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Also, at the gateway, the compressed set of binary data is formed into an IP data packet (Figure 59) Each packet is a discrete, independent unit of data, or datagram, that is presented to the network Each packet wends its way through a packet network, comprising various combinations of routers and switches and interconnecting links, until it reaches the terminating edge gateway, as identi ed by the IP address contained in the packet header (Note that, once again, a logical address is translated into a physical address In this case, the IP address is a set of bits in the rst eld of data, and the physical address is a gateway, rather than a local loop) The key advantage to a packet data network is that all of the resources (ie, circuits and switches) are highly shared.

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That is, the packets are presented to the gateway and queued up in a buffer until such time as the packet switch has computational resources available to process it In other words, the packets are queued until the packet switch can read the address information, consult a routing table, and make a decision as to the speci c route across which the packet should be forwarded Once processed, the packet might queue in a buffer until the selected circuit is available to send it on its way If there are many switches and links en route, the packet must endure this process many times At the terminating gateway, the packet is received, the data packet decompressed (reinserting the periods of silence and the redundancies) and decoded, and an approximation of the original acoustic signal is reconstructed.

1. Brinker, C. J.; Scherer, G. W. 1990. Sol-Gel Science. Academic Press, Boston, MA. 2. Fukushima, J.; Kodaira, K.; Matsushita, T. 1984. Preparation of ferroelectric PZT lms by thermal decomposition of organometallic compounds. J. Mat. Sci. 19:595 598. 3. Budd, K. D.; Dey, S. K.; Payne, D. A. 1985. Sol-gel processing of PbTiO3, PbZrO3, PZT, and PLZT thin lms. Brit. Ceram. Soc. Proc. 36:107 121. 4. Dey, S. K.; Budd, K. D.; Payne, D. A. 1988. Thin- lm ferroelectrics of PZT by sol-gel processing. IEEE Trans. UFFC. 35:80 81. 5. Schneller, T.; Waser, R. 2002. Chemical solution deposition of ferroelectric thin lms state of the art and recent trends. Ferro. 267:293 301. 6. Waser, R.; Schneller, T.; Hoffmann-Eifert, S.; Ehrhart, P. 2001. Advanced chemical deposition techniques from research to production. Int. Ferro. 36:3 20. 7. Waser, R.; Schneller, T.; Ehrhart, P.; Hoffmann-Eifert, P. 2001. Chemical deposition methods for ferroelectric thin lms. Ferro. 259(1 4):205 214. 8. Schwartz, R. W.; Schneller, T.; Waser, R. 2004. Chemical solution deposition of electronic oxide thin lms. C R Chemie 7:433 461. 9. Schwartz, R. W. 1997. Chemical solution deposition of perovskite thin lms. Chem. Mat. 9:2325 2340. 10. Tuttle, B. A.; Schwartz, R. W. 1996. Solution deposition of ferroelectric thin lms. Mat. Res. Bull. 21:49 54. 11. Lakeman, C. D. E.; Payne, D. A. 1994. Sol-gel processing of electrical and magnetic ceramics. Chem. Phys. Mat. 38:305 324. 12. Haertling, G. H. 1992. Current status of thin/thick lm ferroelectrics. Ceram. Trans. 25:1 18.

This compression process essentially reduces the bandwidth in the network required to support the voice transmission To the extent that bandwidth demands are reduced, ef ciency is increased, more data can be sent over the same circuits and through the same switches in the same period of time, and costs are lowered..

SELECT Coalesce( Address1 + str(13)+str(10) + Adress2, Address1, Address2, Address3, SalesNote) AS NewAddress FROM TempSalesContacts

2. C. A. Dahlbom and J. S. Ryan, History and Description of a New Signaling System, Bell Sys. Tech. J., 57, 1978. 3. Speci cation of Signaling System No. 6, Rec. Q.251 Q.300, ITU-T, Geneva, 1988. 4. Notes on the Network, AT&T, New York, 1980. 5. A. R. Modaressi and R. A. Skoog, Signaling System No. 7: A Tutorial, IEEE Commun. Mag., July 1990. 6. W. Stallings, ISDN, Macmillan, New York, 1989. 7. W. Peterson and D. Brown, Cyclic Codes for Error Detection, Proc. IRE, Jan. 1961.

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