Вот ещё немножко контекста для capacitance-only-tie-sets и inductance-only-cut-sets.
Since the presence of capacitance-only-tie-sets is solely
responsible for the non-vanishing of the matrix
![$F_{\alpha \delta}$ $F_{\alpha \delta}$](https://dxdy-02.korotkov.co.uk/f/9/5/4/954bf7474692625044bad6c16b9d4c5782.png)
, it is clear that if
one connects a small linear resistance in series with one of the capacitances
in each capacitance-only-tie-set, the matrix
![$F_{\alpha \delta}$ $F_{\alpha \delta}$](https://dxdy-02.korotkov.co.uk/f/9/5/4/954bf7474692625044bad6c16b9d4c5782.png)
becomes zero.
Again, the small resistance can be chosen small enough so as to simulate
the lead resistance.
Since the presence of inductance-only-cut-sets is solefy responsible
for the non-vanishing of the matrix
![$F_{\alpha \zeta}$ $F_{\alpha \zeta}$](https://dxdy-03.korotkov.co.uk/f/e/e/1/ee17649f5798591d90d6b4f9f11fb6fd82.png)
it is clear that if one connects
a large linear resistance in parallel with one of the inductances in each
inductance-only-cut-set, the matrix
![$F_{\alpha \zeta}$ $F_{\alpha \zeta}$](https://dxdy-03.korotkov.co.uk/f/e/e/1/ee17649f5798591d90d6b4f9f11fb6fd82.png)
becomes zero. Again, the large
resistance can be chosen large enough so as to simulate the insulator resistance.