simpeg.electromagnetics.time_domain.simulation.BaseTDEMSimulation.Adcinv#

property BaseTDEMSimulation.Adcinv#

Inverse of the factored system matrix for the DC resistivity problem.

The solution to the DC resistivity problem is necessary at the initial time for galvanic sources whose currents are non-zero at the initial time. This property is used to compute and store the inverse of the factored linear system matrix for the DC resistivity problem given by:

\[\mathbf{A_{dc}} \, \boldsymbol{\phi_0} = \mathbf{q_{dc}}\]

where \(\mathbf{A_{dc}}\) is the system matrix, \(\boldsymbol{\phi_0}\) represents the discrete solution for the electric potential and \(\mathbf{q_{dc}}\) is the discrete right-hand side. Electric fields are computed by applying a discrete gradient operator to the discrete electric potential solution.

Returns:
pymatsolver.solvers.Base

Inver of the factored systems matrix for the DC resistivity problem.

Notes

See the docstrings for resistivity.BaseDCSimulation, resistivity.Simulation3DCellCentered and resistivity.Simulation3DNodal to learn more about how the DC resistivity problem is solved.