|
# http://pyrocko.org - GPLv3 # # The Pyrocko Developers, 21st Century # ---|P------/S----------~Lg----------
StringPattern, Unicode, Float, Bool, Int, TBase, List, ValidationError, Timestamp, Tuple, Dict)
"``'%s'``" % choice for choice in cls.choices)
4, String.T(), default=('', 'STA', '', 'Z'), help='network, station, location and channel codes')
shape=(None,), dtype=num.float32, serialize_as='base64', serialize_dtype=num.dtype('<f4'), help='numpy array with data samples')
default=1.0, help='sampling interval [s]')
default=0.0, help='time of first sample as a system timestamp [s]')
ydata=self.data, deltat=self.deltat, tmin=self.tmin)
def from_pyrocko_trace(cls, tr, **kwargs): d = dict( codes=tr.nslc_id, tmin=tr.tmin, deltat=tr.deltat, data=num.asarray(tr.get_ydata(), dtype=num.float32)) d.update(kwargs) return cls(**d)
String.T(), Array.T(shape=(None,), dtype=num.float, serialize_as='base64'))
optional=True)
optional=True, shape=(None,), dtype=num.float, serialize_as='base64')
optional=True, shape=(None,), dtype=num.float, serialize_as='base64')
try: from kite import Scene except ImportError: raise ImportError('Kite not installed')
def reshape(arr): return arr.reshape(self.shape)
displacement = self.result[component]
displacement, theta, phi = map( reshape, (displacement, self.theta, self.phi))
sc = Scene( displacement=displacement, theta=theta, phi=phi, config=self.config)
return sc
ComponentSchemeDescription( name='elastic2', source_terms=['m0'], ncomponents=2, default_stored_quantity='displacement', provided_components=[ 'n', 'e', 'd']), ComponentSchemeDescription( name='elastic8', source_terms=['mnn', 'mee', 'mdd', 'mne', 'mnd', 'med'], ncomponents=8, default_stored_quantity='displacement', provided_components=[ 'n', 'e', 'd']), ComponentSchemeDescription( name='elastic10', source_terms=['mnn', 'mee', 'mdd', 'mne', 'mnd', 'med'], ncomponents=10, default_stored_quantity='displacement', provided_components=[ 'n', 'e', 'd']), ComponentSchemeDescription( name='elastic18', source_terms=['mnn', 'mee', 'mdd', 'mne', 'mnd', 'med'], ncomponents=18, default_stored_quantity='displacement', provided_components=[ 'n', 'e', 'd']), ComponentSchemeDescription( name='elastic5', source_terms=['fn', 'fe', 'fd'], ncomponents=5, default_stored_quantity='displacement', provided_components=[ 'n', 'e', 'd']), ComponentSchemeDescription( name='poroelastic10', source_terms=['pore_pressure'], ncomponents=10, default_stored_quantity=None, provided_components=[ 'displacement.n', 'displacement.e', 'displacement.d', 'vertical_tilt.n', 'vertical_tilt.e', 'pore_pressure', 'darcy_velocity.n', 'darcy_velocity.e', 'darcy_velocity.d'])]
# new names? # 'mt_to_displacement_1d' # 'mt_to_displacement_1d_ff_only' # 'mt_to_gravity_1d' # 'mt_to_stress_1d' # 'explosion_to_displacement_1d' # 'sf_to_displacement_1d' # 'mt_to_displacement_3d' # 'mt_to_gravity_3d' # 'mt_to_stress_3d' # 'pore_pressure_to_displacement_1d' # 'pore_pressure_to_vertical_tilt_1d' # 'pore_pressure_to_pore_pressure_1d' # 'pore_pressure_to_darcy_velocity_1d'
(c.name, c) for c in component_scheme_descriptions)
''' Different Green's Function component schemes are available:
================= ========================================================= Name Description ================= ========================================================= ``elastic10`` Elastodynamic for :py:class:`~pyrocko.gf.meta.ConfigTypeA` and :py:class:`~pyrocko.gf.meta.ConfigTypeB` stores, MT sources only ``elastic8`` Elastodynamic for far-field only :py:class:`~pyrocko.gf.meta.ConfigTypeA` and :py:class:`~pyrocko.gf.meta.ConfigTypeB` stores, MT sources only ``elastic2`` Elastodynamic for :py:class:`~pyrocko.gf.meta.ConfigTypeA` and :py:class:`~pyrocko.gf.meta.ConfigTypeB` stores, purely isotropic sources only ``elastic5`` Elastodynamic for :py:class:`~pyrocko.gf.meta.ConfigTypeA` and :py:class:`~pyrocko.gf.meta.ConfigTypeB` stores, SF sources only ``elastic18`` Elastodynamic for :py:class:`~pyrocko.gf.meta.ConfigTypeC` stores, MT sources only ``poroelastic10`` Poroelastic for :py:class:`~pyrocko.gf.meta.ConfigTypeA` and :py:class:`~pyrocko.gf.meta.ConfigTypeB` stores ================= ========================================================= '''
cake.read_nd_model_str(val))
return literal(cake.write_nd_model_str(val))
'global', 'regional', 'local', ]
'full waveform', 'bodywave', 'P wave', 'S wave', 'surface wave', ]
'complete', 'incomplete', 'missing', ]
'displacement', 'velocity', 'acceleration', 'pressure', 'tilt', 'pore_pressure', 'darcy_velocity', 'vertical_tilt']
from pybtex.database.input import bibtex
parser = bibtex.Parser()
if filename is not None: bib_data = parser.parse_file(filename) elif stream is not None: bib_data = parser.parse_stream(stream)
references = []
for id_, entry in bib_data.entries.items(): d = {} avail = entry.fields.keys() for prop in cls.T.properties: if prop.name == 'authors' or prop.name not in avail: continue
d[prop.name] = entry.fields[prop.name]
if 'author' in entry.persons: d['authors'] = [] for person in entry.persons['author']: d['authors'].append(new_str(person))
c = Reference(id=id_, type=entry.type, **d) references.append(c)
return references
r'cake:' + _cake_pat + \ r'|iaspei:' + _iaspei_pat + \ r'|vel_surface:' + _fpat + \ r'|vel:' + _fpat + \ r'|stored:' + _spat + \ r')'
r'^((first|last)?\((' + _spat + r'(\|' + _spat + r')*)\)|(' + _spat + r'))?(' + _fpat + ')?$')
r'^((first|last)?\{(' + _ppat + r'(\|' + _ppat + r')*)\}|(' + _ppat + r'))?(' + _fpat + 'S?)?$')
''' Definition of a time instant relative to one or more named phase arrivals
Instances of this class can be used e.g. in cutting and tapering operations. They can hold an absolute time or an offset to a named phase arrival or group of such arrivals.
Timings can be instantiated from a simple string defintion i.e. with ``Timing(str)`` where ``str`` is something like ``'SELECT{PHASE_DEFS}[+-]OFFSET[S]'`` where ``'SELECT'`` is ``'first'``, ``'last'`` or empty, ``'PHASE_DEFS'`` is a ``'|'``-separated list of phase definitions, and ``'OFFSET'`` is the time offset in seconds. If the an ``'S'`` is appended to ``'OFFSET'``, it is interpreted as a surface slowness in [s/km].
