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Held while the transaction is reading the data Held until TRANSACTION COMMIT Held until TRANSACTION COMMIT n/a

E-commerce applications began in the early 1970s with such innovations as electronic transfer of funds. However, the applications were limited to large corporations and a few daring small businesses. Then came electronic data interchange (EDI), which automated routine transaction processing and extended EC to all industries. (See Appendix 5.1.) Since the commercialization of the Internet and the introduction of the Web in the early 1990s, EC applications have expanded rapidly. By 2000 there was a major shakeout in EC activities when hundreds of dot-com companies went out of business. The shakeout lasted about three years. Since 2003, EC continues its steady progress. Today, most medium and large organizations and many small ones are practicing some EC.

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the path. The session peers negotiate the rate of the BFD packets traveling over the path between them. The rate is determined by comparing the values of the triplet {Desired Min Tx Interval | Required Min Rx Interval | Detect-time Multiplexer} (the unit used for the interval configuration is milliseconds) from the configured local session and from the BFD packet received from the session peer. Each system performs value comparison on a per-session basis and determines the BFD packet sending rate and the rate of expected incoming BFD packets:

Figure 5-8

Location (Where)

An important difference between RMON 1and WON2 is that WON1 works in layer 2 in the OS1 model, while RMON2 works in layer 3. This is a substantial advantage, since hs routers can also be involved in the monitoring. In t i way, you can monitor the network through routers and the WAN connections (routers). W O N 2 also makes it possible to

The signal observed by the detector can be divided into two parts: 1. the portion of light emitted by the source which is absorbed by thc samplc, and 2. the light which is emitted by the heated sample itself (Sec. 3.3.1 and 3.5.4). If the sample temperature is higher than the detector temperature, self-emission of the sample leads to apparent transmission. In absorption measurements the source is hot compared to the sample and behaves as a black body radiator, while in emission experiments the detector 'faces' a hot sample against a cold background. Absorption and emission spectroscopy meet at the point where the sample temperature equals the source (background) tcmperaturc. I n this case, sample and background are in thermal equilibrium and thcrcfore in an equilibriim of radiation, i.e., absorption and emission of radiation by the sample are exactly equal. If the temperature of the background (source) radiator can be changed systematically, it is possible to find the point at which the lines change from absorption to emission 01vice versa (reversal of the lines). At this point, sample and background (source) must have the same temperature if the source can be treated as a black body radiator. If the temperature distribution is homogeneous throughout the sample, any of the lines may be used to determine the temperature. It is in any case advantageous t o use strong lines in order to reduce the error of the measurements. This method is thus useless if, due to a low sample concentration or lack of sample thickness, all lines show little absorbance.

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