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Tempe, AZ: N/A, 2004. [14] Preparation of Papers for IEEE Transactions and Journals, Mar. 2004. htm. inc (RC filter) to match pulse source to transmission * line (user must specify impedance (RFLT) and delay (TDFLT) ) * TDFLT should be approx.

11. Simulation Schematic. For simulation purposes, the connector has been broken into three sections or lumps. In the model specification, we are instructed to not allow the section delay to be more than risetime/10. To allow a 250ps rise time, the circuit should be divided into three as shown in (30). 9 ps Tr = 250 ps Tr ≥ Tpd ( section ) 10 ⇒ Tpd(section) ≤ 25 ps Tr ≥ 10 × Tpd ( section ) ⇒ 25 ps ≥ Tpd ( section ) Tpd ( connector ) 3 = Tpd(section) (30) 25 In a similar vein, the HSPICE suggests [12] that there will be artificial ringing if a signal were to have sharp corners around transitions.

00 E 00 1. y nc ue eq Fr Fig. 10. Magnitude of Z (Zmag) approaches (sqrt(L/C) for the connector. Our objective is to match the magnitude of Z and mitigate the discontinuities. As the frequency increases, Zmag converges on the square root L/C . This means that as the frequency increases we can substitute the square root L/C for it’s more sophisticated cousin with losses and vectors. (29). Z= R + jω L L  G + jωC C Once this substitution is in place, the Complex Conjugation solution is the exact same solution that the “Pot Hole” Method created.

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