Phase definitions can be specified in either of the following ways:
* ``'stored:PHASE_ID'`` - retrieves value from stored travel time table * ``'cake:CAKE_PHASE_DEF'`` - evaluates first arrival of phase with cake (see :py:class:`pyrocko.cake.PhaseDef`) * ``'vel_surface:VELOCITY'`` - arrival according to surface distance / velocity [km/s] * ``'vel:VELOCITY'`` - arrival according to 3D-distance / velocity [km/s]
**Examples:**
* ``'100'`` : absolute time; 100 s * ``'{stored:P}-100'`` : 100 s before arrival of P phase according to stored travel time table named ``'P'`` * ``'{stored:A|stored:B}'`` : time instant of phase arrival A, or B if A is undefined for a given geometry * ``'first{stored:A|stored:B}'`` : as above, but the earlier arrival of A and B is chosen, if both phases are defined for a given geometry * ``'last{stored:A|stored:B}'`` : as above but the later arrival is chosen * ``'first{stored:A|stored:B|stored:C}-100'`` : 100 s before first out of arrivals A, B, and C '''
offset_is_slowness = s.endswith('S') phase_defs = [] select = ''
else: phase_defs = []
else: m = timing_regex_old.match(s) if m: if m.group(3): phase_defs = m.group(3).split('|') elif m.group(5): phase_defs = [m.group(5)] else: phase_defs = []
select = m.group(2) or ''
offset = 0.0 if m.group(6): offset = float(m.group(6))
phase_defs = [ 'stored:' + phase_def for phase_def in phase_defs]
matched = True
raise InvalidTimingSpecification(s)
phase_defs=phase_defs, select=select, offset=offset, offset_is_slowness=offset_is_slowness)
def __str__(self): s = [] if self.phase_defs: sphases = '|'.join(self.phase_defs) # if len(self.phase_defs) > 1 or self.select: sphases = '{%s}' % sphases
if self.select: sphases = self.select + sphases
s.append(sphases)
if self.offset != 0.0 or not self.phase_defs: s.append('%+g' % self.offset) if self.offset_is_slowness: s.append('S')
return ''.join(s)
phase_offset = get_phase( 'vel_surface:%g' % (1.0/self.offset)) offset = phase_offset(args) else:
get_phase(phase_def) for phase_def in self.phase_defs] return None return min(times) return max(times) else: else: return offset
except spit.OutOfBounds: raise OutOfBounds(args)
default='', help=('Can be either ``\'%s\'``, ``\'%s\'``, or ``\'%s\'``. ' % tuple(PhaseSelect.choices)))
defs = [] for x in s.split(','): try: defs.append(float(x)) except ValueError: if x.startswith('!'): defs.extend(cake.PhaseDef.classic(x[1:])) else: defs.append(cake.PhaseDef(x))
return defs
''' Maps an arrival phase identifier to an arrival phase definition. '''
help='name used to identify the phase') help='definition of the phase in either cake syntax as defined in ' ':py:class:`pyrocko.cake.PhaseDef`, or, if prepended with an ' '``!``, as a *classic phase name*, or, if it is a simple ' 'number, as a constant horizontal velocity.')
def phases(self): return [x for x in mkdefs(self.definition) if isinstance(x, cake.PhaseDef)]
def horizontal_velocities(self): return [x for x in mkdefs(self.definition) if isinstance(x, float)]
Exception.__init__(self) self.values = values self.reason = reason self.context = None
def __str__(self): scontext = '' if self.context: scontext = '\n%s' % str(self.context)
if self.reason: scontext += '\n%s' % self.reason
if self.values: return 'out of bounds: (%s)%s' % ( ','.join('%g' % x for x in self.values), scontext) else: return 'out of bounds%s' % scontext
optional=True, shape=(None,), dtype=num.float, help='Latitudes of targets.') optional=True, shape=(None,), dtype=num.float, help='Longitude of targets.') optional=True, shape=(None,), dtype=num.float, help='North shifts of targets.') optional=True, shape=(None,), dtype=num.float, help='East shifts of targets.') optional=True, shape=(None,), dtype=num.float, help='Elevations of targets.')
def coords5(self): self.elevation] raise AttributeError('Empty StaticTarget') raise AttributeError('Inconsistent coordinate sizes.')
def ncoords(self): return 0
''' Get all coordinates as lat lon :returns: Coordinates in Latitude, Longitude :rtype: :class:`numpy.ndarray`, (N, 2) '''
'''Returns the corner coordinates of the multi location object
:returns: In LatLon: lower left, upper left, upper right, lower right :rtype: tuple ''' latlon = self.get_latlon() ll = (latlon[:, 0].min(), latlon[:, 1].min()) ur = (latlon[:, 0].max(), latlon[:, 1].max()) return (ll, (ll[0], ur[1]), ur, (ur[0], ll[1]))
3, String.T(), optional=True, help='network, station, and location codes')
from pyrocko import model
lat, lon = self.effective_latlon
return model.Station( network=self.codes[0], station=self.codes[1], location=self.codes[2], lat=lat, lon=lon, depth=self.depth)
return d else:
'''Base class for discretized sources.
To compute synthetic seismograms, the parameterized source models (see of :py:class:`~pyrocko.gf.seismosizer.Source` derived classes) are first discretized into a number of point sources. These spacio-temporal point source distributions are represented by subclasses of the :py:class:`DiscretizedSource`. For elastodynamic problems there is the :py:class:`DiscretizedMTSource` for moment tensor point source distributions and the :py:class:`DiscretizedExplosionSource` for pure explosion/implosion type source distributions. The geometry calculations are implemented in the base class. How Green's function components have to be weighted and sumed is defined in the derived classes.
Like in the :py:class:`Location` class, the positions of the point sources contained in the discretized source are defined by a common reference point (:py:attr:`lat`, :py:attr:`lon`) and cartesian offsets to this (:py:attr:`north_shifts`, :py:attr:`east_shifts`, :py:attr:`depths`). Alternatively latitude and longitude of each contained point source can be specified directly (:py:attr:`lats`, :py:attr:`lons`). '''
def check_scheme(cls, scheme): ''' Check if given GF component scheme is supported by the class.
Raises :py:class:`UnavailableScheme` if the given scheme is not supported by this discretized source class. '''
raise UnavailableScheme( 'source type "%s" does not support GF component scheme "%s"' % (cls.__name__, scheme))
'lats', 'lons'):
raise NotImplementedError()
raise NotImplementedError()
def effective_latlons(self): ''' Property holding the offest-corrected lats and lons of all points. '''
if self._latlons is None: if self.lats is not None and self.lons is not None: if (self.north_shifts is not None and self.east_shifts is not None): self._latlons = orthodrome.ne_to_latlon( self.lats, self.lons, self.north_shifts, self.east_shifts) else: self._latlons = self.lats, self.lons else: lat = g(self.lat, 0.0) lon = g(self.lon, 0.0) self._latlons = orthodrome.ne_to_latlon( lat, lon, self.north_shifts, self.east_shifts)
return self._latlons
def effective_north_shifts(self): if self.north_shifts is not None: return self.north_shifts else: return num.zeros(self.times.size)
def effective_east_shifts(self): if self.east_shifts is not None: return self.east_shifts else: return num.zeros(self.times.size)
''' Check if receiver has same reference point. '''
return (g(self.lat, 0.0) == receiver.lat and g(self.lon, 0.0) == receiver.lon and self.lats is None and self.lons is None)
''' Compute azimuths and backaziumuths to/from receiver, for all contained points. '''
if self.same_origin(receiver): azis = r2d * num.arctan2(receiver.east_shift - self.east_shifts, receiver.north_shift - self.north_shifts) bazis = azis + 180. else: slats, slons = self.effective_latlons rlat, rlon = receiver.effective_latlon azis = orthodrome.azimuth_numpy(slats, slons, rlat, rlon) bazis = orthodrome.azimuth_numpy(rlat, rlon, slats, slons)
return azis, bazis
''' Compute distances to receiver for all contained points. ''' if self.same_origin(receiver): return num.sqrt((self.north_shifts - receiver.north_shift)**2 + (self.east_shifts - receiver.east_shift)**2)
else: slats, slons = self.effective_latlons rlat, rlon = receiver.effective_latlon return orthodrome.distance_accurate50m_numpy(slats, slons, rlat, rlon)
if self.lats is not None and self.lons is not None: lat = float(self.lats[i]) lon = float(self.lons[i]) else: lat = self.lat lon = self.lon
if self.north_shifts is not None and self.east_shifts is not None: north_shift = float(self.north_shifts[i]) east_shift = float(self.east_shifts[i])
else: north_shift = east_shift = 0.0
return lat, lon, north_shift, east_shift
xs[:, 0] = self.lats xs[:, 1] = self.lons else:
def nelements(self):
def combine(cls, sources, **kwargs): ''' Combine several discretized source models.
