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The result implies that, in the time domain, i t 0:248v t , so that both voltage and current become in nite according to the function e1t . For most practical cases, must be either negative or zero. The above geometrical method does not seem to require knowledge of the analytic expression for H s as a rational function. It is clear, however, that the expression can be written, to within the constant factor k, from the known poles and zeros of H s in the pole-zero plot. See Problem 8.37.



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This chapter has focused on the forced or steady-state response, and it is in obtaining that response that the complex-frequency method is most helpful. However, the natural frequencies, which characterize the transient response, are easily obtained. They are the poles of the network function.

The Domain Name System (DNS)

EXAMPLE 8.10 The same network as in Example 8.8 is shown in Fig. 8-16. source V s is inserted at xx 0 . Obtain the natural response when a

1

Fig. 8-16 The network function is the same as in Example 8.8: H s 0:4 The natural frequencies are then 2 Np/s and 6 Np/s. is of the form s2 12 s 2 s 6 Hence, in the time domain, the natural or transient current





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where the constants A1 and A2 are determined by applying the initial conditions to the complete response, i in if , where if indicates the forced response. EXAMPLE 8.11 The network of Fig. 8-16 is driven by current I s across terminals yy 0 . H s V s =I s Z s . The three branches are in parallel so that H s Z s 1 20s 1 3 s s 2 s 6 2:5 5s 20 The network function is

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The DNS is what provides SIP networks (and all other IP networks) the ability to support mobility. In the Internet, the DNS is used to provide routing addresses for servers providing Web services in the network, as well as find the physical addresses of subscribers for the delivery of e-mail and other media. This requires converting names to numeric IP addresses. The DNS stores the URI of the subscriber and all other entities in the network with an address. This includes application servers. The URI is then translated into an IP address for routing to the final destination. This means that the registrar in the network must update the DNS when any user agent registers with a new IP address.

Again the poles are at 2 Np/s and 6 Np/s, which is the same result as that obtained in Example 8.10.

Magnitude Scaling Let a network have input impedance function Zin s , and let Km be a positive real number. Then, if each resistance R in the network is replaced by Km R, each inductance L by Km L, and each capacitance C by C=Km , the new input impedance function will be Km Zin s . We say that the network has been magnitude-scaled by a factor Km . Frequency Scaling If, instead of the above changes, we preserve each resistance R, replace each inductance L by L=Kf Kf > 0 , and replace each capacitance C by C=Kf , then the new input impedance function will be Zin s=Kf . That is, the new network has the same impedance at complex frequency Kf s as the old had at s. We say that the network has been frequency-scaled by a factor Kf .

quasi sine wave (depending on the type of magnetic sensing device) can be used to count revolutions per minute (rpm) or determine motor shaft accurately. The phase shift between channels A and B permits them to be compared by the motion controller to determine the direction of motor shaft rotation.

EXAMPLE 8.12 Express Z s for the circuit shown in Fig. 8-17 and observe the resulting magnitude scaling. Km Cs K Ls R 1=Cs Z s Km Ls m K R 1=Cs Km R m Cs Km R

1

Fig. 8-17

There are practical applications suggested by this brief exposure to magnitude scaling. For example, if the input current to a network were greater than it should be, a factor Km 10 would reduce the current to 1/10 of the former value.

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