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We rst examine the setup of the connection (Fig. 11.3-1). Trunks T1 and T2 have ISUP signaling. As in TUP signaling, an exchange decides whether to do a continuity check on the seized outgoing trunk, and informs the incoming exchange (Section 9.3.1). In this example, no checks are made. The focus is on the action at the exchanges and the interworking between Q.931 and ISUP signaling messages. We refer to the ISUP and Q.931 messages by their acronyms (Sections 11.2.3 and 10.3.2). User U1 originates the call at TE1, with a SETUP message that includes the complete called address (en-bloc address signaling). Exchange P examines the message, seizes the outgoing trunk T1 to exchange Q, and sends an IAM. It also assigns a B-channel to TE1, cuts through a unidirectional switchblock path, and sends a CALPRC message to TE1. After receiving the IAM, exchange Q seizes outgoing trunk T2 to exchange R, sends an IAM, and cuts through a bidirectional path between T1 and T2.

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the attenuator, maintaining constant nominal cascade gain (product of individual element gains) by varying the gain of the nal module to compensate For each setting we will compare the cascade gain when S12 is zero (unilateral) in the modules before and after the attenuator to the cascade gain when these modules are bilateral In the latter case, we will set S12 = 1/S21 in both modules, the upper limit of reverse gain for unconditional stability We will calculate the overall transfer function by multiplying T matrices, using MATLAB to multiply the matrices and Excel spreadsheets for the other calculations This is similar to what was done in Example 24, but this time we will include the S T matrix conversions on the spreadsheet, rather than using a separate conversion spreadsheet First, we must specify the module parameters more completely than given in Fig 219.

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We must add a phase for each of the S parameters since Fig 219 only gives the magnitude of the transfer functions and the SWRs, which do not reveal the phases of the re ections We will set all the phases to zero in these experiments, mainly in an attempt to prevent a fortuitous choice of phases from canceling the effects of the re ections This also reduces the calculation time some since we will not have to copy varying phases into MATLAB Excerpts from the spreadsheet are shown in Fig 221 The region of the spreadsheet where we enter S parameters is shown at Fig 221a Note that S12 has been set equal to the reciprocal of S21 for Modules 2 and 3 This cascade gain will be compared to the cascade gain that occurs when these two values are set equal to zero.

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