Another Simple Example Sample Clauses

Another Simple Example. To continue teaching by example, what follows is an example of computing the loop inductance of an L shaped trace over a ground plane with the trace's return path through the plane as shown in Figure 3. Note that a line beginning with `+' is a continuation of the previous line. * A FastHenry example using a reference plane
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Another Simple Example. 5 E1 N1 N2 w=8 h=1 E2 N2 N3 w=8 h=1 * Short together the end of the L shaped trace (N3) and its corresponding * point on the ground plane directly beneath (nin) .equiv nin n3 * compute loop inductance from beginning of L (N1) to its corresponding * point directly underneath (nout) .external N1 nout * Compute impedance matrix for one very low frequency (essentially DC) * and one very high frequency .freq fmin=1e-1 fmax=1e19 ndec=0.05 * mark end of file .end In this example, the ground plane is a 1000mil 1000mil sheet of copper (by default) de xxx by three of its four corners, (0; 0; 0), (1000; 0; 0), (1000; 1000; 0). The plane is 1:2 mils thick and its discretization is speci ed by seg1 and seg2 (see Section 1.3.9). The discretization of the plane forms a grid of nodes and interconnecting segments. nin and nout refer to the internal nodes of the plane which are closest to (800; 800; 0) and (0; 200; 0), respectively. To model skin e ects on the trace, the default for the number of laments per segment is set to 8. To compute loop inductance, the node at one end of the trace is shorted to the plane by declaring the the node to be \electrically equivalent" to the node directly underneath. .equiv nin n3 and then the other end is declared as the \port" with the .external statement. In this case, a single loop impedance will be computed. If, however, the .equiv and .external were replaced with .external N1 N3 .external nout nin then the partial inductances and resistances of these two paths would be computed yielding a 2 2 impedance matrix. Computing the impedance for only two frequencies is useful for visualization of the distribution of current in the reference plane as described later in Section 4.
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