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Download - Wolfram Research

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78 2. Tutorial<br />

In[10]:= CircuitEquations[rlcfilter,<br />

Formulation −> SparseTableau] // DisplayForm<br />

Out[10]//DisplayForm=<br />

1 1 1 0 0 0 0 0 0 0 0 0 V$V0 <br />

1 1 0 1 1 0 0 0 0 0 0 0 V$RA<br />

1 1 0 1 0 1 0 0 0 0 0 0 V$C1<br />

0 0 0 0 0 0 1 1 0 0 0 0 V$L1<br />

0 0 0 0 0 0 0 1 1 1 0 0 V$C2<br />

0 0 0 0 0 0 0 0 0 1 1 1 V$RB<br />

.<br />

1 0 0 0 0 0 0 0 0 0 0 0 I$V0<br />

⩵⩵<br />

0 1 0 0 0 0 0 RA 0 0 0 0 I$RA<br />

0 0 C1 s 0 0 0 0 0 1 0 0 0 I$C1<br />

0 0 0 1 0 0 0 0 0 L1 s 0 0 I$L1<br />

<br />

0 0 0 0 C2 s 0 0 0 0 0 1 0<br />

<br />

I$C2<br />

<br />

0 0 0 0 0 1 0 0 0 0 0 RB I$RB <br />

<br />

<br />

<br />

0<br />

0<br />

0<br />

0<br />

0<br />

0<br />

V0<br />

0<br />

0<br />

0<br />

0<br />

0<br />

<br />

<br />

<br />

Sparse Tableau Analysis: The Extended Formulation<br />

Analog Insydes also supports an extended sparse tableau formulation in which the vector of<br />

unknowns comprises the branch voltages v, the branch currents i, and the node voltages v n .<br />

With I denoting an identity matrix of rank n and A T the transpose of the nodal incidence matrix A,<br />

Kirchhoff’s voltage law is expressed indirectly in terms of the node voltages as I v A T v n ⩵ 0.<br />

Therefore, the extended sparse tableau formulation does not require the calculation of a loop matrix,<br />

though at the expense of a larger matrix size than that of the basic variant:<br />

I 0 A <br />

T v 0<br />

0 A 0<br />

<br />

I<br />

<br />

⩵<br />

0<br />

<br />

Y Z 0 v n s <br />

The extended variant is selected by the option setting Formulation −> ExtendedTableau:

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