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Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

Interestingly, the dilaton eld introduces a type of duality into the model. In fact, this duality is related to T-duality, because it relates large and small distances. Given a set of Kasner exponents pj and a dilaton eld f, there exists a dual solution with p = p j j

NSURLConnection * theConnection = [[NSURLConnection alloc] initWithRequest:request delegate:self]; [theConnection release]; } } // We need to implement these two methods in this class if we want to be notified of the success or failure of the NSURLConnection above // -(void)connection:(NSURLConnection *)connection didReceiveResponse:(NSURLResponse *)response { } -(void)connection:(NSURLConnection *)connection didFailWithError:(NSError *)error { }

Figure 7-38 32-bit IP address: Each segment of the dotted decimal address (192, 168, 1, 1) comprises eight bits.

j =1

7

(16.9)

You may believe that a plist (or property list) is an Apple-only technology, but there is a CPAN module, Mac::PropertyList::SAX, that gives you exactly what you need:

Internet. The NET_ID is most commonly used for routing traffic between networks. On the other hand, the Host Identifier (HOST_ID) subfield identifies the address of a system (host) within a subnetwork.

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Notice that since p = p j, expanding dimensions in the theory are the contracting j dimensions in the dual theory and vice versa Pre-big-bang cosmology can be described in terms of this duality It allows for the universe to go through the following stages of evolution: It starts out in a large, at, and cold state It contracts to a self-dual point The universe enters a state where it is small, highly curved, and very hot This is the big bang It enters an expansion phase which is the universe we live in This was the rst attempt at a cosmological model using string theory However, it has since been discarded in favor of brane-based cosmological models.

< xml version="1.0" encoding="UTF-8" > <!DOCTYPE plist PUBLIC "-//Apple//DTD PLIST 1.0//EN" "http://www.apple.com/DTDs/PropertyList-1.0.dtd"> <plist version="1.0"> <dict> <key>parameters</key> <array> <dict> <key>X</key> <real>127.17512512207031</real> <key>Y</key> <real>394.22320556640625</real> </dict> <dict> <key>X</key> <real>161.1126708984375</real> <key>Y</key> <real>193.724853515625</real> </dict> <dict> <key>X</key> <real>57.804325103759766</real> <key>Y</key> <real>371.4683837890625</real> </dict> </array> </dict> </plist>

IP defines distinct address classes, which are used to discriminate between different sized networks. Classes A, B, and C are used for host addressing; the only difference between them is the length of the NET_ID subfield. A Class A address, for example, has an eight-bit NET_ID field and a 24-bit HOST_ID field. They are used for identification of very large networks and can identify as many as 16,777,214 hosts in each network. To date, only about 90 Class A addresses have been assigned. Class B addresses have 16-bit NET_ID and 16-bit HOST_ID fields. They are used to address medium-sized-networks and can identify as many as 65,534 hosts within each network. Class C addresses, which are far and away the most common, have a 24-bit NET_ID field and an eight-bit HOST_ID field. These addresses are used for smaller networks and can identify no more than 254 devices within any given network. There are 2,097,152 possible Class C NET_IDs which are commonly assigned to corporations that have fewer than 250 employees (or devices!). There are two additional address types. Class D addresses are used for IP multicasting, such as transmitting a television signal to multiple recipients, whereas Class E addresses are reserved for experimental use.

This is because several problems with the model could not be resolved, and brane models of the universe are compelling because of how the elds of the standard model and gravity are described Before going on to brane-world cosmology though, let s see how the Kasner metric can describe an accelerating universe An interesting effect that can arise when considering some spatial dimensions contracting and others expanding is that the contracting dimensions actually cause the expanding dimensions to accelerate1 Suppose that we have n > 1 contracting dimensions with three expanding spatial dimensions It can be shown that they cause the three spatial dimensions not only to expand, but to do so in an in ationary manner without a cosmological constant.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

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