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This is the IT9 tolerance grade for the size range 18 to 30 mm. We proceed next to find the limits on the 25D9 hole. From Table 27.4, for a d shaft, we find = 0, = 16, and = 0.44. Therefore, using Eq. (19.3), we find the fundamental deviation for a d shaft to be Fundamental deviation = + D 16(23.2)0.44 =0+ 1000 1000 = 0.064 mm But this is also the upper deviation for a d shaft. Therefore, for a D hole, we have Lower deviation (hole) = upper deviation (shaft) = ( 0.064) = 0.064 mm The upper deviation for the hole is the sum of the lower deviation and the IT grade. Thus Upper deviation (hole) = 0.064 + 0.052 = 0.116 mm The two limits of the hole dimensions are therefore Upper limit = 25 + 0.116 = 25.116 mm Lower limit = 25 + 0.064 = 25.064 mm For the h shaft, we find from Table 19.4 that = = = 0. Therefore, the fundamental deviation, which is the same as the upper deviation, is zero. The lower deviation equals the upper deviation minus the tolerance grade, or Lower deviation (shaft) = 0 0.052 = 0.052 mm Therefore, the shaft limits are Upper limit = 25 + 0 = 25.000 mm Lower limit = 25 0.052 = 24.948 mm

CGRect tempbounds = CGRectZero; tempbounds.size = layerSize; tempbounds = CGRectIntegral(CGRectInset(tempbounds, tx, ty)); CGContextSetShadow(ctx, CGSizeMake(5,5), 5); #if TARGET_IPHONE_SIMULATOR sleep(2.5); //fake slow drawing on the simulator #endif CGContextDrawImage(ctx, tempbounds, imgRef); self.offscreenContext = [[(id) ctx retain] autorelease]; NSLog(@"Image loaded for %d", pageToDraw); //when we re done filling, we need to redisplay content [self performSelectorOnMainThread:@selector(setNeedsDisplay) withObject:nil waitUntilDone:NO]; }]; [q addOperation:op]; }

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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Setting RE (Not Receiver Enable) to low, the R (Receiver) pin is enabled, allowing the STAMP to receive any data coming over the A and B RS-485 network lines Setting DE (Driver Enable) to high allows the STAMP to transmit data over the RS-485 network Vcc and Vdd are electronic terms with the same meaning Setting up the RS-485 network for transmitting serial data using the BASIC STAMP would begin by setting P0 high and using Serout on P1 to transmit the data In order to receive data, you would need to set P0 to low and using Serin to receive serial data on P1 An RS-485 network operates with a controller/slave communication protocol One controller commands everything, and one or more slaves respond to the commands This example uses one BASIC STAMP as the controller and one BASIC STAMP as the slave The circuit shown in Fig.

Let us consider the general case of two cylinderlike surfaces in contact.They are represented by a cam and a follower. The radius of curvature of the follower 1 is equal to the radius of the roller Rr for the roller follower, and it goes to infinity for a flat

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.

follower. The radius of the cam s curvature 2 can be found from the following equation [compare to Eq. (4.23)]: 2 = R0 + s + s (4.36)

When the NSOperation finishes, it will call setNeedsDisplay on the view in the main thread so the view knows to draw the image data to screen. You can do this in real time. Drawing from a buffer is fast. Any time the BigViewPageView is asked to drawRect, it pulls the image data from the current cgContext for drawing; it s also filling new cgContexts in the background if you change the expected drawing size of the image through some bizarre action like zooming. Before the new buffer is ready, your image will stretch to fill and probably pixelate for a moment while the NSOperation is preparing new data.

2-16 can easily be expanded to have up to 32 BASIC STAMPs communicating on one RS-485 network by connecting additional slaves to the network A and B lines..

Equating d 2/d = s + s to zero, we can find the position of the cam, where a minimum of 2 occurs, and find its value from Eq. (4.36). Assuming perfect alignment of the contacting bodies, we have conditions described by Hertz and can check maximum compressive stress c from his well-known equation c = 0.558 where P(1/ 1 + 1/ 2) L[(1 2 )/E1 + (1 2 )/E2] 1 2 (4.37)

P = normal load between cam and follower L = actual thickness of contacting follower and cam 1, 2 = Poisson s ratios for follower and cam, respectively E1, E2 = moduli of elasticity of follower and cam, respectively

Some selected data concerning properties of materials for cams and followers are given in [4.7]. Equation (4.37) may be used for finding the minimum permissible value min of the cam s profile radius of curvature. We recall that min was necessary for calculating the values of R0 and Rr from Eqs. (4.23) and (4.26), respectively. Rearranging Eq. (4.37) gives, for a roller follower,

(4.38)

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