Concatenenates all point sources in the given discretized ``sources``. Care must be taken when using this function that the external amplitude factors and reference times of the parameterized (undiscretized) sources match or are accounted for. '''
first = sources[0]
if not all(type(s) == type(first) for s in sources): raise Exception('DiscretizedSource.combine must be called with ' 'sources of same type.')
latlons = [] for s in sources: latlons.append(s.effective_latlons)
lats, lons = num.hstack(latlons)
if all((s.lats is None and s.lons is None) for s in sources): rlats = num.array([s.lat for s in sources], dtype=num.float) rlons = num.array([s.lon for s in sources], dtype=num.float) same_ref = num.all( rlats == rlats[0]) and num.all(rlons == rlons[0]) else: same_ref = False
cat = num.concatenate times = cat([s.times for s in sources]) depths = cat([s.depths for s in sources])
if same_ref: lat = first.lat lon = first.lon north_shifts = cat([s.effective_north_shifts for s in sources]) east_shifts = cat([s.effective_east_shifts for s in sources]) lats = None lons = None else: lat = None lon = None north_shifts = None east_shifts = None
return cls( times=times, lat=lat, lon=lon, lats=lats, lons=lons, north_shifts=north_shifts, east_shifts=east_shifts, depths=depths, **kwargs)
moments = self.moments() norm = num.sum(moments) if norm != 0.0: w = moments / num.sum(moments) else: w = num.ones(moments.size)
if self.lats is not None and self.lons is not None: lats, lons = self.effective_latlons rlat, rlon = num.mean(lats), num.mean(lons) n, e = orthodrome.latlon_to_ne_numpy(rlat, rlon, lats, lons) else: rlat, rlon = g(self.lat, 0.0), g(self.lon, 0.0) n, e = self.north_shifts, self.east_shifts
cn = num.sum(n*w) ce = num.sum(e*w) clat, clon = orthodrome.ne_to_latlon(rlat, rlon, cn, ce)
if self.lats is not None and self.lons is not None: lat = clat lon = clon north_shift = 0. east_shift = 0. else: lat = g(self.lat, 0.0) lon = g(self.lon, 0.0) north_shift = cn east_shift = ce
depth = num.sum(self.depths*w) time = num.sum(self.times*w) return tuple(float(x) for x in (time, lat, lon, north_shift, east_shift, depth))
'elastic2', 'elastic8', 'elastic10', )
self.check_scheme(scheme)
if scheme == 'elastic2': return self.m0s[:, num.newaxis].copy()
elif scheme in ('elastic8', 'elastic10'): m6s = num.zeros((self.m0s.size, 6)) m6s[:, 0:3] = self.m0s[:, num.newaxis] return m6s else: assert False
self.check_scheme(scheme)
azis, bazis = self.azibazis_to(receiver)
sb = num.sin(bazis*d2r-num.pi) cb = num.cos(bazis*d2r-num.pi)
m0s = self.m0s n = azis.size
cat = num.concatenate rep = num.repeat
if scheme == 'elastic2': w_n = cb*m0s g_n = filledi(0, n) w_e = sb*m0s g_e = filledi(0, n) w_d = m0s g_d = filledi(1, n)
elif scheme == 'elastic8': w_n = cat((cb*m0s, cb*m0s)) g_n = rep((0, 2), n) w_e = cat((sb*m0s, sb*m0s)) g_e = rep((0, 2), n) w_d = cat((m0s, m0s)) g_d = rep((5, 7), n)
elif scheme == 'elastic10': w_n = cat((cb*m0s, cb*m0s, cb*m0s)) g_n = rep((0, 2, 8), n) w_e = cat((sb*m0s, sb*m0s, sb*m0s)) g_e = rep((0, 2, 8), n) w_d = cat((m0s, m0s, m0s)) g_d = rep((5, 7, 9), n)
else: assert False
return ( ('displacement.n', w_n, g_n), ('displacement.e', w_e, g_e), ('displacement.d', w_d, g_d), )
from pyrocko.gf.seismosizer import ExplosionSource sources = [] for i in range(self.nelements): lat, lon, north_shift, east_shift = self.element_coords(i) sources.append(ExplosionSource( time=float(self.times[i]), lat=lat, lon=lon, north_shift=north_shift, east_shift=east_shift, depth=float(self.depths[i]), moment=float(self.m0s[i])))
return sources
return self.m0s
from pyrocko.gf.seismosizer import ExplosionSource time, lat, lon, north_shift, east_shift, depth = \ self.centroid_position()
return ExplosionSource( time=time, lat=lat, lon=lon, north_shift=north_shift, east_shift=east_shift, depth=depth, moment=float(num.sum(self.m0s)))
def combine(cls, sources, **kwargs): ''' Combine several discretized source models.
Concatenenates all point sources in the given discretized ``sources``. Care must be taken when using this function that the external amplitude factors and reference times of the parameterized (undiscretized) sources match or are accounted for. '''
if 'm0s' not in kwargs: kwargs['m0s'] = num.concatenate([s.m0s for s in sources])
return super(DiscretizedExplosionSource, cls).combine(sources, **kwargs)
'elastic5', )
self.check_scheme(scheme)
return self.forces
self.check_scheme(scheme)
azis, bazis = self.azibazis_to(receiver)
sa = num.sin(azis*d2r) ca = num.cos(azis*d2r) sb = num.sin(bazis*d2r-num.pi) cb = num.cos(bazis*d2r-num.pi)
forces = self.forces fn = forces[:, 0] fe = forces[:, 1] fd = forces[:, 2]
f0 = fd f1 = ca * fn + sa * fe f2 = ca * fe - sa * fn
n = azis.size
if scheme == 'elastic5': ioff = 0
cat = num.concatenate rep = num.repeat
w_n = cat((cb*f0, cb*f1, -sb*f2)) g_n = ioff + rep((0, 1, 2), n) w_e = cat((sb*f0, sb*f1, cb*f2)) g_e = ioff + rep((0, 1, 2), n) w_d = cat((f0, f1)) g_d = ioff + rep((3, 4), n)
return ( ('displacement.n', w_n, g_n), ('displacement.e', w_e, g_e), ('displacement.d', w_d, g_d), )
def combine(cls, sources, **kwargs): ''' Combine several discretized source models.
