simpeg.electromagnetics.time_domain.Simulation3DMagneticField.getRHS#
- Simulation3DMagneticField.getRHS(tInd)[source]#
- Right-hand sides for the given time index. - This method returns the right-hand sides for the time index provided. The right-hand side for each source is constructed according to: \[\mathbf{q}_k = \mathbf{C^T M_{f\rho} s}_{\mathbf{e},k} \; - \frac{1}{\Delta t_k} \big [ \mathbf{s}_{\mathbf{m},k} + \mathbf{s}_{\mathbf{m},k-1} \big ]\]- where - \(\Delta t_k\) is the step length 
- \(\mathbf{C}\) is the discrete curl operator 
- \(\mathbf{s_m}\) and \(\mathbf{s_e}\) are the integrated magnetic and electric source terms, respectively 
- \(\mathbf{M_{f\rho}}\) is the inner-product matrix for resisitivites projected to faces 
 - See the Notes section of the doc strings for - Simulation3DMagneticFieldfor a full description of the formulation.- Parameters:
- tIndint
- The time index; between - [0, n_steps].
 
- tInd
- Returns:
- (n_edges,n_sources)numpy.ndarray
- The right-hand sides. 
 
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