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On the technical side, we bypassed most of the higher-level layers of the iPhone networking stack including Bonjour and got our hands dirty with raw POSIX UDP sockets and multicasting This allowed us to engineer a network protocol for iTap that both supports autodetection and works with Windows as well as Mac OS X To get multicasting to work reliably, we had to turn to the introspection capabilities of the POSIX API to enumerate the available network interfaces and query their states This work also allowed us to build a WiFi detection algorithm more tailored to iTap s needs than the SCNetworkReachability framework is Although not strictly dealing with iPhone development per se, the Qt toolkit (wwwqtsoftwarecom) proved to be the perfect toolkit to implement our receiver application with.

This is a fourth-degree polynomial in s, and it has four roots; hence, the complete solution will consist of four constants which can be determined from the four initial conditions x1, x2, x 1, and x 2. If damping is less than critical, oscillatory motion occurs, and all four roots of Eq. (31.63) are complex with negative real parts, in the form s1,2 = n1 ip1 So the complete solution is x1 = exp ( n1t) (A1 cos p1t + A2 sin p1t) + exp ( n2t) (B1 cos p2t + B2 sin p2t) x2 = exp ( n1t) (A 1 cos p1t + A2 sin p1t) + exp ( n2t) (B cos p2 t + B 2 sin p2t) 1 Since the amplitude ratio A/B is determined by Eq. (31.62), there are only four independent constants in Eq. (31.65) which are determined by the initial conditions of the system. Forced Vibration. Quite often an auxiliary spring-mass-damper system is added to the main system to reduce the vibration of the main system. The secondary system is (31.65) s3,4 = n2 ip2 (31.64)

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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.

called a dynamic absorber. Since in such cases the force acts on the main system only, consider a force P sin t acting on the primary mass m. Referring to Fig. 31.18, we see that the equations of motion are m1 1 + (c1 + c2 )x 1 + (k1 + k2 )x1 c2 x 2 k2 x2 = P sin t x m2 2 + c2 x 2 + k2 x2 c2 x 1 k2 x 1 = 0 x Assuming a solution of the type x1 = A1 cos t + A2 sin t P/k1 (31.67) x2 = A3 cos t + A4 sin t P/k1 and substituting into Eqs. (31.66), we find that the Ai are given as A1 = 2 [2D1 2 2 D2( 2 2)] 1 2 D2 + D2 1 2 2 [D1( 2 2) + 2D2 2 2] 1 2 D 21 + D 2 2 (31.68) A3 = (2D1 2 2 D2 ) D2 + D2 1 2

DB-9 (F) 7 65 4 3 2

2 1 2 2

Although we still had to write a fair amount of platform-specific code to support the iTap receiver on both Mac OS X and Windows, using the Qt GUI toolkit saved us from having to code two completely separate applications for these two platforms Last but not least, we ve found NSNotification and friends to be an invaluable tool in the struggle to keep our code clean and modular We hope that we ve managed to pass some of the knowledge we gained while developing iTap on to you, and we hope to see a great number of new and exciting iPhone applications soon!.

(31.66)

A2 =

RS-232

3.4.1 Basic Parameters The apparently simple four-bar linkage is actually an incredibly sophisticated device which can perform wonders once proper design techniques are known and used. Figure 3.5 shows the parameters required to define the general case. Such a linkage can be used for three types of motion: 1. Crank-angle coordination. Motion of driver link b causes prescribed motion of link d. 2. Path generation. Motion of driver link b causes point C to move along a prescribed path. 3. Motion generation. Movement of driver link b causes line CD to move in a prescribed planar motion.

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