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95 lines
2.5 KiB
Python
95 lines
2.5 KiB
Python
from SimPEG import Utils, np, sp
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class BaseModel(object):
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"""SimPEG Model"""
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__metaclass__ = Utils.Save.Savable
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counter = None #: A SimPEG.Utils.Counter object
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def __init__(self):
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pass
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def transform(self, m):
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"""
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:param numpy.array m: model
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:rtype: numpy.array
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:return: transformed model
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The *transform* changes the model into the physical property.
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A common example of this is to invert for electrical conductivity
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in log space. In this case, your model will be log(sigma) and to
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get back to sigma, you can take the exponential:
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"""
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return m
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def transformDeriv(self, m):
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"""
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:param numpy.array m: model
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:rtype: scipy.csr_matrix
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:return: derivative of transformed model
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The *transform* changes the model into the physical property.
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The *transformDeriv* provides the derivative of the *transform*.
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"""
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return sp.identity(m.size)
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def example(self, mesh, type=None):
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return np.random.rand(mesh.nC)
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class LogModel(BaseModel):
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"""SimPEG LogModel"""
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def __init__(self, **kwargs):
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BaseModel.__init__(self, **kwargs)
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def transform(self, m):
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"""
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:param numpy.array m: model
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:rtype: numpy.array
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:return: transformed model
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The *transform* changes the model into the physical property.
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A common example of this is to invert for electrical conductivity
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in log space. In this case, your model will be log(sigma) and to
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get back to sigma, you can take the exponential:
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.. math::
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m = \log{\sigma}
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\exp{m} = \exp{\log{\sigma}} = \sigma
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"""
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return np.exp(Utils.mkvc(m))
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def transformDeriv(self, m):
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"""
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:param numpy.array m: model
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:rtype: scipy.csr_matrix
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:return: derivative of transformed model
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The *transform* changes the model into the physical property.
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The *transformDeriv* provides the derivative of the *transform*.
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If the model *transform* is:
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.. math::
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m = \log{\sigma}
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\exp{m} = \exp{\log{\sigma}} = \sigma
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Then the derivative is:
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.. math::
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\\frac{\partial \exp{m}}{\partial m} = \\text{sdiag}(\exp{m})
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"""
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return Utils.sdiag(np.exp(Utils.mkvc(m)))
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