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A third radiofrequency pulse now allows us to read these frequencies by inducing transverse relaxation which results in an FID which is detected and analysed This experiment results in a data matrix, s(t1 , t2 ) 2Dimensional Fourier transformation of this matrix yields a 2-D frequency spectrum S( 1 , 2 ) where corresponds to chemical shifts (ie PPM) in one-dimensional NMR A key point to understand is that the diagonal of this spectrum corresponds to the one-dimensional spectrum for the sample where 1 = 2 COSY spectroscopy allows identi cation of throughbond coupling effects in an experiment distinct from NOESY as off-diagonal peaks (sometimes referred to as cross-peaks; 1 = 2 ) Like NOEs, spin spin coupling becomes weaker with distance and correlation effects are only observed when two nuclei are linked by up to a maximum of three bonds.

Return Loss (dB)

Correlation effects are in principle possible between any pair of nuclei possessing spin but, for the.

M (g/mole)

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the Abney effect, and various color discrimination experiments. It includes correlates for brightness and saturation. A correlate for hue can also be easily calculated although hue composition has not been speci cally de ned. The model is also inadequately de ned for related stimuli since it does not include correlates for lightness and chroma. There is no way to distinguish between brightness colorfulness matching and lightness chroma matching using the ATD model. It is unclear which type of matching is predicted by the adaptation transform, but it is likely to be more similar to brightness colorfulness matching due to the way absolute units are used in the ATD model. The ATD model cannot be used (without modi cation) to predict background or surround effects or effects based on medium changes, such as discounting the illuminant. Examples of calculated values using the ATD model as described in this chapter are given in Table 14.1.

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of the image and the screen is rst established We use as an example two of the most commonly used screen sizes: 1024 1024 and 2048 2048 If the size of an input image is larger than 2048 2048, the reformatting takes two steps First, a two-dimensional bilinear interpolation is performed to shrink the image at a 5:4 ratio in both directions; this means that an image size of 2000 2510 is reformatted to 1600 2008 Second, a suitable number of blank lines are added to extend the size to 2048 2048 If a 1024 1024 image is desired, a further subsampling ratio of 2:1 from the 2048 image is performed For imaging plates that produce pixel matrix sizes smaller than 2048 2048, the image is extended to 2048 2048 by adding blank lines and then subsampling (if necessary) to obtain a 1024 1024 image.

J Jones April 12 6:01 pm to 6:12 pm 415-566-9982 operator assisted April 12 6:15 pm to 6:16 pm 415-334-8847 long distance April 12 6:23 pm to 6:38 pm 408-223-7745 April 13 9:12 am to 9:23 am 408-223-7745 April 13 10:15 am to 10:21 am 408-223-7745 operator assisted April 15 11:01 am to 11:21 am 415-964-4738 April 15 11:39 am to 12:01 pm 703-570-5770 incomplete April 15 12:10 pm to 12:40 pm 703-841-5770 wrong number April 16 12:34 pm to 12:56 pm 415-964-3130 ............................. .............................

The second method is to center the CR image on the screen without altering its size For an image size smaller than the screen, the screen is lled with blank (black) pixels and lines For an image size larger than the screen, only a portion of the image is displayed; a scroll function is used to roam the image (see 12) Similar methods can be used for DR images 10612 Background Removal The second CR preprocessing function is to remove the image background due to X-ray collimation In pediatric, extremity, and other special localized body part images, collimation can result in the inclusion of signi cant white background that should be removed in order to reduce unwanted background in the image during soft copy display This topic was extensively discussed in Section 334, with results shown in Figure 315.

SSE = ( yi y)

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