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When we subsequently tighten other fasteners in the same joint, we further compress the joint Because this act allows previously tightened fasteners to contract a little, it reduces the tension in those fasteners even if we achieved perfect initial preload in each when we first tightened it The effect a fastener has on a previously tightened fastener is illustrated in Fig 2214 The new fastener applies a compressive load to the joint which had been previously preloaded by the first bolt Estimating Minimum Clamping Force Elastic interactions can be a special problem in large-diameter and/or gasketed joints Since our example is neither, and involves only two bolts, we will assume that these interactions cost us, worst case,.

/* Prompt the user to select the columns to be updated */ printf("*** Salesperson Update Program ***\n\n"); parmcnt = 1; for (i = 0; i < COLCNT; I++) { /* Ask about this column */ printf("Update %s column (y/n) ",columns[i].name); gets(inbuf); if (inbuf[0] == 'y') { columns[i].selected = 'y'; parmcnt += 1; } } /* Allocate a SQLDA structure to pass parameter values */

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.

Quantization creates an efficient, discrete representation for the data to be transmitted [10]. Code word assignment takes the quantized values and produces a digital bit stream for transmission. Hypothetically, the quantized values could be simply represented using uniform- or fixedlength code words. Under this approach, every quantized value would be represented with the same number of bits. As outlined previously in general terms, greater efficiency, in terms of bit rate, can be achieved with entropy coding. Entropy coding attempts to exploit the statistical properties of the signal to be encoded. A signal, whether it is a pixel value or a transform coefficient, has a certain amount of information, or entropy, based on the probability of the different possible values or events occurring. For example, an event that occurs infrequently conveys much more new information than one that occurs often. The fact that some events occur more frequently than others can be used to reduce the average bit rate. Huffman Coding. Huffman coding, which is utilized in the ATSC DTV video compression system, for example, is one of the most common entropy coding schemes [10]. In Huffman coding, a codebook is generated that can approach the minimum average description length (in bits) of events, given the probability distribution of all the events. Events that are more likely to occur are assigned shorter-length code words and those less likely to occur are assigned longer-length code words. Run Length Coding. In video compression, most of the transform coefficients frequently are quantized to zero [10]. There may be a few non-zero low-frequency coefficients and a sparse scattering of non-zero

FIGURE 18-8

11.7.3 Axial Thrust and Radial Separating Forces The formulas that follow are used to calculate the axial thrust force Wx and the radial separating force WR for bevel and hypoid gears. The direction of the pinion (driver) rotation should be viewed from the pinion back. For a pinion (driver) with a right-hand (RH) spiral with clockwise (cw) rotation or a left-hand (LH) spiral with counterclockwise (ccw) rotation, the axial and separating force components acting on the pinion are, respectively, WxP = WtP sec P (tan sin sin P cos ) WRP = WtP sec P (tan cos + sin P sin ) (11.6) (11.7)

Using EXECUTE with a SQLDA (continued)

For a pinion (driver) with an LH spiral with cw rotation or an RH spiral with ccw rotation, the force components acting on the pinion are, respectively, WxP = WtP sec P (tan sin + sin P cos ) WRP = WtP sec P (tan cos sin P sin ) (11.8) (11.9)

Part V:

For a pinion (driver) with an RH spiral with cw rotation or an LH spiral with ccw rotation, the force components acting on the gear (driven) are, respectively, WxG = WtG sec G (tan sin + sin G cos ) WRG = WtG sec G (tan cos sin G sin ) (11.10) (11.11)

high-frequency coefficients, but most of the coefficients typically have been quantized to zero To exploit this phenomenon, the two-dimensional array of transform coefficients is reformatted and prioritized into a one-dimensional sequence through either a zigzag or alternate scanning process This results in most of the important non-zero coefficients (in terms of energy and visual perception) being grouped together early in the sequence They will be followed by long runs of coefficients that are quantized to zero These zero-value coefficients can be efficiently represented through run length encoding In run length encoding, the number (run) of consecutive zero coefficients before a non-zero coefficient is encoded, followed by the non-zero coefficient value The run length and the coefficient value can be entropy-coded, either separately or jointly The scanning separates most of the zero and the non-zero coefficients into groups, thereby enhancing the efficiency of the run length encoding process.