Concatenenates all point sources in the given discretized ``sources``. Care must be taken when using this function that the external amplitude factors and reference times of the parameterized (undiscretized) sources match or are accounted for. '''
if 'forces' not in kwargs: kwargs['forces'] = num.vstack([s.forces for s in sources])
return super(DiscretizedSFSource, cls).combine(sources, **kwargs)
return num.sum(self.forces**2, axis=1)
from pyrocko.gf.seismosizer import SFSource time, lat, lon, north_shift, east_shift, depth = \ self.centroid_position()
fn, fe, fd = map(float, num.sum(self.forces, axis=0)) return SFSource( time=time, lat=lat, lon=lon, north_shift=north_shift, east_shift=east_shift, depth=depth, fn=fn, fe=fe, fd=fd)
shape=(None, 6), dtype=num.float, help='rows with (m_nn, m_ee, m_dd, m_ne, m_nd, m_ed)')
'elastic8', 'elastic10', 'elastic18', )
self.check_scheme(scheme)
m6s = self.m6s n = m6s.shape[0] rep = num.repeat
if scheme == 'elastic18': w_n = m6s.flatten() g_n = num.tile(num.arange(0, 6), n) w_e = m6s.flatten() g_e = num.tile(num.arange(6, 12), n) w_d = m6s.flatten() g_d = num.tile(num.arange(12, 18), n)
else: azis, bazis = self.azibazis_to(receiver)
sa = num.sin(azis*d2r) ca = num.cos(azis*d2r) s2a = num.sin(2.*azis*d2r) c2a = num.cos(2.*azis*d2r) sb = num.sin(bazis*d2r-num.pi) cb = num.cos(bazis*d2r-num.pi)
f0 = m6s[:, 0]*ca**2 + m6s[:, 1]*sa**2 + m6s[:, 3]*s2a f1 = m6s[:, 4]*ca + m6s[:, 5]*sa f2 = m6s[:, 2] f3 = 0.5*(m6s[:, 1]-m6s[:, 0])*s2a + m6s[:, 3]*c2a f4 = m6s[:, 5]*ca - m6s[:, 4]*sa f5 = m6s[:, 0]*sa**2 + m6s[:, 1]*ca**2 - m6s[:, 3]*s2a
cat = num.concatenate
if scheme == 'elastic8': w_n = cat((cb*f0, cb*f1, cb*f2, -sb*f3, -sb*f4)) g_n = rep((0, 1, 2, 3, 4), n) w_e = cat((sb*f0, sb*f1, sb*f2, cb*f3, cb*f4)) g_e = rep((0, 1, 2, 3, 4), n) w_d = cat((f0, f1, f2)) g_d = rep((5, 6, 7), n)
elif scheme == 'elastic10': w_n = cat((cb*f0, cb*f1, cb*f2, cb*f5, -sb*f3, -sb*f4)) g_n = rep((0, 1, 2, 8, 3, 4), n) w_e = cat((sb*f0, sb*f1, sb*f2, sb*f5, cb*f3, cb*f4)) g_e = rep((0, 1, 2, 8, 3, 4), n) w_d = cat((f0, f1, f2, f5)) g_d = rep((5, 6, 7, 9), n)
else: assert False
return ( ('displacement.n', w_n, g_n), ('displacement.e', w_e, g_e), ('displacement.d', w_d, g_d), )
from pyrocko.gf.seismosizer import MTSource sources = [] for i in range(self.nelements): lat, lon, north_shift, east_shift = self.element_coords(i) sources.append(MTSource( time=float(self.times[i]), lat=lat, lon=lon, north_shift=north_shift, east_shift=east_shift, depth=float(self.depths[i]), m6=self.m6s[i]))
return sources
n = self.nelements moments = num.zeros(n) for i in range(n): m = moment_tensor.symmat6(*self.m6s[i]) m_evals = num.linalg.eigh(m)[0]
# incorrect for non-dc sources: !!!! m0 = num.linalg.norm(m_evals)/math.sqrt(2.) moments[i] = m0
return moments
from pyrocko.gf.seismosizer import MTSource time, lat, lon, north_shift, east_shift, depth = \ self.centroid_position()
return MTSource( time=time, lat=lat, lon=lon, north_shift=north_shift, east_shift=east_shift, depth=depth, m6=num.sum(self.m6s, axis=0))
def combine(cls, sources, **kwargs): ''' Combine several discretized source models.
Concatenenates all point sources in the given discretized ``sources``. Care must be taken when using this function that the external amplitude factors and reference times of the parameterized (undiscretized) sources match or are accounted for. '''
if 'm6s' not in kwargs: kwargs['m6s'] = num.vstack([s.m6s for s in sources])
return super(DiscretizedMTSource, cls).combine(sources, **kwargs)
'poroelastic10', )
self.check_scheme(scheme) return self.pp[:, num.newaxis].copy()
self.check_scheme(scheme)
azis, bazis = self.azibazis_to(receiver)
sb = num.sin(bazis*d2r-num.pi) cb = num.cos(bazis*d2r-num.pi)
pp = self.pp n = bazis.size
w_un = cb*pp g_un = filledi(1, n) w_ue = sb*pp g_ue = filledi(1, n) w_ud = pp g_ud = filledi(0, n)
w_tn = cb*pp g_tn = filledi(6, n) w_te = sb*pp g_te = filledi(6, n)
w_pp = pp g_pp = filledi(7, n)
w_dvn = cb*pp g_dvn = filledi(9, n) w_dve = sb*pp g_dve = filledi(9, n) w_dvd = pp g_dvd = filledi(8, n)
return ( ('displacement.n', w_un, g_un), ('displacement.e', w_ue, g_ue), ('displacement.d', w_ud, g_ud), ('vertical_tilt.n', w_tn, g_tn), ('vertical_tilt.e', w_te, g_te), ('pore_pressure', w_pp, g_pp), ('darcy_velocity.n', w_dvn, g_dvn), ('darcy_velocity.e', w_dve, g_dve), ('darcy_velocity.d', w_dvd, g_dvd), )
return self.pp
from pyrocko.gf.seismosizer import PorePressurePointSource time, lat, lon, north_shift, east_shift, depth = \ self.centroid_position()
return PorePressurePointSource( time=time, lat=lat, lon=lon, north_shift=north_shift, east_shift=east_shift, depth=depth, pp=float(num.sum(self.pp)))
def combine(cls, sources, **kwargs): ''' Combine several discretized source models.
Concatenenates all point sources in the given discretized ``sources``. Care must be taken when using this function that the external amplitude factors and reference times of the parameterized (undiscretized) sources match or are accounted for. '''
if 'pp' not in kwargs: kwargs['pp'] = num.concatenate([s.pp for s in sources])
return super(DiscretizedPorePressureSource, cls).combine(sources, **kwargs)
''' Green's function store meta information.
Currently implemented :py:class:`~pyrocko.gf.store.Store` configuration types are:
* :py:class:`~pyrocko.gf.meta.ConfigTypeA` - cylindrical or spherical symmetry, 1D earth model, single receiver depth
* Problem is invariant to horizontal translations and rotations around vertical axis. * All receivers must be at the same depth (e.g. at the surface) * High level index variables: ``(source_depth, receiver_distance, component)``
* :py:class:`~pyrocko.gf.meta.ConfigTypeB` - cylindrical or spherical symmetry, 1D earth model, variable receiver depth
* Symmetries like in Type A but has additional index for receiver depth * High level index variables: ``(source_depth, receiver_distance, receiver_depth, component)``
* :py:class:`~pyrocko.gf.meta.ConfigTypeC` - no symmetrical constraints but fixed receiver positions
* Cartesian source volume around a reference point * High level index variables: ``(ireceiver, source_depth, source_east_shift, source_north_shift, component)`` '''
help='Name of the store. May consist of upper and lower-case letters, ' 'digits, dots and underscores. The name must start with a ' 'letter.')
optional=True, help='Name of the original store, if this store has been derived from ' 'another one (e.g. extracted subset).')
default='1.0', optional=True, help='User-defined version string. Use <major>.<minor> format.')
optional=True, help='Identifier of the backend used to compute the store.')
optional=True, help='Comma-separated list of author names.')
optional=True, help="Author's contact email address.")
optional=True, help='Time of creation of the store.')
Region.T(), help='Geographical regions for which the store is representative.')
optional=True, help='Distance range scope of the store ' '(%s).' % fmt_choices(ScopeType))
optional=True, help='Wave type stored (%s).' % fmt_choices(WaveType))
optional=True, help='Information about the inclusion of near-field terms in the ' 'modelling (%s).' % fmt_choices(NearfieldTermsType))
optional=True, help='Free form textual description of the GF store.')
Reference.T(), help='Reference list to cite the modelling code, earth model or ' 'related work.')
optional=True, help='Layered earth model in ND (named discontinuity) format.')
optional=True, help='Receiver-side layered earth model in ND format.')
optional=True, help='Hint to indicate if the spatial sampling of the store is dense ' 'enough for multi-linear interpolation at the source.')
optional=True, help='Hint to indicate if the spatial sampling of the store is dense ' 'enough for multi-linear interpolation at the receiver.')
optional=True, help='Hint to indicate the lower bound of valid frequencies [Hz].')
optional=True, help='Hint to indicate the upper bound of valid frequencies [Hz].')
optional=True, help='Sample rate of the GF store [Hz].')
default=1.0, help='Gain value, factored out of the stored GF samples. ' '(may not work properly, keep at 1.0).', optional=True)
default='elastic10', help='GF component scheme (%s).' % fmt_choices(ComponentScheme))
optional=True, help='Physical quantity of stored values (%s). If not given, a ' 'default is used based on the GF component scheme. The default ' 'for the ``"elastic*"`` family of component schemes is ' '``"displacement"``.' % fmt_choices(QuantityType))
TPDef.T(), help='Mapping of phase names to phase definitions, for which travel ' 'time tables are available in the GF store.')
optional=True, help='Number of GF components. Use :gattr:`component_scheme` instead.')
optional=True, help='Heuristic hash value which can be used to uniquely identify the ' 'GF store for practical purposes.')
optional=True, help='Store reference name composed of the store\'s :gattr:`id` and ' 'the first six letters of its :gattr:`uuid`.')
