9 X9 @& |( f+ O+ H$ ^5 o9 X; `9 n$ G( X1 l' ] T4 T
+++/// Caution. Disconnected subnetwork. During the Y-matrix elimination for phasor voltages, a near-zero diagonal element . M$ k1 Y3 [- f: M/ T9 r for node "XX0013" exists just prior to reciprocation. Statistics follow: Original ABS(Ykk) = 0.00000000E+00, v: W: z+ G: s8 M0 J
questionable value = 0.00000000E+00, tolerance ratio TOLMAT = 1.00000000E-08 . The node in question might be 7 ]+ I N J8 S: z) S$ k connected to other nodes, forming a subnetwork, but that subnetwork has no, or only very weak, paths to ground or $ R- l1 P, `5 o9 s to any other known voltage node of the steady-state network. The solution voltages for this isolated subnetwork " o+ h2 ?0 [0 U) K will now be set to zero, as the solution continues.$ z6 C" S! h4 }1 U! J! D% R4 D
+++/// Caution. Disconnected subnetwork. During the Y-matrix elimination for phasor voltages, a near-zero diagonal element, ~- _& R( f4 z' u% Z
for node "XX0003" exists just prior to reciprocation. Statistics follow: Original ABS(Ykk) = 0.00000000E+00,' `5 {4 I- I) G
questionable value = 0.00000000E+00, tolerance ratio TOLMAT = 1.00000000E-08 . The node in question might be6 t+ y ^+ T+ P$ ?
connected to other nodes, forming a subnetwork, but that subnetwork has no, or only very weak, paths to ground or2 j9 H$ j# @2 A
to any other known voltage node of the steady-state network. The solution voltages for this isolated subnetwork * L" ?) R/ h6 O/ A7 {- S( v will now be set to zero, as the solution continues. # X# i4 J8 Y" a: J$ Y6 q8 o; W8 y% C( d1 s* \, O6 d! a( y