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The value of b for other sections is measured as shown in Fig. 36.8. In determining shear stress in a beam, the dimension b is not always measured parallel to the neutral axis. The beam sections shown in Fig. 36.8 show how to measure b in order to compute the static moment Q. It is the tendency of the shaded area to slide relative to the unshaded area which causes the shear stress. Shear flow q is defined by the equation q= VQ I (36.34)

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where q is in force units per unit length of the beam at the section under consideration. So shear flow is simply the shear force per unit length at the section defined by y = y1. When the shear flow is known, the shear stress is determined by the equation = q b (36.35)

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AudioQueueNewOutput() creates the playback queue The queue doesn t read the file directly Instead, the second argument, AQOutputCallback, is the callback function shown in Figure 3-2 It will read data from the file into buffers and add those buffers to the queue The third argument to AudioQueueNewOutput() is an argument to the callback function, which can be any data you find useful in that function In this case, I m passing self so that the callback function will be able to make Objective-C method calls on my audio playback class You need to set the buffer size used when reading data from the file Choosing a buffer size is a balancing act Buffers that are too small will mean the callback function gets more calls, which means more time spent filling buffers In an extreme case, the callback could be called so frequently that audio playback would stutter.

A thermal stress is caused by the existence of a temperature gradient in a member. A temperature stress is created in a member when it is constrained so as to prevent expansion or contraction due to temperature change.

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.

FIGURE 36.8 Correct way to measure dimension b to determine shear stress for various sections. (From Applied Mechanics of Materials, by Joseph E. Shigley. Copyright 1976 by McGraw-Hill, Inc. Used with permission of the McGraw-Hill Book Company.)

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36.5.1 Temperature Stresses These stresses are found by assuming that the member is not constrained and then computing the stresses required to cause it to assume its original dimensions. If the temperature of an unrestrained member is uniformly increased, the member expands and the normal strain is

At the other extreme, larger buffers require more memory, and memory is always at a premium on the iPhone In this case, I used a utility method, DeriveBufferSize(), to find the right buffer size for a certain amount of time, as determined by the audio format It s also reasonable to just use a fixed buffer size, if you expect to deal only with certain encodings Deriving sizes on the fly allows more flexibility, but greater flexibility is not always necessary Audio data needs to be handled slightly differently depending on whether it is encoded with a constant bit rate (CBR) or a variable bit rate (VBR) VBR packets may vary in size, so Code Audio uses packet descriptors to track the size and other information about individual packets CBR packets are all the same, so this is not necessary.

= ( T)

(36.36)

1 2 3 4

where T = temperature change and = coefficient of linear expansion. The coefficient of linear expansion increases to some extent with temperature. Some mean values for various materials are shown in Table 36.2. Figure 36.9 illustrates two examples of temperature stresses. For the bar in Fig. 36.9a, x = ( T)E y = z = x (36.37)

The stresses in the flat plate of Fig. 36.9b are x = y = ( T)E 1 z = x (36.38)

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