self.component_scheme].ncomponents
self.ncomponents = ncomponents raise InvalidNComponents( 'ncomponents=%i incompatible with component_scheme="%s"' % ( self.ncomponents, self.component_scheme))
self.update()
return self._index_function(*args)
return self._indices_function(*args)
return self._vicinity_function(*args)
return self._vicinities_function(*args)
return self._grid_interpolation_coefficients(*args)
return nodes(self.coords[minlevel:level])
return nditer_outer(self.coords[minlevel:level])
i = 0 arrs = [] ntotal = 1 for mi, ma, inc in zip(self.mins, self.effective_maxs, self.deltas): if gdef and len(gdef) > i: sssn = gdef[i] else: sssn = (None,)*4
arr = num.linspace(*start_stop_num(*(sssn + (mi, ma, inc)))) ntotal *= len(arr)
arrs.append(arr) i += 1
arrs.append(self.coords[-1]) return nditer_outer(arrs[:level])
nthreads=0): assert implementation in ['c', 'python']
out = [] delays = source.times for comp, weights, icomponents in source.make_weights( receiver, self.component_scheme):
weights *= self.factor
args = self.make_indexing_args(source, receiver, icomponents) delays_expanded = num.tile(delays, icomponents.size//delays.size) out.append((comp, args, delays_expanded, weights))
return out
raise NotImplementedError('should be implemented in subclass')
interpolation=None): ''' Get shear moduli at given points from contained velocity model.
:param lat: surface origin for coordinate system of ``points`` :param points: NumPy array of shape ``(N, 3)``, where each row is a point ``(north, east, depth)``, relative to origin at ``(lat, lon)`` :param interpolation: interpolation method. Choose from ``('nearest_neighbor', 'multilinear')`` :returns: NumPy array of length N with extracted shear moduli at each point
The default implementation retrieves and interpolates the shear moduli from the contained 1D velocity profile. ''' parameter='shear_moduli', interpolation=interpolation)
''' Get Vs at given points from contained velocity model.
:param lat: surface origin for coordinate system of ``points`` :param points: NumPy array of shape ``(N, 3)``, where each row is a point ``(north, east, depth)``, relative to origin at ``(lat, lon)`` :param interpolation: interpolation method. Choose from ``('nearest_neighbor', 'multilinear')`` :returns: NumPy array of length N with extracted shear moduli at each point
The default implementation retrieves and interpolates Vs from the contained 1D velocity profile. ''' return self.get_material_property(lat, lon, points, parameter='vs', interpolation=interpolation)
''' Get Vp at given points from contained velocity model.
:param lat: surface origin for coordinate system of ``points`` :param points: NumPy array of shape ``(N, 3)``, where each row is a point ``(north, east, depth)``, relative to origin at ``(lat, lon)`` :param interpolation: interpolation method. Choose from ``('nearest_neighbor', 'multilinear')`` :returns: NumPy array of length N with extracted shear moduli at each point
The default implementation retrieves and interpolates Vp from the contained 1D velocity profile. ''' return self.get_material_property(lat, lon, points, parameter='vp', interpolation=interpolation)
''' Get rho at given points from contained velocity model.
:param lat: surface origin for coordinate system of ``points`` :param points: NumPy array of shape ``(N, 3)``, where each row is a point ``(north, east, depth)``, relative to origin at ``(lat, lon)`` :param interpolation: interpolation method. Choose from ``('nearest_neighbor', 'multilinear')`` :returns: NumPy array of length N with extracted shear moduli at each point
The default implementation retrieves and interpolates rho from the contained 1D velocity profile. ''' return self.get_material_property(lat, lon, points, parameter='rho', interpolation=interpolation)
interpolation=None):
raise TypeError('Interpolation method not defined! available: ' "multilinear", "nearest_neighbor")
vs_profile = earthmod.profile('vs') profile = num.interp( store_depth_profile, z_profile, vs_profile)
vp_profile = earthmod.profile('vp') profile = num.interp( store_depth_profile, z_profile, vp_profile)
rho_profile = earthmod.profile('rho')
profile = num.interp( store_depth_profile, z_profile, rho_profile)
store_depth_profile, z_profile, vs_profile) store_depth_profile, z_profile, rho_profile)
else: raise TypeError( 'parameter %s not available' % parameter)
elif interpolation == 'nearest_neighbor': kind = 'nearest' else: raise TypeError( 'Interpolation method %s not available' % interpolation)
except ValueError: raise OutOfBounds()
if self.modelling_code_id in ('psgrn_pscmp', 'poel'): return True return False
return not self.is_static()
raise NotImplementedError('must be implemented in subclass')
''' Get tabulated phase definition. '''
for pdef in self.tabulated_phases: if pdef.id == phase_id: return pdef
raise StoreError('No such phase: %s' % phase_id)
raise StoreError( 'Cannot fix travel time table holes in GF stores of type %s.' % self.short_type)
''' Cylindrical symmetry, 1D earth model, single receiver depth
* Problem is invariant to horizontal translations and rotations around vertical axis.
* All receivers must be at the same depth (e.g. at the surface) High level index variables: ``(source_depth, distance, component)``
* The ``distance`` is the surface distance between source and receiver points. '''
default=0.0, help='Fixed receiver depth [m].')
help='Minimum source depth [m].')
help='Maximum source depth [m].')
help='Grid spacing of source depths [m]')
help='Minimum source-receiver surface distance [m].')
help='Maximum source-receiver surface distance [m].')
help='Grid spacing of source-receiver surface distance [m].')
'elastic2', 'elastic5', 'elastic8', 'elastic10', 'poroelastic10']
return math.sqrt(args[0]**2 + args[1]**2)
return args[0]
return self.receiver_depth
[self.source_depth_min, self.distance_min], dtype=num.float) [self.source_depth_max, self.distance_max], dtype=num.float) [self.source_depth_delta, self.distance_delta], dtype=num.float) vicinity_eps).astype(num.int) + 1 (mi, ma, n) in zip(self.mins, self.effective_maxs, self.ns)) + \ (num.arange(self.ncomponents),)
ia = int(round((a - amin) / da)) ib = int(round((b - bmin) / db)) try: return num.ravel_multi_index((ia, ib, ig), (na, nb, ng)) except ValueError: raise OutOfBounds()
ia = num.round((a - amin) / da).astype(int) ib = num.round((b - bmin) / db).astype(int) try: return num.ravel_multi_index((ia, ib, ig), (na, nb, ng)) except ValueError: for ia_, ib_, ig_ in zip(ia, ib, ig): try: num.ravel_multi_index((ia_, ib_, ig_), (na, nb, ng)) except ValueError: raise OutOfBounds()
ias = indi12((a - amin) / da, na) ibs = indi12((b - bmin) / db, nb) return ias, ibs
ias, ibs = grid_interpolation_coefficients(a, b)
if not (0 <= ig < ng): raise OutOfBounds()
indis = [] weights = [] for ia, va in ias: iia = ia*nb*ng for ib, vb in ibs: indis.append(iia + ib*ng + ig) weights.append(va*vb)
return num.array(indis), num.array(weights)
xa = (a - amin) / da xb = (b - bmin) / db
xa_fl = num.floor(xa) xa_ce = num.ceil(xa) xb_fl = num.floor(xb) xb_ce = num.ceil(xb) va_fl = 1.0 - (xa - xa_fl) va_ce = (1.0 - (xa_ce - xa)) * (xa_ce - xa_fl) vb_fl = 1.0 - (xb - xb_fl) vb_ce = (1.0 - (xb_ce - xb)) * (xb_ce - xb_fl)
ia_fl = xa_fl.astype(num.int) ia_ce = xa_ce.astype(num.int) ib_fl = xb_fl.astype(num.int) ib_ce = xb_ce.astype(num.int)
if num.any(ia_fl < 0) or num.any(ia_fl >= na): raise OutOfBounds()
if num.any(ia_ce < 0) or num.any(ia_ce >= na): raise OutOfBounds()
if num.any(ib_fl < 0) or num.any(ib_fl >= nb): raise OutOfBounds()
if num.any(ib_ce < 0) or num.any(ib_ce >= nb): raise OutOfBounds()
irecords = num.empty(a.size*4, dtype=num.int) irecords[0::4] = ia_fl*nb*ng + ib_fl*ng + ig irecords[1::4] = ia_ce*nb*ng + ib_fl*ng + ig irecords[2::4] = ia_fl*nb*ng + ib_ce*ng + ig irecords[3::4] = ia_ce*nb*ng + ib_ce*ng + ig
