Files
simpeg/SimPEG/Model.py
T

95 lines
2.5 KiB
Python

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