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where x = 2.043 is the dimensionless wave number for a massless s112 quark. For a nucleon n = 3, and taking R = 1.5 fm gives ( p 2 ) /2m, Y 115 MeV for the difference between the bag energy and nucleon mass, a 12% correction. For the pion the problem becomes acute: the preceding estimate would give a correction much larger than the pion mass. Of course the assumption that m >> I/ R leading to the above equations is not satisfied for this case, but the results indicate serious problems. The discussion of more sophisticated attempts to correct for CM motion is technical and we will not consider it further. Let us simply note that the ( correction term in (12.69) can be written ( p2 ) /2m o 1/R, which is the same form as the zero-point energy contribution (12.57). Therefore, one empirical approach is t o keep a term such as (12.57) in the bag energy and interpret the constant 20 as measuring both zero-point energy and center-of-mass energy (and possible self-energy contributions). &om the preceding discussion, if we take 20= 1.8 and R N 1.5 fm in (12.57), then Zo/R ~li MeV and for the 240 nucleon we estimate that about half of the phenomenological energy ZolR is actually CM energy and not zero-point energy.

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Without a doubt, the fastest way to integrate Spry data into your page is with the Spry Table object. The only preliminary step required is to set up a Spry XML data set inserting a Spry Table does the rest, and even includes enhanced functionality. With a fully functioning Spry table, you ll be able to sort columns and automatically update an associated Spry detail region under user interaction. The Spry Table object also includes robust CSS support that display different CSS styles on odd and even rows as well as when the user s mouse hovers or clicks on any row. To insert a Spry table in your page, follow these steps:

select from the Calculation Result Is pop-up menu immediately below the formula box of the Specify Calculation dialog. The calculation result data type options, shown in Figure 7.9, are Text, Number, Date, Time, Timestamp, and Container.

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Play back the transition or skim it by moving the mouse pointer over it to check that it looks the way you want it to. If necessary, change the settings for the transition, or change to another transition. If possible, stick with just one transition type to give your movie a consistent look, or use Cross Dissolve transitions and one other type of transition. Using many different

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When the Pages panel appears, you can use it to quickly move from page to page in a multipage document and to switch between displaying master pages and document pages. To display a particular document page, double-click its icon. The selected page is centered in the document window. To display a master spread, double-click its icon in the lower half of the panel.

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2.4 THE RIPPLE PROBLEM IN OMNIDIRECTIONAL PATTERNS A common application of circular arrays is to generate an omnidirectional radiation pattern in the azimuthal plane. An example of this using isotropic radiators was presented in Figure 2.7, where a ripple amplitude of about 8 dB was obtained. We will here present several additional design cases, and study how the ripple depends on the choice of design parameters.

CREATE TABLE flashStore_products ( `id` int NOT NULL AUTO_INCREMENT, `name` varchar(25), `category` int(3) NOT NULL DEFAULT 0, `description` TEXT, `thumbnail` varchar(200) NOT NULL DEFAULT , `price` varchar(10) NOT NULL, `active` int(1) NOT NULL DEFAULT 1, PRIMARY KEY (`id`) )

10.4 DOLPH CHEBYSHEV PATTERN SYNTHESIS 10.4.1 Isotropic Elements The array factor of a linear, equally spaced array antenna [Eq. (10.5)], can be identified as a polynomial by substituting w = ejkd sin [Schelkunoff 1943], thus obtaining

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