weights = num.empty(a.size*4, dtype=num.float) weights[0::4] = va_fl * vb_fl weights[1::4] = va_ce * vb_fl weights[2::4] = va_fl * vb_ce weights[3::4] = va_ce * vb_ce
return irecords, weights
nc = icomponents.size dists = source.distances_to(receiver) n = dists.size return (num.tile(source.depths, nc//n), num.tile(dists, nc//n), icomponents)
def short_extent(self): return '%g:%g:%g x %g:%g:%g' % ( self.source_depth_min/km, self.source_depth_max/km, self.source_depth_delta/km, self.distance_min/km, self.distance_max/km, self.distance_delta/km)
from pyrocko import eikonal_ext, spit
nodes = self.nodes(level=-1)
delta = self.deltas[-1] assert num.all(delta == self.deltas)
nsources, ndistances = self.ns
points = num.zeros((nodes.shape[0], 3)) points[:, 0] = nodes[:, 1] points[:, 2] = nodes[:, 0]
speeds = self.get_material_property( 0., 0., points, parameter='vp' if mode == cake.P else 'vs', interpolation='multilinear')
speeds = speeds.reshape((nsources, ndistances))
times = sptree.interpolate_many(nodes)
times[num.isnan(times)] = -1. times = times.reshape(speeds.shape)
try: eikonal_ext.eikonal_solver_fmm_cartesian( speeds, times, delta) except eikonal_ext.EikonalExtError as e: if str(e).endswith('please check results'): logger.debug( 'Got a warning from eikonal solver ' '- may be ok...') else: raise
def func(x): ibs, ics = \ self.grid_interpolation_coefficients(*x)
t = 0 for ib, vb in ibs: for ic, vc in ics: t += times[ib, ic] * vb * vc
return t
return spit.SPTree( f=func, ftol=sptree.ftol, xbounds=sptree.xbounds, xtols=sptree.xtols)
''' Cylindrical symmetry, 1D earth model, variable receiver depth
* Symmetries like in :py:class:`ConfigTypeA` but has additional index for receiver depth
* High level index variables: ``(source_depth, receiver_distance, receiver_depth, component)`` '''
help='Minimum receiver depth [m].')
help='Maximum receiver depth [m].')
help='Grid spacing of receiver depths [m]')
help='Minimum source depth [m].')
help='Maximum source depth [m].')
help='Grid spacing of source depths [m]')
help='Minimum source-receiver surface distance [m].')
help='Maximum source-receiver surface distance [m].')
help='Grid spacing of source-receiver surface distances [m].')
'elastic2', 'elastic5', 'elastic8', 'elastic10', 'poroelastic10']
return math.sqrt((args[1] - args[0])**2 + args[2]**2)
return args[2]
return args[1]
return args[0]
return self.coords[1]
self.mins = num.array([ self.receiver_depth_min, self.source_depth_min, self.distance_min], dtype=num.float)
self.maxs = num.array([ self.receiver_depth_max, self.source_depth_max, self.distance_max], dtype=num.float)
self.deltas = num.array([ self.receiver_depth_delta, self.source_depth_delta, self.distance_delta], dtype=num.float)
self.ns = num.floor((self.maxs - self.mins) / self.deltas + vicinity_eps).astype(num.int) + 1 self.effective_maxs = self.mins + self.deltas * (self.ns - 1) self.deltat = 1.0/self.sample_rate self.nrecords = num.product(self.ns) * self.ncomponents self.coords = tuple(num.linspace(mi, ma, n) for (mi, ma, n) in zip(self.mins, self.effective_maxs, self.ns)) + \ (num.arange(self.ncomponents),) self.nreceiver_depths, self.nsource_depths, self.ndistances = self.ns
amin, bmin, cmin = self.mins da, db, dc = self.deltas na, nb, nc = self.ns ng = self.ncomponents
def index_function(a, b, c, ig): ia = int(round((a - amin) / da)) ib = int(round((b - bmin) / db)) ic = int(round((c - cmin) / dc)) try: return num.ravel_multi_index((ia, ib, ic, ig), (na, nb, nc, ng)) except ValueError: raise OutOfBounds()
def indices_function(a, b, c, ig): ia = num.round((a - amin) / da).astype(int) ib = num.round((b - bmin) / db).astype(int) ic = num.round((c - cmin) / dc).astype(int) try: return num.ravel_multi_index((ia, ib, ic, ig), (na, nb, nc, ng)) except ValueError: raise OutOfBounds()
def grid_interpolation_coefficients(a, b, c): ias = indi12((a - amin) / da, na) ibs = indi12((b - bmin) / db, nb) ics = indi12((c - cmin) / dc, nc) return ias, ibs, ics
def vicinity_function(a, b, c, ig): ias, ibs, ics = grid_interpolation_coefficients(a, b, c)
if not (0 <= ig < ng): raise OutOfBounds()
indis = [] weights = [] for ia, va in ias: iia = ia*nb*nc*ng for ib, vb in ibs: iib = ib*nc*ng for ic, vc in ics: indis.append(iia + iib + ic*ng + ig) weights.append(va*vb*vc)
return num.array(indis), num.array(weights)
def vicinities_function(a, b, c, ig):
xa = (a - amin) / da xb = (b - bmin) / db xc = (c - cmin) / dc
xa_fl = num.floor(xa) xa_ce = num.ceil(xa) xb_fl = num.floor(xb) xb_ce = num.ceil(xb) xc_fl = num.floor(xc) xc_ce = num.ceil(xc) va_fl = 1.0 - (xa - xa_fl) va_ce = (1.0 - (xa_ce - xa)) * (xa_ce - xa_fl) vb_fl = 1.0 - (xb - xb_fl) vb_ce = (1.0 - (xb_ce - xb)) * (xb_ce - xb_fl) vc_fl = 1.0 - (xc - xc_fl) vc_ce = (1.0 - (xc_ce - xc)) * (xc_ce - xc_fl)
ia_fl = xa_fl.astype(num.int) ia_ce = xa_ce.astype(num.int) ib_fl = xb_fl.astype(num.int) ib_ce = xb_ce.astype(num.int) ic_fl = xc_fl.astype(num.int) ic_ce = xc_ce.astype(num.int)
if num.any(ia_fl < 0) or num.any(ia_fl >= na): raise OutOfBounds()
if num.any(ia_ce < 0) or num.any(ia_ce >= na): raise OutOfBounds()
if num.any(ib_fl < 0) or num.any(ib_fl >= nb): raise OutOfBounds()
if num.any(ib_ce < 0) or num.any(ib_ce >= nb): raise OutOfBounds()
if num.any(ic_fl < 0) or num.any(ic_fl >= nc): raise OutOfBounds()
if num.any(ic_ce < 0) or num.any(ic_ce >= nc): raise OutOfBounds()
irecords = num.empty(a.size*8, dtype=num.int) irecords[0::8] = ia_fl*nb*nc*ng + ib_fl*nc*ng + ic_fl*ng + ig irecords[1::8] = ia_ce*nb*nc*ng + ib_fl*nc*ng + ic_fl*ng + ig irecords[2::8] = ia_fl*nb*nc*ng + ib_ce*nc*ng + ic_fl*ng + ig irecords[3::8] = ia_ce*nb*nc*ng + ib_ce*nc*ng + ic_fl*ng + ig irecords[4::8] = ia_fl*nb*nc*ng + ib_fl*nc*ng + ic_ce*ng + ig irecords[5::8] = ia_ce*nb*nc*ng + ib_fl*nc*ng + ic_ce*ng + ig irecords[6::8] = ia_fl*nb*nc*ng + ib_ce*nc*ng + ic_ce*ng + ig irecords[7::8] = ia_ce*nb*nc*ng + ib_ce*nc*ng + ic_ce*ng + ig
weights = num.empty(a.size*8, dtype=num.float) weights[0::8] = va_fl * vb_fl * vc_fl weights[1::8] = va_ce * vb_fl * vc_fl weights[2::8] = va_fl * vb_ce * vc_fl weights[3::8] = va_ce * vb_ce * vc_fl weights[4::8] = va_fl * vb_fl * vc_ce weights[5::8] = va_ce * vb_fl * vc_ce weights[6::8] = va_fl * vb_ce * vc_ce weights[7::8] = va_ce * vb_ce * vc_ce
return irecords, weights
self._index_function = index_function self._indices_function = indices_function self._grid_interpolation_coefficients = grid_interpolation_coefficients self._vicinity_function = vicinity_function self._vicinities_function = vicinities_function
nc = icomponents.size dists = source.distances_to(receiver) n = dists.size receiver_depths = num.empty(nc) receiver_depths.fill(receiver.depth) return (receiver_depths, num.tile(source.depths, nc//n), num.tile(dists, nc//n), icomponents)
return (receiver.depth, source.depth, source.distance_to(receiver))
def short_extent(self): return '%g:%g:%g x %g:%g:%g x %g:%g:%g' % ( self.receiver_depth_min/km, self.receiver_depth_max/km, self.receiver_depth_delta/km, self.source_depth_min/km, self.source_depth_max/km, self.source_depth_delta/km, self.distance_min/km, self.distance_max/km, self.distance_delta/km)
from pyrocko import eikonal_ext, spit
nodes_sr = self.nodes(minlevel=1, level=-1)
delta = self.deltas[-1] assert num.all(delta == self.deltas[1:])
nreceivers, nsources, ndistances = self.ns
points = num.zeros((nodes_sr.shape[0], 3)) points[:, 0] = nodes_sr[:, 1] points[:, 2] = nodes_sr[:, 0]
speeds = self.get_material_property( 0., 0., points, parameter='vp' if mode == cake.P else 'vs', interpolation='multilinear')
speeds = speeds.reshape((nsources, ndistances))
receiver_times = [] for ireceiver in range(nreceivers): nodes = num.hstack([ num_full( (nodes_sr.shape[0], 1), self.coords[0][ireceiver]), nodes_sr])
times = sptree.interpolate_many(nodes)
times[num.isnan(times)] = -1.
