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Listing 8-23: ch08_api_cache.php (Part 4 of 6)

where the subscripts TE/TM etc. indicate the polarizations of the incident/scattered fields. The radar cross section is usually defined as a far field quantity, but can in principle also be defined in the near field. In this chapter we assume far field conditions with the definition as in Equations (11.1) and (11.2). We will analyze the co-polarized RCS the matrix component TETE as well as the cross-polarized component, TETM. When the illuminating antenna and the receiving antenna are at the same location, we have the monostatic radar cross section. If the two are separated in angle, we get the bistatic radar cross section. However, we will only consider the monostatic case here. The TE and TM field components are defined relative to the z axis, that is, the transversal (T) components are perpendicular to the z direction (cylinder axis in the cases to be studied). The scattering cross section depends also on the antenna matching. A short-circuited antenna reradiates the energy that could otherwise have been absorbed in a matched termination. This part of the cross section is termed the antenna mode contribution; the amplitude and phase depend on the antenna load. The remaining part is the residual mode contribution; together they make up the total radar cross section of the antenna. Other definitions can be found in the literature, but the ones just described are chosen here for their simplicity. See also [Hansen 1989, Munk 2003]. We will assume that the cylindrical array that we are going to analyze has the feed lines terminated in matched loads. However, in Section 11.6 we will introduce a certain mismatch as a means for controlling the total scattering.

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Most scripting done with Flash 5 actions, such as loadMovie, loadVariables, and startDrag, cannot be previewed with the Play command. Enabling Frame Actions or Buttons in the Control menu has no effect with new scripting actions. You need to use Test Movie to try out most interactive functions in a Flash movie.

You can buy the T-mount adapter at a camera shop for about $15. It is possible to find the reversal ring, but it is not as easy as it used to be. If you can t find one locally or online, you can make your own (see the Making Your Own Lens-to-Lens Reversal Adapter sidebar for instructions). The size of the reversal ring should be determined by the lens you want to use for macro photography. You can also use step-up and step-down rings to adjust the size for different lenses in your collection.

of allowed spin spin transitions between microstates that are coincidentally degenerate. For example, when a resonating nucleus (I = 1/2) is coupled with two identical neighbouring nuclei (I = 1/2) then inspection of the appropriate spin splitting diagram shows that there are actually four allowed spin spin transitions between the eight spin-coupled microstates generated, of which two transitions are degenerate, hence the appearance of three resonance frequency lines in the 1:2:1 intensity ratio characteristic of an NMR triplet (Figure 5.8). An important point to be aware of is that these rules only apply when ] (in Hz). Typically in most organic and biological macromolecules nuclei spin spin coupling takes place through one, two, three and possibly four consecutive covalent bonds. Such spin spin coupling behaviour may be called 1] (single-bond), 2] (geminal), 3] (vicinal) and 4] (long range) coupling respectively. The magnitudes of coupling constants vary substantially (Table 5.2). By de nition, spin systems are clusters of spin-coupled nuclei that are prevented from spin-coupling, or are otherwise unable to spin-couple, with neighbouring spin systems. There can be an enormous number of varieties of spin systems. For this reason, NMR spectroscopists frequently use a shorthand alphabetic nomenclature to denote the given type of spin system

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