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Dr. P. F. Chen (hereafter PFC) has questioned two main differences between the CDK analogue model and his FDM numerical results: 1) The CDK analogue model in-phase Vy fall off rapidly with increasing period, whereas his numeri- cal Hz/Hy do not; 2) The CDK quadrature Vy do not show a reversal, whereas his Hz/Hy do. Upon examining the curves in Fig. 4 carefully, it can be concluded that the CDK quadra- ture Vy do, in fact, also indicate a reversal. It can clearly be seen from the shape of the CDK curves (dashed line), that with decreasing period each response curve is approaching a reversal, though at a period some what below 1 min, being the lowest period included in the analogue model measure- ments. The CDK in-phase response curves as well, are each approaching a maximum at periods well below 1 min, and should each reach a maximum at roughly the same period as the corresponding quadrature reversal, being characteristic of the specific location ( y) between the conductors. These shifts to longer periods with distance indicated in the CDK results, are similar to those in the PFC (solid line) results which for sites at increasing distances from the major conductor (b), show shifts to longer periods to be roughly Tc = 2, 3, and 8 min at y =− 45, −40, and −30 km respectively. With respect to the more rapid fall-off in-phase response with in- creasing period, as well as the quadrature reversals at lower periods in the CDK 3D results as compared with the PFC re- sults, these are precisely the characteristics that distinguish 3D from 2D responses. The CDK model for the 1-60 min period range is certainly 3D for all but the shortest periods, since for the near-end (x = 30 km) traverse the conductor length is definitely too small to satisfy the criteron for a 2D conductor in terms of host conductivity skin depths. Thus, the PFC roughly constant in-phase Hz/Hy over the 1-60 min range appear to show a 2D rather than what should be a 3D response. Unfortunately, PFC does not include any explanation re- garding the numerical grid design, the boundary conditions, or the convergence criteria used in his finite difference nu- merical model for the high conductivity contrast (∼5000), and the large (1-60 min) period range for which the highly resistive host skin depth changes by nearly a factor of 8.

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