times = times.reshape(speeds.shape)
try: eikonal_ext.eikonal_solver_fmm_cartesian( speeds, times, delta) except eikonal_ext.EikonalExtError as e: if str(e).endswith('please check results'): logger.debug( 'Got a warning from eikonal solver ' '- may be ok...') else: raise
receiver_times.append(times)
def func(x): ias, ibs, ics = \ self.grid_interpolation_coefficients(*x)
t = 0 for ia, va in ias: times = receiver_times[ia] for ib, vb in ibs: for ic, vc in ics: t += times[ib, ic] * va * vb * vc
return t
return spit.SPTree( f=func, ftol=sptree.ftol, xbounds=sptree.xbounds, xtols=sptree.xtols)
''' No symmetrical constraints but fixed receiver positions.
* Cartesian 3D source volume around a reference point
* High level index variables: ``(ireceiver, source_depth, source_east_shift, source_north_shift, component)`` '''
Receiver.T(), help='List of fixed receivers.')
help='Origin of the source volume grid.')
help='Minimum source depth [m].')
help='Maximum source depth [m].')
help='Source depth grid spacing [m].')
help='Minimum easting of source grid [m].')
help='Maximum easting of source grid [m].')
help='Source volume grid spacing in east direction [m].')
help='Minimum northing of source grid [m].')
help='Maximum northing of source grid [m].')
help='Source volume grid spacing in north direction [m].')
ireceiver, _, source_east_shift, source_north_shift, _ = args sorig = self.source_origin sloc = Location( lat=sorig.lat, lon=sorig.lon, north_shift=sorig.north_shift + source_north_shift, east_shift=sorig.east_shift + source_east_shift)
return self.receivers[args[0]].distance_to(sloc)
# to be improved... ireceiver, sdepth, source_east_shift, source_north_shift, _ = args sorig = self.source_origin sloc = Location( lat=sorig.lat, lon=sorig.lon, north_shift=sorig.north_shift + source_north_shift, east_shift=sorig.east_shift + source_east_shift)
return math.sqrt( self.receivers[args[0]].distance_to(sloc)**2 + sdepth**2)
return args[1]
return self.receivers[args[0]].depth
return self.coords[0]
self.mins = num.array([ self.source_depth_min, self.source_east_shift_min, self.source_north_shift_min], dtype=num.float)
self.maxs = num.array([ self.source_depth_max, self.source_east_shift_max, self.source_north_shift_max], dtype=num.float)
self.deltas = num.array([ self.source_depth_delta, self.source_east_shift_delta, self.source_north_shift_delta], dtype=num.float)
self.ns = num.floor((self.maxs - self.mins) / self.deltas + vicinity_eps).astype(num.int) + 1 self.effective_maxs = self.mins + self.deltas * (self.ns - 1) self.deltat = 1.0/self.sample_rate self.nreceivers = len(self.receivers) self.nrecords = \ self.nreceivers * num.product(self.ns) * self.ncomponents
self.coords = (num.arange(self.nreceivers),) + \ tuple(num.linspace(mi, ma, n) for (mi, ma, n) in zip(self.mins, self.effective_maxs, self.ns)) + \ (num.arange(self.ncomponents),) self.nreceiver_depths, self.nsource_depths, self.ndistances = self.ns
self._distances_cache = {}
amin, bmin, cmin = self.mins da, db, dc = self.deltas na, nb, nc = self.ns ng = self.ncomponents nr = self.nreceivers
def index_function(ir, a, b, c, ig): ia = int(round((a - amin) / da)) ib = int(round((b - bmin) / db)) ic = int(round((c - cmin) / dc)) try: return num.ravel_multi_index((ir, ia, ib, ic, ig), (nr, na, nb, nc, ng)) except ValueError: raise OutOfBounds()
def indices_function(ir, a, b, c, ig): ia = num.round((a - amin) / da).astype(int) ib = num.round((b - bmin) / db).astype(int) ic = num.round((c - cmin) / dc).astype(int)
try: return num.ravel_multi_index((ir, ia, ib, ic, ig), (nr, na, nb, nc, ng)) except ValueError: raise OutOfBounds()
def vicinity_function(ir, a, b, c, ig): ias = indi12((a - amin) / da, na) ibs = indi12((b - bmin) / db, nb) ics = indi12((c - cmin) / dc, nc)
if not (0 <= ir < nr): raise OutOfBounds()
if not (0 <= ig < ng): raise OutOfBounds()
indis = [] weights = [] iir = ir*na*nb*nc*ng for ia, va in ias: iia = ia*nb*nc*ng for ib, vb in ibs: iib = ib*nc*ng for ic, vc in ics: indis.append(iir + iia + iib + ic*ng + ig) weights.append(va*vb*vc)
return num.array(indis), num.array(weights)
def vicinities_function(ir, a, b, c, ig):
xa = (a-amin) / da xb = (b-bmin) / db xc = (c-cmin) / dc
xa_fl = num.floor(xa) xa_ce = num.ceil(xa) xb_fl = num.floor(xb) xb_ce = num.ceil(xb) xc_fl = num.floor(xc) xc_ce = num.ceil(xc) va_fl = 1.0 - (xa - xa_fl) va_ce = (1.0 - (xa_ce - xa)) * (xa_ce - xa_fl) vb_fl = 1.0 - (xb - xb_fl) vb_ce = (1.0 - (xb_ce - xb)) * (xb_ce - xb_fl) vc_fl = 1.0 - (xc - xc_fl) vc_ce = (1.0 - (xc_ce - xc)) * (xc_ce - xc_fl)
ia_fl = xa_fl.astype(num.int) ia_ce = xa_ce.astype(num.int) ib_fl = xb_fl.astype(num.int) ib_ce = xb_ce.astype(num.int) ic_fl = xc_fl.astype(num.int) ic_ce = xc_ce.astype(num.int)
if num.any(ia_fl < 0) or num.any(ia_fl >= na): raise OutOfBounds()
if num.any(ia_ce < 0) or num.any(ia_ce >= na): raise OutOfBounds()
if num.any(ib_fl < 0) or num.any(ib_fl >= nb): raise OutOfBounds()
if num.any(ib_ce < 0) or num.any(ib_ce >= nb): raise OutOfBounds()
if num.any(ic_fl < 0) or num.any(ic_fl >= nc): raise OutOfBounds()
if num.any(ic_ce < 0) or num.any(ic_ce >= nc): raise OutOfBounds()
irig = ir*na*nb*nc*ng + ig
irecords = num.empty(a.size*8, dtype=num.int) irecords[0::8] = ia_fl*nb*nc*ng + ib_fl*nc*ng + ic_fl*ng + irig irecords[1::8] = ia_ce*nb*nc*ng + ib_fl*nc*ng + ic_fl*ng + irig irecords[2::8] = ia_fl*nb*nc*ng + ib_ce*nc*ng + ic_fl*ng + irig irecords[3::8] = ia_ce*nb*nc*ng + ib_ce*nc*ng + ic_fl*ng + irig irecords[4::8] = ia_fl*nb*nc*ng + ib_fl*nc*ng + ic_ce*ng + irig irecords[5::8] = ia_ce*nb*nc*ng + ib_fl*nc*ng + ic_ce*ng + irig irecords[6::8] = ia_fl*nb*nc*ng + ib_ce*nc*ng + ic_ce*ng + irig irecords[7::8] = ia_ce*nb*nc*ng + ib_ce*nc*ng + ic_ce*ng + irig
