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It s important to note that Core Audio will treat compressed formats such as MP3 as VBR data even if they are encoded at a constant bit rate Uncompressed formats like AIFF will be treated as CBR data The play method calls the callback function directly before starting playback to prime the queue with its initial set of buffers Playback begins with the call to AudioQueueStart() It continues only so long as the application s run loop is executing If you play audio on the main thread of an iPhone app, this happens automatically Background threads don t automatically have a run loop, though, so if you use a background thread, you d need to create your own run loop for playback to continue beyond the initial priming of the queue..

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.

36.5.2 Thermal Stresses Heating of the top surface of the restrained member in Fig. 36.10a causes end moments of M= and maximum bending stresses of x = ( T)E 2 (36.40) ( T)EI h (36.39)

D0 15

with compression of the top surface. If the constraints are removed, the bar will curve to a radius

Listing 3-9. Starting Audio Playback Using Audio Queue Services - (IBAction)play:(id)sender { OSStatus result; // Open the audio file from an existing NSString path NSURL *sndFileURL = [NSURL fileURLWithPath:path];

FIGURE 36.9 Examples of temperature stresses. In each case the temperature rise T is uniform throughout. (a) Straight bar with ends restrained; (b) flat plate with edges restrained.

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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.

FIGURE 36.10 Examples of thermal stresses. (a) Rectangular member with ends restrained (temperature difference between top and bottom results in end moments and bending stresses); (b) thick-walled tube has maximum stresses in tangential and longitudinal directions.

1 2 3

h ( T)

AudioFileOpenURL((CFURLRef)sndFileURL, kAudioFileReadPermission, 0, &mAudioFile); // Get the audio format UInt32 dataFormatSize = sizeof(mDataFormat); AudioFileGetProperty(mAudioFile, kAudioFilePropertyDataFormat, &dataFormatSize, &mDataFormat); // Create the playback queue AudioQueueNewOutput(&mDataFormat, AQOutputCallback, self, CFRunLoopGetCurrent(), kCFRunLoopCommonModes, 0, &mQueue); // Get buffer size, number of packets to read UInt32 maxPacketSize; UInt32 propertySize = sizeof (maxPacketSize); // Get the theoretical max packet size without scanning the entire file AudioFileGetProperty(mAudioFile, kAudioFilePropertyPacketSizeUpperBound, &propertySize, &maxPacketSize); // Get sizes for up to 0.5 seconds of audio DeriveBufferSize(mDataFormat, maxPacketSize, 0.5, &bufferByteSize, &mNumPacketsToRead); // Allocate packet descriptions array bool isFormatVBR = (mDataFormat.mBytesPerPacket == 0 || mDataFormat.mFramesPerPacket == 0); if (isFormatVBR) { mPacketDescs = (AudioStreamPacketDescription*) malloc (mNumPacketsToRead * sizeof (AudioStreamPacketDescription)); } else { mPacketDescs = NULL; } // Get magic cookie (for compressed formats like MPEG 4 AAC) UInt32 cookieSize = sizeof(UInt32); OSStatuscouldNotGetProperty = AudioFileGetPropertyInfo(mAudioFile, kAudioFilePropertyMagicCookieData, &cookieSize, NULL); if ((couldNotGetProperty == noErr)&& cookieSize) { char* magicCookie = (char *) malloc (cookieSize); AudioFileGetProperty(mAudioFile, kAudioFilePropertyMagicCookieData, &cookieSize, magicCookie); AudioQueueSetProperty(mQueue, kAudioQueueProperty_MagicCookie, magicCookie, cookieSize); free(magicCookie); } // Allocate and prime audio queue buffers mCurrentPacket = 0; for (int i = 0; i < kNumberBuffers; ++i) { AudioQueueAllocateBuffer(mQueue, bufferByteSize, &mBuffers[i]); AQOutputCallback(self, mQueue, mBuffers[i]); } // Start and run queue mIsRunning = true; AudioQueueStart(mQueue, NULL); }

The thick-walled tube of Fig. 36.10b with a hot interior surface has tangential and longitudinal stresses in the outer and inner surfaces of magnitude lo = to = 2ri2 ln(ro/ri) ( T)E 1 2 ro ri2 2(1 ) ln(ro/ri) 2ro2 ln(ro/ri) ( T)E 1 ro2 r i2 2(1 ) ln(ro/ri) (36.41)

(36.42)

76 5432

where the subscripts i and o refer to the inner and outer radii, respectively, and the subscripts t and l refer to the tangential (circumferential) and longitudinal directions. Radial stresses of lesser magnitude will also exist, although not at the inner or outer surfaces. If the tubing of Fig. 36.10b is thin, then the inner and outer stresses are equal, although opposite, and are lo = to = ( T)E 2(1 ) (36.43) ( T)E li = ti = 2(1 ) at points not too close to the tube ends.

When two elastic bodies having curved surfaces are pressed against each other, the initial point or line of contact changes into area contact, because of the deformation, and a three-dimensional state of stress is induced in both bodies. The shape of the contact area was originally deduced by Hertz, who assumed that the curvature of the

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