0293 0.00353 -0.0004 -0.0013 0.0004 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.511 0.559 0.507 0.329 2 -13.7 2.271 0.149 -1.512 -0.84 -1.882 0.126 7.584 0.255 0.12 0.112 -0.63 0.044 0.566 0.3051 0.424 -0.0408 0.0221 0.0022 0 -0.0004 0 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.507 0.571 0.539 0.345 3 -13.9 2.15 0.368 -1.315 -0.89 -1.789 0.105 8.645 0.284 0.17 0.011 -0.562 -0.396 0.562 0.3482 0.3 -0.0512 0.0321 -0.00137 0 0 0 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.474 0.557 0.515 0.335 4 -14.59387 2.132 0.726 -1.506 -0.885 -1.78139 0.10009 10.20357 0.26112 0.17 0 -0.53663 0.00115 0.51499 0.35267 0.25726 -0.0567 0.02249 0.00053 0 0 0 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.466 0.566 0.553 0.331 5 -15.63449 2.116 1.027 -1.721 -0.878 -1.68982 0.098 8.38571 0.28229 0.17747 0 -0.44173 -0.59234 0.51133 0.30443 0.17039 -0.04288 0.02372 0.00233 0 0 0 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.43 0.568 0.578 0.294 7.5 -17.12864 2.223 0.169 -0.756 -1.077 -1.72135 0.125 5.77927 0.38692 0.38278 0 -0.3428 -1.13827 0.57479 0.16789 0.21872 -0.0308 0.0171 -0.00298 0 0 0 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.386 0.527 0.6 0.379 10 -17.65672 2.132 0.367 -0.8 -1.282 -1.948 0.163 4.13478 0.32216 0.33417 0 -0.19908 -0.32493 0.32431 0.16858 0.12681 0.00668 -0.00165 0.00092 0 0 0 0.596 0.117 1.616 -0.733 -0.128 -0.756 400 0.395 0.481 0.495 0.442 """) #: Equation constants (that are IMT-independent) for global model CONSTS = { # hanging-wall model coefficient "h4": 1.0, # flag variable for Japan site data "SJ": 0 }
[docs]class BozorgniaCampbell2016HighQ(BozorgniaCampbell2016): """ Implements the BC15 GMPE by Bozorgnia & Campbell (2016) for vertical-component ground motions from the PEER NGA-West2 Project Applies regional corrections in path scaling term for regions with low attenuation (high quality factor, Q) (e.g. eastern China) """ def _get_delta_c20(self, C): """ Retrieve regional-dependent coefficient accounting for differences in anelastic attenuation """ return C['Dc20_CH']
[docs]class BozorgniaCampbell2016LowQ(BozorgniaCampbell2016): """ Implements the BC15 GMPE by Bozorgnia & Campbell (2016) for vertical-component ground motions from the PEER NGA-West2 Project Applies regional corrections in path scaling term for regions with high attenuation (low quality factor, Q) (e.g. Japan and Italy) """ def _get_delta_c20(self, C): """ Retrieve regional-dependent coefficient accounting for differences in anelastic attenuation """ return C['Dc20_JP']
[docs]class BozorgniaCampbell2016AveQJapanSite(BozorgniaCampbell2016): """ Implements the BC15 GMPE by Bozorgnia & Campbell (2016) for vertical-component ground motions from the PEER NGA-West2 Project Incorporates the difference in linear Vs30 scaling for sites in Japan by activating the flag variable in shallow site reponse scaling Applies the average attenuation case (Dc20=0) """ #: Equation constants (that are IMT-independent) for Japan sites CONSTS = { # hanging-wall model coefficient "h4": 1.0, # flag variable for Japan site data "SJ": 1 }
[docs]class BozorgniaCampbell2016HighQJapanSite(BozorgniaCampbell2016AveQJapanSite): """ Implements the BC15 GMPE by Bozorgnia & Campbell (2016) for vertical-component ground motions from the PEER NGA-West2 Project Incorporates the difference in linear Vs30 scaling for sites in Japan by activating the flag variable in shallow site reponse scaling Applies regional corrections in path scaling term for regions with low attenuation (high quality factor, Q) """ def _get_delta_c20(self, C): """ Retrieve regional-dependent coefficient accounting for differences in anelastic attenuation """ return C['Dc20_CH']
[docs]class BozorgniaCampbell2016LowQJapanSite(BozorgniaCampbell2016AveQJapanSite): """ Implements the BC15 GMPE by Bozorgnia & Campbell (2016) for vertical-component ground motions from the PEER NGA-West2 Project Incorporates the difference in linear Vs30 scaling for sites in Japan by activating the flag variable in shallow site reponse scaling Applies regional corrections in path scaling term for regions with high attenuation (low quality factor, Q) """ def _get_delta_c20(self, C): """ Retrieve regional-dependent coefficient accounting for differences in anelastic attenuation """ return C['Dc20_JP']