weights = num.empty(a.size*8, dtype=num.float) weights[0::8] = va_fl * vb_fl * vc_fl weights[1::8] = va_ce * vb_fl * vc_fl weights[2::8] = va_fl * vb_ce * vc_fl weights[3::8] = va_ce * vb_ce * vc_fl weights[4::8] = va_fl * vb_fl * vc_ce weights[5::8] = va_ce * vb_fl * vc_ce weights[6::8] = va_fl * vb_ce * vc_ce weights[7::8] = va_ce * vb_ce * vc_ce
return irecords, weights
self._index_function = index_function self._indices_function = indices_function self._vicinity_function = vicinity_function self._vicinities_function = vicinities_function
k = (receiver.lat, receiver.lon, receiver.north_shift, receiver.east_shift) dh = min(self.source_north_shift_delta, self.source_east_shift_delta) dv = self.source_depth_delta
for irec, rec in enumerate(self.receivers): if (k, irec) not in self._distances_cache: self._distances_cache[k, irec] = math.sqrt( (receiver.distance_to(rec)/dh)**2 + ((rec.depth - receiver.depth)/dv)**2)
if self._distances_cache[k, irec] < 0.1: return irec
raise OutOfBounds( reason='No GFs available for receiver at (%g, %g).' % receiver.effective_latlon)
nc = icomponents.size
dists = source.distances_to(self.source_origin) azis, _ = source.azibazis_to(self.source_origin)
source_north_shifts = - num.cos(d2r*azis) * dists source_east_shifts = - num.sin(d2r*azis) * dists source_depths = source.depths - self.source_origin.depth
n = dists.size ireceivers = num.empty(nc, dtype=num.int) ireceivers.fill(self.lookup_ireceiver(receiver))
return (ireceivers, num.tile(source_depths, nc//n), num.tile(source_east_shifts, nc//n), num.tile(source_north_shifts, nc//n), icomponents)
dist = source.distance_to(self.source_origin) azi, _ = source.azibazi_to(self.source_origin)
source_north_shift = - num.cos(d2r*azi) * dist source_east_shift = - num.sin(d2r*azi) * dist source_depth = source.depth - self.source_origin.depth
return (self.lookup_ireceiver(receiver), source_depth, source_east_shift, source_north_shift)
def short_extent(self): return '%g:%g:%g x %g:%g:%g x %g:%g:%g' % ( self.source_depth_min/km, self.source_depth_max/km, self.source_depth_delta/km, self.source_east_shift_min/km, self.source_east_shift_max/km, self.source_east_shift_delta/km, self.source_north_shift_min/km, self.source_north_shift_max/km, self.source_north_shift_delta/km)
choices=['cos', 'linear'], default='cos', optional=True)
self._pattern = pattern SObject.__init__(self)
def __str__(self): return self._pattern
def regex(self): pool = SimplePattern._pool if self.pattern not in pool: rpat = '|'.join(fnmatch.translate(x) for x in self.pattern.split('|')) pool[self.pattern] = re.compile(rpat, re.I)
return pool[self.pattern]
return self.regex.match(s)
'amp_spec_dis', 'amp_spec_vel', 'amp_spec_acc', 'envelope_dis', 'envelope_vel', 'envelope_acc']
# filter = FrequencyResponse.T()
''' Get linear interpolation index and weight. '''
r = round(x) if abs(r - x) < vicinity_eps: i = int(r) if not (0 <= i < n): raise OutOfBounds()
return ((int(r), 1.),) else: f = math.floor(x) i = int(f) if not (0 <= i < n-1): raise OutOfBounds()
v = x-f return ((i, 1.-v), (i + 1, v))
units = { 'k': 1e3, 'M': 1e6, }
factor = 1.0 if s and s[-1] in units: factor = units[s[-1]] s = s[:-1] if not s: raise ValueError('unit without a number: \'%s\'' % s)
if s: return float(s) * factor else: return None
Exception.__init__(self, 'invalid grid specification: %s' % s)
try: result = [] for dspec in spec.split(','): t = dspec.split('@') num = start = stop = step = None if len(t) == 2: num = int(t[1]) if num <= 0: raise GridSpecError(spec)
elif len(t) > 2: raise GridSpecError(spec)
s = t[0] v = [float_or_none(x) for x in s.split(':')] if len(v) == 1: start = stop = v[0] if len(v) >= 2: start, stop = v[0:2] if len(v) == 3: step = v[2]
if len(v) > 3 or (len(v) > 2 and num is not None): raise GridSpecError(spec)
if step == 0.0: raise GridSpecError(spec)
result.append((start, stop, step, num))
except ValueError: raise GridSpecError(spec)
return result
swap = step is not None and step < 0. if start is None: start = [mi, ma][swap] if stop is None: stop = [ma, mi][swap] if step is None: step = [inc, -inc][ma < mi] if num is None: if (step < 0) != (stop-start < 0): raise GridSpecError()
num = int(round((stop-start)/step))+1 stop2 = start + (num-1)*step if abs(stop-stop2) > eps: num = int(math.floor((stop-start)/step))+1 stop = start + (num-1)*step else: stop = stop2
if start == stop: num = 1
return start, stop, num
return num.nditer( x, op_axes=(num.identity(len(x), dtype=num.int)-1).tolist())
ns = [x.size for x in xs] nnodes = num.prod(ns) ndim = len(xs) nodes = num.empty((nnodes, ndim), dtype=xs[0].dtype) for idim in range(ndim-1, -1, -1): x = xs[idim] nrepeat = num.prod(ns[idim+1:], dtype=num.int) ntile = num.prod(ns[:idim], dtype=num.int) nodes[:, idim] = num.repeat(num.tile(x, ntile), nrepeat)
return nodes
a = num.empty(n, dtype=num.int) a.fill(x) return a
DiscretizedExplosionSource, DiscretizedSFSource, DiscretizedMTSource, DiscretizedPorePressureSource]
Earthmodel1D StringID ScopeType WaveformType QuantityType NearfieldTermsType Reference Region CircularRegion RectangularRegion PhaseSelect InvalidTimingSpecification Timing TPDef OutOfBounds Location Receiver '''.split() + [ S.__name__ for S in discretized_source_classes + config_type_classes] + ''' ComponentScheme component_scheme_to_description component_schemes Config GridSpecError Weighting Taper SimplePattern WaveformType ChannelSelection StationSelection WaveformSelection nditer_outer dump load discretized_source_classes config_type_classes UnavailableScheme InterpolationMethod SeismosizerTrace SeismosizerResult Result StaticResult '''.split() |